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    <title>Physics-Uspekhi. The Extracts from the Internet</title>
    <link>http://ufn.ru/en/news/</link>
    <description>The monthly rewiew of the current state of the most topical problems in physics and in associated fields.</description>
    <language>en-us</language>
    <lastBuildDate>Sun, 31 Jan 2010 21:10:05 GMT</lastBuildDate>
    <item>
      <title>Quantum model of “Zitterbewegung”</title>
      <description>С. Roos and his group at the Institute for Quantum Optics and Quantum &#13;
Information (Innsbruck, Austria) carried out an experiment  with &lt;sup&gt;40&lt;/sup&gt;Ca&lt;sup&gt;+&lt;/sup&gt; ions&#13;
in which they recorded the “quivering motion” effect (Zitterbewegung) &#13;
predicted for electrons by E. Schrodinger in 1930 using the Dirac equation. &#13;
Rapid spatial oscillations of a particle arise owing to a superposition of &#13;
states with positive and negative energies. The experiment with ions is a &#13;
quantum model of the “Zitterbewegung” of electrons; in other words, the joint &#13;
evolution of the vibrational degrees of freedom and the internal spin state of the &#13;
ion is described by the same equation as the spatial trajectory of free &#13;
electrons. Laser pulses transferred ions into a prescribed initial state and a &#13;
short time later their fluorescent radiation was observed. The properties of &#13;
this radiation yielded the characteristics of the “Zitterbewegung”. The &#13;
“Zitterbewegung” can be experimentally observed with a quantum model in which &#13;
it is linked to the spin state of the ion. At the moment it is quite unfeasible &#13;
to detect this effect with real electrons since its amplitude is only &amp;asymp;&amp;nbsp;10&lt;sup&gt;-10&lt;/sup&gt;&amp;nbsp;cm and its frequency is &amp;asymp;&amp;nbsp;10&lt;sup&gt;21&lt;/sup&gt;&amp;nbsp;Hz. The idea of quantum models &#13;
was suggested by R.&amp;nbsp;Feynman in 1982 for those cases in which the complex &#13;
behavior is beyond any hope of direct or numerical computer experiments. &#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nature08688"&gt;&lt;i&gt;Nature&lt;/i&gt; &lt;b&gt;463&lt;/b&gt; 68 (2010) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/2/#1</link>
      <guid>http://ufn.ru/en/news/2010/2/#1</guid>
      <pubDate>Sun, 31 Jan 2010 21:00:01 GMT</pubDate>
    </item>
    <item>
      <title>The E&lt;sub&gt;8&lt;/sub&gt; group in crystals</title>
      <description>R.&amp;nbsp;Coldea (Oxford University) and his colleagues in Germany and Great Britain &#13;
discovered in neutron scattering experiments that the distribution of spins in &#13;
quasi-one-dimensional ferromagnetic crystal of cobalt niobate CoNb&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;6&lt;/sub&gt; at &#13;
low temperature and in high magnetic field obeys the symmetry group E&lt;sub&gt;8&lt;/sub&gt;. In 1989 &#13;
A.B.&amp;nbsp;Zamolodchikov (The L.D. Landau Institute of Theoretical Physics) showed &#13;
that in certain cases this Lie group describes the spectrum of excitations for &#13;
the Ising model. In recent years the E&lt;sub&gt;8&lt;/sub&gt; group was also discussed in &#13;
elementary particles theory but has never been observed in real physical &#13;
systems. The phase transition in quasi-one-dimensional Ising model occurs&#13;
when the magnetic field directed along the atomic chains increases above a certain&#13;
critical value which separates the magnetically ordered and the paramagnetic phases. The&#13;
experiment studied the spin excitations in the two above phases and also investigated the&#13;
properties of crystals in the immediate vicinity of the phase transition point. The measured&#13;
ratio of the two lower resonance frequencies (two meson states) of atomic chains close to the &#13;
critical magnetic field of &amp;asymp;&amp;nbsp;5&amp;nbsp;T was found to lie close to the golden ratio 1.618, in &#13;
agreement with the prediction of A.B.&amp;nbsp;Zamolodchikov's theory. &#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1180085"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;327&lt;/b&gt; 177 (2010) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/2/#2</link>
      <guid>http://ufn.ru/en/news/2010/2/#2</guid>
      <pubDate>Sun, 31 Jan 2010 21:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Goos&amp;nbsp;&amp;ndash;&amp;nbsp;Hanchen effect for neutrons</title>
      <description>Researchers at the Delft University of Technology (The Netherlands) and the &#13;
Rutherford Appleton Laboratory (Great Britain) were able for the first time to &#13;
detect the Goos&amp;nbsp;&amp;ndash;&amp;nbsp;Hanchen effect in the reflection of spin-polarized neutrons by &#13;
a potential barrier. This effect which was already predicted by Isaac Newton for &#13;
light, produces a gap between the points of incidence and reflection of the &#13;
beam. In a manner of speech, we can say that the beam penetrates into the sample &#13;
and is reflected at a certain depth under the reflecting surface. The effect was &#13;
first measured for light by F.&amp;nbsp;Goos and H.&amp;nbsp;Hanchen in 1947. In the case of &#13;
neutrons, reflection imparts a certain phase shift to the wave function of a &#13;
particle, which may be represented by a spatial translation along the reflecting &#13;
surface. The experiment above made it possible to measure the Goos&amp;nbsp;&amp;ndash;&amp;nbsp;Hanchen &#13;
effect owing to the fact that the height of the relecting potential barrier in &#13;
magnetic field depends on neutron spin direction (and on the orienttion of the neutron &#13;
magnetic moment) so that neutrons of different degree of spin polarization are &#13;
reflected at a different efficiency. The neutron beam was reflected by a layer &#13;
of permalloy Fe&lt;sub&gt;0.2&lt;/sub&gt;Ni&lt;sub&gt;0.8&lt;/sub&gt;, 3&amp;micro;m thick. The choice of this material with &#13;
high magnetic permeability was predicated on the need to create magnetic field &#13;
under the reflecting surface and thus produce phase-shifted wave function. Reflected neutrons were&#13;
recorded by a neutron reflectometer OffSpec. A small change in the polarization of&#13;
the reflected beam was an indication of nonzero Goos&amp;nbsp;&amp;ndash;&amp;nbsp;Hanchen effect. The &#13;
Goos&amp;nbsp;&amp;ndash;&amp;nbsp;Hanchen effect may be used for practical applications, such as generation of&#13;
coherent neutron beams, and for creating neutron “waveguides”.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.104.010401"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;104&lt;/b&gt; 010401 (2010) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/2/#3</link>
      <guid>http://ufn.ru/en/news/2010/2/#3</guid>
      <pubDate>Sun, 31 Jan 2010 21:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Electron “liquid crystal” in iron-based superconductor</title>
      <description>J.C.&amp;nbsp;Davis (Brookhaven National Laboratory), Р.С.&amp;nbsp;Canfield (Ames Laboratory) and &#13;
co-workers conducted a scanning tunneling spectroscopy study of the compound &#13;
Ca(Fe&lt;sub&gt;1-x&lt;/sub&gt;Co&lt;sub&gt;x&lt;/sub&gt;)&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt; (x is the fraction of dopant atoms) and &#13;
discovered a static spatially ordered state of electron wave functions whose &#13;
structure resembles that of liquid crystals. This compound is a parent of one &#13;
class of superconductors — layered iron-based high-temperature superconductors &#13;
(see review papers in &#13;
&lt;a href="http://ufn.ru/en/articles/2008/12/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;51&lt;/b&gt; 1201, 1229, 1261 (2008)&lt;/a&gt;). Electron wave functions &#13;
of elongated shape were observed on the specimen surface, stretching along one &#13;
of the crystal axes. Their longitudianl size was approximately eight time the &#13;
distance between two neighboring iron atoms, and they were in spatial correlation with&#13;
the dopant atoms. It was conjectured that the “liquid crystal” state of electrons is&#13;
critically important for the high-temperature superconductivity to emerge. Similar&#13;
 ordered electron states have already been reported in cuprate superconductors. This &#13;
may be an indication that the superconductivity mechanism in iron-based superconductors &#13;
is closer to the currently unknown superconductivity mechanism in cuprates than to the &#13;
Bardeen&amp;nbsp;&amp;ndash;&amp;nbsp;Cooper&amp;nbsp;&amp;ndash;&amp;nbsp;Schrieffer mechanism in low-temperature superconductors. &#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1181083"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;327&lt;/b&gt; 181 (2010) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/2/#4</link>
      <guid>http://ufn.ru/en/news/2010/2/#4</guid>
      <pubDate>Sun, 31 Jan 2010 21:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Gamma-radiation background at intermediate galactic latitudes</title>
      <description>The results have been published of observing cosmic gamma radiation at &#13;
intermediate galactic latitudes 10&amp;deg;&amp;nbsp;&amp;le;&amp;nbsp;|b|&amp;nbsp;&amp;le;&amp;nbsp;20&amp;deg; in the energy &#13;
range 100&amp;nbsp;MeV to 10&amp;nbsp;GeV, obtained by the Large Area Telescope (LAT) on board the &#13;
cosmic Fermi gamma observatory during the first five months after launch. &#13;
New background measurements do not confirm some earlier observations conducted &#13;
by the EGRET gamma telescope on the orbital Compton Observatory in &#13;
1991&amp;nbsp;&amp;ndash;&amp;nbsp;2000. According to the standard model of the origin of the diffuse galactic &#13;
gamma radiation, it is generated when charged particles of cosmic rays interact &#13;
with interstellar gas and radiation. This model is calibrated using cosmic rays &#13;
data and provides sufficiently specific predictions for the gamma radiation &#13;
background. The EGRET has earlier detected an excess of gamma radiation flux in &#13;
comparison with the standard model outlined above. This information gave rise to &#13;
conjectures on additional contributions to gamma background from particles of &#13;
dark matter and other hypothetical sources. The LAT is more sensitive than the &#13;
EGRET by approximately an order of magnitude but the LAT data reveal no excess &#13;
in the gamma background and thus the measured spectrum supports with high &#13;
accuracy the predictions of the standard model of background generation.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.251101"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 251101 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/2/#5</link>
      <guid>http://ufn.ru/en/news/2010/2/#5</guid>
      <pubDate>Sun, 31 Jan 2010 21:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Parity violation in nuclear collisions</title>
      <description>The “chiral magnetic effect”, predicted in 1998 by D.&amp;nbsp;Kharzeev, R.D.&amp;nbsp;Pisarski &#13;
and M.H.G.&amp;nbsp;Tytgat was first detected at the RHIC accelerator (Relativistic Heavy &#13;
Ion Collider) in the US using the STAR detector of the Brookhaven National &#13;
Laboratory. The effect consists in parity violation (violation of the symmetry &#13;
under mirror reflection) which manifests itself in a partial spatial separation &#13;
of positively and negatively charged quarks along the direction of the orbital &#13;
angular momentum of the colliding nuclei. The separation of charges is caused by &#13;
the difference between the numbers of quarks of different chirality in the new &#13;
metastable domains and by the strong magnetic field of intensity up to &amp;asymp;&amp;nbsp;10&lt;sup&gt;15&lt;/sup&gt;&amp;nbsp;T &#13;
which arises in nonzero impact parameter collisions of nuclei. The experimenters collided &#13;
nuclei of Au&amp;nbsp;+&amp;nbsp;Au and Cu&amp;nbsp;+&amp;nbsp;Cu with center-of-mass energy &#13;
of 200&amp;nbsp;GeV. The distribution of charges on the two sides of the plane of &#13;
reaction (i.e. along the direction of the angular momentum) was measured using &#13;
correlation analysis. Possible sources of background noise and experimental &#13;
uncertainty such as the contribution of scattering of three or more particles and &#13;
of resonance decays were studied and eliminated. This resulted in identification &#13;
of statistically significant correlations which could correspond to parity &#13;
violation. As predicted by theoretical calculations, the measured effect was &#13;
found to be stronger in the case of copper nuclei than with gold nuclei.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0909.1739 "&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 251601 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/1/#1</link>
      <guid>http://ufn.ru/en/news/2010/1/#1</guid>
      <pubDate>Thu, 31 Dec 2009 21:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Measurement of ultralow temperatures</title>
      <description>D.M.&amp;nbsp;Weld and coworkers at the Massachusetts Institute of Technology developed a &#13;
sufficiently universal technique of thermometry of ultracold atoms in optical &#13;
lattices. The method of spin-gradient thermometry was tested successfully in &#13;
nonuniform magnetic field on the gas of &lt;sup&gt;87&lt;/sup&gt;Rb atoms trapped in a &#13;
three-dimensional laser beam lattice. The gas was maintained in the Mott &#13;
insulator regime in which conductivity is zero due to strong repulsion between &#13;
particles. The width of the transition zone between atom clouds in different &#13;
spin states (and having different magnetic moments) depends on temperature; &#13;
these clouds separated in the gradient of the external magnetic field. As &#13;
temperature decreases, the transition becomes sharper; incomplete separation at &#13;
finite temperatures is caused by spin excitations. Therefore, the temperature of &#13;
the gas can be found from observations of the transition zone. In this &#13;
particular experiment it was possible to measure temperatures down to 1 nK and &#13;
the researchers predict that the new technique will allow measuring temperatures &#13;
down to &amp;asymp;&amp;nbsp;50&amp;nbsp;pK. The study of atoms in optical lattices at ultralow &#13;
temperatures is important for implementing quantum spin Hamiltonians which model &#13;
materials with unique properties, such as high-temperature superconductors.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.245301"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 245301 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/1/#2</link>
      <guid>http://ufn.ru/en/news/2010/1/#2</guid>
      <pubDate>Thu, 31 Dec 2009 21:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Relativistic plasma “mirror”</title>
      <description>М.&amp;nbsp;Kando and coworkers at the Advanced Photon Research Center (Kioto, Japan)&#13;
and the P.N.&amp;nbsp;Lebedev Physical Institute of the RAS (Moskow, Russia) studied the&#13;
reflection of laser pulses from relativistically moving “mirror”. The&#13;
“mirror” was the plasma wave (modulation of electron density) generated by the&#13;
high-power laser pulse. When laser light propagates toward the “mirror”,&#13;
the double Doppler effect increases the frequency of the reflected light by a factor of 37&#13;
to 66. The frequency jump of this magnitude may prove useful in a number of&#13;
practical applications, for instance, for laser acceleration of ions or for&#13;
generation of ultrashort pulses. The reflection coefficient in this experiment&#13;
was 1.3&amp;nbsp;&amp;times;&amp;nbsp;10&lt;sup&gt;-4&lt;/sup&gt; to 0.6&amp;nbsp;&amp;times;&amp;nbsp;10&lt;sup&gt;-3&lt;/sup&gt; which is close to the quantity&#13;
predicted by the theory for this experiment. The experiment with reflection by a&#13;
relativistic plasma “mirror” was first carried out in 2007. In this new&#13;
experiment it proved possible to achieve considerably higher reflectivity and to&#13;
investigate in detail the characteristics of the reflected light.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.235003"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 235003 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/1/#3</link>
      <guid>http://ufn.ru/en/news/2010/1/#3</guid>
      <pubDate>Thu, 31 Dec 2009 21:00:03 GMT</pubDate>
    </item>
    <item>
      <title>A close pair of compact stars</title>
      <description>С. Badenes and his coworkers in the US and Israel discovered a binary system at&#13;
a distance of about 50 pc from the Earth in which one object is a white dwarf&#13;
with a mass of about 0.9M&lt;sub&gt;&amp;#9737;&lt;/sub&gt; and the second object is a neutron star or&#13;
a black hole with a mass higher than 1.6M&lt;sub&gt;&amp;#9737;&lt;/sub&gt;. This system therefore&#13;
contains the nearest to the Earth known compact remnant of supernova explosion.&#13;
The binary system SDSS&amp;nbsp;1257&amp;nbsp;+&amp;nbsp;5428 with the orbital period of 4.6 hours was&#13;
found by studying the spectral features of objects of the Sloan Digital Sky&#13;
Survey catalog and was then additionally investigated by the DIS spectrograph on&#13;
the 3.5-meter ARC telescope in New Mexico. The components of the pair gradually&#13;
move closer because of the emission of gravitational waves. Estimates of the&#13;
orbital parameters make it possible to conclude that these compact stars will&#13;
collide not later than about 500 million years. Т.A. Thompson and his colleagues&#13;
at the Ohio State University used this data to evaluate the total number and&#13;
rate of mergers of binary systems of this type. By their calculations, the&#13;
Galaxy contains about 10&lt;sup&gt;6&lt;/sup&gt; such systems and the rate of mergers in the Galaxy&#13;
is estimated as &amp;asymp;&amp;nbsp;5&amp;nbsp;&amp;times;&amp;nbsp;10&lt;sup&gt;-4&lt;/sup&gt;&amp;nbsp;yr&lt;sup&gt;-1&lt;/sup&gt;. It cannot be excluded that a collision of&#13;
a white dwarf and a compact object generate gamma bursts, powerful neutrino flashes&#13;
and also ultrahigh-energy cosmic rays. Binary systems with white dwarfs might constitute&#13;
the principal source of background gravitational wave signal in the currently planned&#13;
space interferometer LISA.&#13;
&#13;
Sources: &lt;a href="http://arxiv.org/abs/0910.2709"&gt;arXiv:0910.2709v1 [astro-ph.SR]&lt;/a&gt;, &#13;
&lt;a href="http://arxiv.org/abs/0912.0009"&gt;arXiv:0912.0009v1 [astro-ph.HE]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/1/#4</link>
      <guid>http://ufn.ru/en/news/2010/1/#4</guid>
      <pubDate>Thu, 31 Dec 2009 21:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Waves on a cell membrane</title>
      <description>The propagation of wave excitations along the outer shell of live cells depends &#13;
on many physical and chemical factors, some of them nonlinear, so that the &#13;
observation and theoretical explanation of the properties of waves on cell &#13;
membranes is an interesting and complex problem of biophysics. Surface waves are &#13;
directly linked to the ability of cells to move. Researchers at the Institute of &#13;
Biophotonics Engineering and Research Center for Applied sciences (Taipei, &#13;
Taiwan) were able to clarify how waves propagate on the surface of fibroblasts, &#13;
i.e. cells of connective tissue. The method of observation they used is known as &#13;
noninterferometric wide-field optical profilometry (NIWOP). It is based on using &#13;
the interval of linear dependence of light intensity on the amount of spatial &#13;
shifting out of focal point of the microscope. This technique made it possible &#13;
to achieve the required resolution in the three-dimensional picture of wave &#13;
propagation. The experimenters measured wave profiles and their speed (&amp;asymp;&amp;nbsp;100&amp;nbsp;nm&amp;nbsp;s&lt;sup&gt;-1&lt;/sup&gt;), their dispersion and other characteristics. Observations &#13;
confirm the detailed theory of wave propagation suggested by R.&amp;nbsp;Shlomovitz and &#13;
N.S.&amp;nbsp;Gov in 2007. Their model was based on the interaction between the force of &#13;
repulsion that arises when the protein actin polymerizes, and the compressive &#13;
force produced by the protein myosin which forms links between actin fibers. The &#13;
researchers discovered that waves disappeared when they added reagents blocking &#13;
myosin and polymerization of actin, which confirms the decisive role of these &#13;
proteins in the wave process. The outlined results may lead to important &#13;
applications in medical sciences and biotechnologies. &#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.238101"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 238101 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2010/1/#5</link>
      <guid>http://ufn.ru/en/news/2010/1/#5</guid>
      <pubDate>Thu, 31 Dec 2009 21:00:05 GMT</pubDate>
    </item>
    <item>
      <title>ЕМС effect in light nuclei</title>
      <description>In 1983 the European Muon Collaboration (ЕМС) discovered an effect which reflected how the maximum &#13;
momentum of quarks in a nucleon depends on the characteristics of the nucleus to which the nucleon &#13;
belongs. J.&amp;nbsp;Seely et al. at the Thomas Jefferson Laboratory carried out an experiment which revealed &#13;
new features of the ЕМС effect. A conclusion was made in a number of theoretical papers attempting &#13;
to interpret the ЕМС effect that it is linked to the mean density or mass of the nucleus. The new &#13;
experiment demonstrated, however, that these parameters give an ambiguous description of the effect &#13;
and may be of only secondary importance. This experiment studied the scattering of 5.8&amp;nbsp;GeV electrons &#13;
by targets of &lt;sup&gt;2&lt;/sup&gt;H, &lt;sup&gt;3&lt;/sup&gt;Не, &lt;sup&gt;4&lt;/sup&gt;Не, &lt;sup&gt;9&lt;/sup&gt;Ве and &lt;sup&gt;12&lt;/sup&gt;С nuclei. It was found that the magnitude of &#13;
the ЕМС effect of the nucleus &lt;sup&gt;9&lt;/sup&gt;Ве is close to that of &lt;sup&gt;12&lt;/sup&gt;С even though the mean density of &#13;
the nucleus &lt;sup&gt;9&lt;/sup&gt;Ве is considerably lower. The conclusion is that the mean nuclear density is not a &#13;
decisive factor for the ЕМС effect. It was also established that the light nuclei &lt;sup&gt;3&lt;/sup&gt;Не and &lt;sup&gt;4&lt;/sup&gt;Не &#13;
differ greatly in the magnitude of the ЕМС effect. The key to the explanation of the obtained &#13;
results may lie in the cluster structure of nuclei. E.&amp;nbsp;g. the nucleus of beryllium may be regarded as &#13;
two bound nuclei of &lt;sup&gt;4&lt;/sup&gt;Не plus an additional neutron revolving around them, the average density of &#13;
the &lt;sup&gt;9&lt;/sup&gt;Ве nucleus being considerably lower than the density of each of the &lt;sup&gt;4&lt;/sup&gt;Не nuclei. In view &#13;
of this, the ЕМС effect in such nuclei may be a function of not average but local density so that &#13;
the ЕМС effect of the nucleus &lt;sup&gt;9&lt;/sup&gt;Ве is analogous to the effect of individual nuclei &lt;sup&gt;4&lt;/sup&gt;Не. In &#13;
other words, the properties of nucleons in nuclei are determined not by the mass or mean density of &#13;
the nucleus as a whole but by the local environment of the nucleon, such as the characteristics of &#13;
the clusters contained in this nucleon. &#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0904.4448"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 202301 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/12/#1</link>
      <guid>http://ufn.ru/en/news/2009/12/#1</guid>
      <pubDate>Mon, 30 Nov 2009 21:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Emission cone of Vavilov&amp;nbsp;&amp;ndash;&amp;nbsp;Cherenkov radiation in “left-handed” matter</title>
      <description>Researchers at the Zhejiang University, Hangzhou (China) and Massachusetts Institute of &#13;
Technology (USA) observed for the first time the reversed Vavilov&amp;nbsp;&amp;ndash;&amp;nbsp;Cherenkov radiation &#13;
generated in a “left-handed” medium (a medium whose dielectric permittivity and magnetic &#13;
permeability are simultaneously negative). As V.G.&amp;nbsp;Veselago predicted in 1967 &#13;
(see &lt;a href="http://ufn.ru/en/articles/1968/4/a/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;10&lt;/b&gt; 509 (1968)&lt;/a&gt;), the cone of emission of the Cherenkov radiation and the energy flow in &#13;
“left-handed” materials are directed backward relative to the motion of the particle. &#13;
The experiment described here used microwave radiation propagating through a metamaterial, &#13;
that is, an array of conductors. A charged particle was imitated by a sequence of dipoles &#13;
with the phase changing in a certain manner; the dipoles were excited in a waveguide &#13;
consisting of 14 gaps. The speed at which this “particle” was moving was &lt;i&gt;v&amp;nbsp;=&amp;nbsp;1,9c/n&lt;/i&gt; &#13;
where &lt;i&gt;n&lt;/i&gt; is the refractive index of the metamaterial. This set of dipoles is completely &#13;
equivalent from the standpoint of emission of radio waves to a real charged particle; &#13;
however, the imitation made it possible to achieve considerably higher (and measurable) &#13;
intensity of the Vavilov&amp;nbsp;&amp;ndash;&amp;nbsp;Cherenkov radiation in the frequency range &#13;
8.1-9.5&amp;nbsp;GHz. The &#13;
Vavilov&amp;nbsp;&amp;ndash;&amp;nbsp;Cherenkov radiation could not propagate in metamaterials studied earlier (owing to the nature of their anisotropy) so for observing the Vavilov&amp;nbsp;&amp;ndash;&amp;nbsp;Cherenkov radiation a metamaterial with a special configuration of unit cells was fabricated. The reversed &#13;
Vavilov&amp;nbsp;&amp;ndash;&amp;nbsp;Cherenkov radiation may prove useful in fast particle detectors, e.g. in &#13;
accelerator experiments. For details on media with negative refractive index see papers by &#13;
V.G.&amp;nbsp;Veselago in &lt;a href="http://ufn.ru/en/articles/2003/7/k/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;46&lt;/b&gt; 764 (2003)&lt;/a&gt;, &lt;a href="http://ufn.ru/en/articles/2009/6/i/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;52&lt;/b&gt; 649 (2009) &lt;/a&gt;. &#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.194801"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 194801 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/12/#2</link>
      <guid>http://ufn.ru/en/news/2009/12/#2</guid>
      <pubDate>Mon, 30 Nov 2009 21:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein condensate of strontium atoms</title>
      <description>Two independent groups of researchers from the Rice University in US and the Institute for &#13;
Quantum Optics and Quantum Information (IQOQI) in Austria prepared the Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein condensate of atoms of strontium isotope &lt;sup&gt;84&lt;/sup&gt;Sr whose natural abundance is only 0,56%. Even though the abundances of the isotopes &lt;sup&gt;86&lt;/sup&gt;Sr and  &lt;sup&gt;88&lt;/sup&gt;Sr are much higher, they cannot be cooled evaporatively owing to the excessively large (in the case of &lt;sup&gt;86&lt;/sup&gt;Sr) or too small (&lt;sup&gt;88&lt;/sup&gt;Sr) atomic scattering length. Contrary to these two, the rare isotope &lt;sup&gt;84&lt;/sup&gt;Sr has the &#13;
scattering length of 123&amp;nbsp;Bohr radii which suits cooling ideally; in the experiments of both groups, &#13;
evaporative cooling was the concluding stage after laser cooling in magnetooptic trap. The &#13;
transition to condensate state was identified by monitoring the optical profile of the cloud of gas &#13;
and from the value of the chemical potential calculated from the dynamics of expansion of the cloud. &#13;
It is suggested that the condensate of &lt;sup&gt;84&lt;/sup&gt;Sr atoms be used in ultraprecise experiments, in new &#13;
systems for quantum computation and as a buffer gas in cooling other isotopes, e.&amp;nbsp;g. the fermion &#13;
isotope &lt;sup&gt;87&lt;/sup&gt;Sr, to degenerate state. &#13;
&#13;
Sources: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.200402"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 200402 (2009) &lt;/a&gt;; &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.200401&#13;
"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 200401 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/12/#3</link>
      <guid>http://ufn.ru/en/news/2009/12/#3</guid>
      <pubDate>Mon, 30 Nov 2009 21:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Laser acceleration of neutral atoms</title>
      <description>U.&amp;nbsp;Eichmann and his colleagues at the Institute for Optics and Atomic Physics (Berlin) and &#13;
the Max Planck Institute discovered the effect of acceleration of neutral atoms by &#13;
pondermotive force in the field of nonuniform laser radiation. Typically, one considers &#13;
the effect of the pondermotive force on charged particles but in fact a similar force may &#13;
arise in the case of neutral atoms in view of the dynamical polarization of atoms after &#13;
they were excited to Rydberg states. The electron on a distant orbit may then be &#13;
accelerated as a free particle by the pondermotive force (the acceleration of the nucleus &#13;
is much weaker because of its large mass). If the electron after acceleration remains &#13;
bonded to the atomic nucleus, the momentum of the accelerated electron is transferred to &#13;
the atom as a whole. In the experiment of the German scientists a beam of neutral helium &#13;
atoms was illuminated by short focused pulses of laser light, and roughly one per cent of &#13;
atoms felt acceleration. In some cases the acceleration of an atom was greater than the &#13;
acceleration of free fall &lt;i&gt;g&lt;/i&gt; by a factor of 10&lt;sup&gt;14&lt;/sup&gt; — record-high for accelerations of &#13;
neutral atoms in external fields ever observed. &#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nature08481"&gt;&lt;i&gt;Nature&lt;/i&gt; &lt;b&gt;461&lt;/b&gt; 1261 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/12/#4</link>
      <guid>http://ufn.ru/en/news/2009/12/#4</guid>
      <pubDate>Mon, 30 Nov 2009 21:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Polarization of microwave background and cosmological parameters</title>
      <description>The observation of polarization of cosmic microwave background is one of the most efficient methods &#13;
of studying physical processes in the early Universe and of improving the cosmological parameters. &#13;
Measurements of polarization of microwave background became technically possible in 2002 and have &#13;
been conducted since then with gradually better precision by a number of instruments. From 2005 to &#13;
2007 observations were conducted at the South Pole with a 2.6&amp;nbsp;m QUaD radio telescope equipped with &#13;
31 pairs of orthogonal bolometers sensitive to the polarization of electromagnetic waves and &#13;
functioning at two frequencies: 100 and 150&amp;nbsp;GHz. By now the data gathered during this period has &#13;
been processed and more accurate values of cosmological parameters were computed. The accuracy of &#13;
results is the highest if datasets of several detectors are used simultaneously (WMAP, ACBAR, &#13;
QUaD etc.). For example, according to the latest data, the most probable value of the Hubble &#13;
constant is H&lt;sub&gt;0&lt;/sub&gt;&amp;nbsp;=&amp;nbsp;70.6&amp;nbsp;km&amp;nbsp;s&lt;sup&gt;-1&lt;/sup&gt;Mpc&lt;sup&gt;-1&lt;/sup&gt;, the index of the density perturbation spectrum &#13;
&lt;i&gt;n&lt;sub&gt;s&lt;/sub&gt;&amp;nbsp;=&amp;nbsp;0.960&lt;/i&gt;, and a scenario is possible in which the index depends on scale (on the running index). It was also possible to improve the constraint on the tensor mode of perturbations &#13;
(gravitational waves) in comparison with scalar perturbations (density perturbations); now the ratio &#13;
of these components is estimated as &lt;i&gt;r&amp;lt;0,33&lt;/i&gt; at the confidence level 95%. &#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0906.1003"&gt;&lt;i&gt;Astrophysical Journal&lt;/i&gt; &lt;b&gt;705&lt;/b&gt; 978 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/12/#5</link>
      <guid>http://ufn.ru/en/news/2009/12/#5</guid>
      <pubDate>Mon, 30 Nov 2009 21:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Testing of Bell's inequalities in a system of Josephson qubits</title>
      <description>Researchers at the University of California at Santa Barbara experimentally confirmed that &#13;
Bell's inequalities are violated in a macroscopic system composed of two Josephson qubits &#13;
(quantum bits) implemented using superconducting Josephson contacts. Violation of Bell's &#13;
inequalities has already been tested in a number of quantum processes which excluded the &#13;
possibility of the     “hidden-variables” interpretation. In the new experiment two &#13;
Josephson qubits were transferred to entangled quantum state (&lt;a href="http://ufn.ru/en/news/2006/10/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;49&lt;/b&gt; 1111 (2006)&lt;/a&gt;) using an electromagnetic &#13;
resonator after which quantum correlations between the states of qubits were &#13;
measured. For this particular experiment, Bell's inequality can be written in the form &lt;i&gt;S&amp;lt;2&lt;/i&gt; &#13;
where &lt;i&gt;S&lt;/i&gt; depends on the state of qubits. Measurements showed that &lt;i&gt;S&amp;nbsp;=&amp;nbsp;2.0732&amp;nbsp;&amp;plusmn;&amp;nbsp;0.0003&lt;/i&gt; i.e. Bell's inequality is violated at the level of 244 standard deviations and therefore the state of the qubits in this experiment cannot be classically described.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nature08363"&gt;&lt;i&gt;Nature&lt;/i&gt; &lt;b&gt;461&lt;/b&gt; 504 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/11/#1</link>
      <guid>http://ufn.ru/en/news/2009/11/#1</guid>
      <pubDate>Sat, 31 Oct 2009 21:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Persistent current in a ring</title>
      <description>J.&amp;nbsp;Harris (Yale University, USA) and his co-workers measured for the first time the persistent electric current in metallic (non-superconducting) rings. The &#13;
persistent ring current predicted theoretically by М.&amp;nbsp;Buttiker, Y.&amp;nbsp;Imry and R.B.&amp;nbsp;Landauer &#13;
in 1983 is an element of the equilibrium quantum state of electrons in the ring. It was &#13;
predicted that the persistent current in micron-size rings at temperatures &lt;i&gt;T&amp;lt;1&lt;/i&gt;&amp;nbsp;К may &#13;
reach 1&amp;nbsp;nА. The external magnetic field breaks the time reversal symmetry which forces one &#13;
of the possible current directions to be selected, plus this current is a periodic &#13;
function &lt;i&gt;I(&amp;Phi;)&lt;/i&gt; of the magnetic flux &amp;Phi; across the ring (due to the Aharonov&amp;nbsp;&amp;ndash;&amp;nbsp;Bohm &#13;
effect). Attempts were made earlier to use superconducting quantum interferometers &#13;
(SQUIDs) to measure the magnetic field generated by the persistent current but the &#13;
sensitivity of this method proved insufficient owing to, among other factors, the feedback &#13;
to the ring current from oscillations of the superconducting current in SQUIDs. J.&amp;nbsp;Harris &#13;
and his team measured the effect induced by the magnetic field of the current in the &#13;
micromechanical silicon cantilever probe. Aluminum rings were attached to the end of the &#13;
probe and the system measured the shift of the resonance frequency of mechanical &#13;
vibrations of the cantilever due to the interaction between the magnetic moments of ring &#13;
currents and the external magnetic field. The oscillations of the cantilever were caused &#13;
by a piezo-mechanical vibrator and were observed using a laser interferometer. This &#13;
technique has the sensitivity  (&amp;asymp;20&amp;nbsp;pА&amp;nbsp;Hz&lt;sup&gt;-1/2&lt;/sup&gt;) approximately an order of magnitude better than the approach based on SQUIDs. The results of measurements both with &#13;
a single aluminum ring and with a large set of rings are in good agreement with theoretical &#13;
predictions. It was found that current oscillations &lt;i&gt;I(&amp;Phi;)&lt;/i&gt; in different rings of the &#13;
set had uncorrelated phases both in the first and the second harmonics. Measuring &#13;
persistent currents in microscopic rings can help in studying quantum phase transitions &#13;
and quantum coherence at low temperatures.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1178139"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;326&lt;/b&gt; 272 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/11/#2</link>
      <guid>http://ufn.ru/en/news/2009/11/#2</guid>
      <pubDate>Sat, 31 Oct 2009 21:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Splitting of Cooper pairs</title>
      <description>Two independent groups of researchers created efficient sources of electrons entangled in &#13;
spin states (EPR-pairs); they act by splitting Cooper pairs of electrons tunneling through &#13;
a superconductor. The difficulty that faced earlier attempts to generate EPR pairs stemmed &#13;
from the fact that electrons in metals sit below the  Fermi surface so that releasing them &#13;
immediately destroys entanglement. The ground state in superconductors is the condensate of &#13;
Cooper pairs in spin-singlet state so these pairs can be separated from the superconductor &#13;
by way of tunneling. L.&amp;nbsp;Hofstetter and his colleagues in Switzerland, Hungary and Denmark &#13;
solved the remaining problem of splitting Cooper pairs into individual electrons by using &#13;
the Coulomb repulsion of the electrons that went through tunneling into two quantum dots. &#13;
Quantum dots would appear in the region where the nanowire made of indium arsenide &#13;
intersected with the central superconductor and two metal contacts in normal &#13;
(non-superconducting) state. Control electrodes make it possible to vary the depth of the &#13;
potential well of quantum dots in such a way that only one electron passed through each &#13;
quantum dot at any one moment of time. The electrons of a Cooper pair are inherently &#13;
quantum-correlated (entangled) along the direction of spin and this entanglement of &#13;
electrons survived after the pair was split. The experiment of L.G.&amp;nbsp;Herrmann and &#13;
colleagues in France, Spain and Germany generally resembles the one described above but it &#13;
used carbon nanotubes instead of nanowire. New sources of EPR pairs of electrons may find &#13;
important applications in fundamental research, such as the study of the &#13;
Einstein&amp;nbsp;&amp;ndash;&amp;nbsp;Podolsky&amp;nbsp;&amp;ndash;&amp;nbsp;Rosen paradox. &#13;
&#13;
Sources: &lt;a href="http://dx.doi.org/10.1038/nature08432"&gt;&lt;i&gt;Nature&lt;/i&gt; &lt;b&gt;461&lt;/b&gt; 960 (2009) &lt;/a&gt;; &lt;a href="http://arxiv.org/abs/0909.3243v1"&gt;arXiv:0909.3243v1 [cond-mat.mes-hall]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/11/#3</link>
      <guid>http://ufn.ru/en/news/2009/11/#3</guid>
      <pubDate>Sat, 31 Oct 2009 21:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein condensate of calcium atoms</title>
      <description>S.&amp;nbsp;Kraft (Federal Physico-Technical Institute, Germany) and his co-workers were able to &#13;
produce for the first time the Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein condensate of atoms of the alkali earth &#13;
metal, &lt;sup&gt;40&lt;/sup&gt;Ca. At the initial stage of the experiment atoms were laser-cooled in a &#13;
magneto-optical trap using the transitions &lt;sup&gt;1&lt;/sup&gt;S&lt;sub&gt;0&lt;/sub&gt;-&lt;sup&gt;1&lt;/sup&gt;P&lt;sub&gt;1&lt;/sub&gt;, &lt;sup&gt;1&lt;/sup&gt;S&lt;sub&gt;0&lt;/sub&gt;-&lt;sup&gt;3&lt;/sup&gt;P&lt;sub&gt;1&lt;/sub&gt; etc. &#13;
The main process that restricted the effectiveness of cooling was losses via &#13;
three-particle atomic interactions. At the last stage the atomic cloud was loaded into an &#13;
optical dipole trap and cooled evaporatively. The transition of about 2&amp;times;10&lt;sup&gt;4&lt;/sup&gt; &#13;
atoms to the Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein condensate state at 170&amp;nbsp;nK was identified using the characteristic Gaussian density profile. The formation of the condensate was also &#13;
confirmed by the large chemical potential of the gas, which was calculated on the basis of &#13;
the measured velocities of anisotropic expansion of the cloud. Quantum intercombination &#13;
transitions with very narrow spectral lines &lt;sup&gt;1&lt;/sup&gt;S&lt;sub&gt;0&lt;/sub&gt;-&lt;sup&gt;3&lt;/sup&gt;P&lt;sub&gt;1&lt;/sub&gt; (only 370&amp;nbsp;Hz) are possible &#13;
in atoms of &lt;sup&gt;40&lt;/sup&gt;Ca. Consequently, Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein condensates of &lt;sup&gt;40&lt;/sup&gt;Ca atoms are &#13;
very promising for highest-precision measurements of the gravitational field. Furthermore, &#13;
&lt;sup&gt;40&lt;/sup&gt;Ca atoms in the non-degenerate ground state have no magnetic moment, which &#13;
additionally increases the accuracy of measurements in view of the absence of interaction &#13;
with external magnetic fields.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.130401"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 130401 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/11/#4</link>
      <guid>http://ufn.ru/en/news/2009/11/#4</guid>
      <pubDate>Sat, 31 Oct 2009 21:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Magnetism of carbon</title>
      <description>Researchers in Czechia and the Netherlands J.&amp;nbsp;Cervenka, M.I.&amp;nbsp;Katsnelson and &#13;
C.F.J.&amp;nbsp;Flipse have clarified the mechanism of formation of ferromagnetic properties of specimens &#13;
of polycrystalline graphite at room temperatures. A number of experiments established that &#13;
various forms of carbon manifest ferromagnetism (see e.g. &lt;a href="http://ufn.ru/en/news/2004/1/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;47&lt;/b&gt; 102 (2004)&lt;/a&gt;) but its &#13;
nature remained unclear. Hypotheses were advanced that carbon owes the observed magnetism &#13;
either to metal impurities or to defects of crystal structure. The new experiment used a &#13;
magnetic force microscope, a SQUID magnetometer and an atomic force microscope for &#13;
measurements; this made it possible to study simultaneously and at high spatial resolution &#13;
both magnetic and electronic properties of samples. The obtained microscopic images provide &#13;
direct evidence supporting the second hypothesis: the graphite magnetism arises owing to defects &#13;
in the structure of atomic layers and that impurities do not play a significant role. A &#13;
two-dimensional network of defects (only 2&amp;nbsp;nm thick each) is formed along atomic &#13;
planes of carbon in graphite; these networks delimit homogeneous regions, i.e. grains of the &#13;
polycrystal. Ferromagnetism originates with unpaired electrons localized on defects at &#13;
grain boundaries. Magnetic carbon may find applications in spintronic devices and in medical &#13;
fields for designing biological sensors.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nphys1399"&gt;&lt;i&gt;Nature Physics&lt;/i&gt; &lt;b&gt;5&lt;/b&gt; 840 (2009) &lt;/a&gt;; &lt;a href="http://arxiv.org/abs/0910.2130"&gt;arXiv:0910.2130v1 [cond-mat.mtrl-sci]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/11/#5</link>
      <guid>http://ufn.ru/en/news/2009/11/#5</guid>
      <pubDate>Sat, 31 Oct 2009 21:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Testing the isotropy of the the speed of light</title>
      <description>Ch. Eisele, A. Yu. Nevsky and S. Schiller (Institut fur Experimentalphysik, &#13;
Heinrich-Heine-University at Dusseldorf, Germany) conducted a test of independence of the &#13;
speed of light of the direction of propagation, with record accuracy so far. The setting &#13;
of the experiment resembles that of the  classical Michelson&amp;nbsp;&amp;ndash;&amp;nbsp;Morley experiment. The setup &#13;
includes two mutually perpendicular optical waveguides with slightly different resonance &#13;
frequencies in which standing electromagnetic waves are excited by a laser. The difference &#13;
between frequencies in the two waveguides is measured by observing beats of the sum signal &#13;
as a function of spatial orientation of the apparatus. In the 13 months that the &#13;
experiment was run the apparatus was turned by 90 degrees approximately 175,000 times. &#13;
Considerable effort was made to exclude external factors of different types that produce &#13;
systematic errors. No anisotropy of the speed of light was detected at accuracy of &#13;
&amp;asymp;&amp;nbsp;10&lt;sup&gt;-17&lt;/sup&gt; which confirms the local Lorentz invariance at this level. The &#13;
measurements conducted are important for testing the suggested approaches to constructing &#13;
the Unified field theory: indeed, the Lorentz invariance holds only approximately in some &#13;
models.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.090401"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 090401 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/10/#1</link>
      <guid>http://ufn.ru/en/news/2009/10/#1</guid>
      <pubDate>Wed, 30 Sep 2009 20:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Ferromagnetism in Fermi gas</title>
      <description>W. Ketterle (Massachusetts Institute of Technology) and his colleagues succeeded for the &#13;
first time in detecting ferromagnetic properties of ultracold gas consisting of &lt;sup&gt;6&lt;/sup&gt;Li &#13;
atoms. Ferromagnetism was previously observed in gases only in the state of Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein &#13;
condensate. The possibility of transition of Fermi gases to ferromagnetic state when the &#13;
interparticle interaction is repulsive has been discussed in a number of theoretical &#13;
papers but no definitive conclusions have been made on the feasibility of such &#13;
transitions. In the new experiment, a cloud of ultracold gas which is a mixture of atoms &#13;
with oppositely oriented spins was held in an optical trap. The transition to &#13;
ferromagnetic state at a temperature of less than 1&amp;nbsp;&amp;micro;K was identified by an indirect &#13;
method of detecting a drop in the rate of inelastic three-particle collisions that result &#13;
in the formation of molecules, by detecting the point when the minimal kinetic energy of &#13;
particles is reached, and by recognizing certain characteristics of expansion of the gas &#13;
cloud. These properties were exactly those predicted for the ferromagnetic gas. The gas &#13;
field contained about 100 magnetic domains of volumes of about 5&amp;nbsp;&amp;micro;m&lt;sup&gt;3&lt;/sup&gt; with about 50 atoms of the gas in each. This experiment demonstrated that ferromagnetism may arise in &#13;
a system of Fermi particles possessing no crystal lattice.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1177112"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;325&lt;/b&gt; 1521 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/10/#2</link>
      <guid>http://ufn.ru/en/news/2009/10/#2</guid>
      <pubDate>Wed, 30 Sep 2009 20:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Buffer-gas cooling</title>
      <description>S.C.&amp;nbsp;Doret (Massachusetts Institute of Technology) and his colleagues developed a new method of &#13;
cooling a gas to  the state of Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein condensate — the gas was cooled via collisions of &#13;
its atoms with atoms of auxiliary buffer gas. The Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein condensate is typically produced by &#13;
a preliminary laser cooling but this method works with only a few gases. In the experiment of &#13;
S.C.&amp;nbsp;Doret and his colleagues, &lt;sup&gt;4&lt;/sup&gt;He atoms were evaporated by light pulses from the inner walls of &#13;
the vessel and a small fraction of them (&amp;asymp;&amp;nbsp;10&lt;sup&gt;-5&lt;/sup&gt;) were raised by microwave pulses to &#13;
an excited state &lt;sup&gt;4&lt;/sup&gt;He&lt;sup&gt;*&lt;/sup&gt;. Atoms of &lt;sup&gt;4&lt;/sup&gt;He in the ground state acted as buffer gas; collisions &#13;
with them cooled &lt;sup&gt;4&lt;/sup&gt;He&lt;sup&gt;*&lt;/sup&gt; atoms to a temperature of &amp;asymp;&amp;nbsp;500&amp;nbsp;&amp;micro;K. Then in a short time &lt;sup&gt;4&lt;/sup&gt;He &#13;
atoms were again absorbed by vessel walls so what was left in the vessel was a cooled gas of &lt;sup&gt;4&lt;/sup&gt;He&lt;sup&gt;*&lt;/sup&gt; &#13;
atoms. Further cooling for the transition to the Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein condensate used the conventional &#13;
evaporation technique. The buffer-gas method can cool many atomic and molecular gases for which &#13;
other methods of cooling are inapplicable.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.103005"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 103005 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/10/#3</link>
      <guid>http://ufn.ru/en/news/2009/10/#3</guid>
      <pubDate>Wed, 30 Sep 2009 20:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Improved atomic force microscope</title>
      <description>Researchers at the IBM research laboratory in Zurich (Switzerland) and the Institute for &#13;
Nanomaterials Science (Utrecht, the Netherlands) improved the resolution of the atomic &#13;
force microscope (AFM) to a level at which individual atoms composing a molecule can be &#13;
observed. This became feasible by using a single molecule of carbon monoxide CO as the tip &#13;
of the needle of the AFM. The factor that limited the resolution of AFM with a metal tip &#13;
was the distortion of the structure of the specimen by van der Waals forces when the tip &#13;
approached the specimen surface, or atoms jumped to the tip off the specimen surface, &#13;
adsorbed on the needle, and also destroyed the observed features. The advantages of a CO &#13;
tip used as the needle tip lie in the considerable stability of this molecule against &#13;
outside influences and van der Waals forces. As an illustration, L.&amp;nbsp;Gross and his &#13;
colleagues carried out observations of a carefully scrutinized molecule C&lt;sub&gt;22&lt;/sub&gt;H&lt;sub&gt;14&lt;/sub&gt;. &#13;
The improved microscope made it possible to resolve all five carbon rings as well as all &#13;
constituent carbon and hydrogen atoms in the molecule. It was possible to measure &#13;
interatomic distances of only 0.14&amp;nbsp;nm, which is a record resolution of an atomic force &#13;
microscope.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1176210"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;325&lt;/b&gt; 1110 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/10/#4</link>
      <guid>http://ufn.ru/en/news/2009/10/#4</guid>
      <pubDate>Wed, 30 Sep 2009 20:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Search for gravitational waves</title>
      <description>It is assumed that cosmic gamma bursts of short duration (less than two seconds) occur &#13;
because of a merger of two neutron stars, or a neutron star and a black hole in a binary &#13;
system, while long-duration gamma bursts with a softer spectrum are generated in supernova &#13;
explosions. In both cases gamma radiation must be accompanied with a powerful burst of &#13;
gravitational waves. The data collected by the detectors LIGO (in the USA) and VIRGO (in &#13;
Italy) were compared with the catalog of 137 gamma bursts most of which were observed by &#13;
the Swift satellite. The study found no statistically significant correlation of signals &#13;
which puts a bound on the total energy of gravitational radiation, or (if energy is given) &#13;
on the distance to the sources of bursts. Typical gamma bursts occur in other galaxies, at &#13;
cosmologically large distances. A gamma burst can be recorded by LIGO or VIRGO only if the &#13;
burst source happens to be relatively near. Preliminary evaluations showed that such &#13;
events cannot be dismissed as impossible but that their probability is very low. An &#13;
earlier search by the LIGO detector of a gravitational signal from a relatively near and &#13;
extremely bright gamma burst GRB&amp;nbsp;030329 also failed to find a signal. According to &#13;
calculations, gravitational waves from gamma bursts should be confidently recorded by future&#13;
improved detectors with sensitivity raised by approximately an order of magnitude compared &#13;
to today's LIGO and VIRGO.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0908.3824"&gt;	arXiv:0908.3824v1 [astro-ph.HE]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/10/#5</link>
      <guid>http://ufn.ru/en/news/2009/10/#5</guid>
      <pubDate>Wed, 30 Sep 2009 20:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Parity violation in ytterbium atoms</title>
      <description>Parity violation (the invariance of the properties of systems under mirror reflections) &#13;
was first detected in 1957 in the asymmetry of the ejection of electrons from decaying &#13;
cobalt-60 atoms in magnetic field. The record amplitude of this effect was observed in &#13;
cesium atoms. D.&amp;nbsp;Budker and coworkers at the Berkeley National Laboratory (USA)  measured &#13;
the degree of parity violation in atoms of &lt;sup&gt;174&lt;/sup&gt;Yb, which proved to be approximately &#13;
100 times stronger than in cesium atoms. Transitions were observed between ytterbium &#13;
atomic levels 6s&lt;sup&gt;2&lt;/sup&gt;&amp;nbsp;&lt;sup&gt;1&lt;/sup&gt;S&lt;sub&gt;0&lt;/sub&gt;&amp;nbsp;&amp;rarr; &amp;nbsp;5d6s&amp;nbsp;&lt;sup&gt;3&lt;/sup&gt;D&lt;sub&gt;1&lt;/sub&gt; that corresponded to the wavelength of the absorbed photons of &#13;
408&amp;nbsp;nm. These transitions are forbidden by selection rules; in other words, they occur with very &#13;
low probability. Transitions to upper levels in a beam of ytterbium atoms were excited by &#13;
laser pulses in crossed electric and magnetic fields. The time rate of these excitation &#13;
transitions of atoms was measured by observing the fluorescent emission from spontaneous &#13;
transitions of atoms to lower levels. The time rate of atomic transitions in the &#13;
left-hand-oriented configuration of fields was higher than in the case of right-handed &#13;
orientation. Parity violation arises as a result of mixing of levels of different parity &#13;
due to the weak interaction in the external electric field. So far the accuracy achieved &#13;
in the experiment is only 14% &#13;
but it proved sufficient for detecting the record-high parity in &lt;sup&gt;174&lt;/sup&gt;Yb. Future experimental &#13;
measurement of parity violation in various isotopes of nuclei and in transitions between levels of &#13;
hyperfine splitting could provide new data on the distribution of neutrons in nuclei and perhaps &#13;
could find effects go ing beyond the Standard Model of elementary particles; they will also lead to &#13;
measurements of the anapole moment of nuclei (see &lt;a href="http://ufn.ru/en/articles/1997/11/d/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;40&lt;/b&gt; 1161 (1997)&lt;/a&gt;).&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.103.071601"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;103&lt;/b&gt; 071601 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/9/#1</link>
      <guid>http://ufn.ru/en/news/2009/9/#1</guid>
      <pubDate>Mon, 31 Aug 2009 20:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Mechanism of growth of carbon nanotubes</title>
      <description>Researchers at University of Lyon (France) and the Rice University (USA) established that &#13;
as new atoms join a carbon nanotube in the course of its growth, the nanotube revolves &#13;
around is axis. This mechanism of nanotube growth was predicted in a theoretical paper by &#13;
B.&amp;nbsp;Yakobson. Field emission microscope was used to observe nanotubes in the process of &#13;
catalyzed growth, with the FEM tip moving along the growth zone of the nanotube. The image &#13;
of the nanotube was projected onto a phosphorus-covered screen and the processes taking &#13;
place were video-recorded. In one of the experiments a nanotube made 180 rotations around &#13;
its axis during 11&amp;nbsp;min of observation. Another interesting result was the observation that &#13;
the nanotube revolved stepwise, not smoothly, doing one complete turn in approximately 24 &#13;
steps. Atoms join the rotating nanotube in pairs and form a helical structure. Unique &#13;
mechanical and electronic properties of carbon nanotubes hold great promise for the future &#13;
in designing new superstrong materials and elements of microelectronics. Clarifying the &#13;
mechanism of nanotube growth may help control this process in industrial-scale production.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1021/nl901380u"&gt;&lt;i&gt;Nano Lett.&lt;/i&gt; &lt;b&gt;9&lt;/b&gt; 2961 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/9/#2</link>
      <guid>http://ufn.ru/en/news/2009/9/#2</guid>
      <pubDate>Mon, 31 Aug 2009 20:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Transparent aluminum</title>
      <description>J.&amp;nbsp;Wark (Oxford University, Great Britain) and coworkers observed a transition in aluminum &#13;
to a phase transparent to UV radiation in response to irradiation by laser pulses. &#13;
Aluminum foil was exposed to pulses of the most powerful in the world x-ray laser FLASH &#13;
operating in Hamburg. The radiation flux density for 92&amp;nbsp;eV photons over a small area of &#13;
the foil reached 10&lt;sup&gt;16&lt;/sup&gt;&amp;nbsp;W&amp;nbsp;cm&lt;sup&gt;-2&lt;/sup&gt;. The light of the laser produced single ionization &#13;
of practically all aluminum atoms by knocking out electrons off the L shells, without &#13;
destroying the crystal structure; this kept the specimen transparent to UV photons for &#13;
40&amp;nbsp;fs.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nphys1341"&gt;&lt;i&gt;Nature Physics&lt;/i&gt; &lt;b&gt;5&lt;/b&gt; 693 (2009)&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/9/#3</link>
      <guid>http://ufn.ru/en/news/2009/9/#3</guid>
      <pubDate>Mon, 31 Aug 2009 20:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Nanolaser went over the diffraction limit</title>
      <description>М.Т.&amp;nbsp;Hill (Technical University of Eindhoven, The Netherlands) and his colleagues in The &#13;
Netherlands and the USA designed a microscopic laser whose transverse dimensions are below &#13;
the diffraction limit of the radiation it emits. The device consists of alternating &#13;
semiconducting InP/InGaAs/InP structures of square cross section, 90 to 350&amp;nbsp;nm thick, &#13;
bounded on both sides by dielectric layers of SiN 20&amp;nbsp;nm in thickness; the entire structure &#13;
was coated with an outer layer of silver. Epitaxy, electron-beam lithography and some &#13;
other methods were used to create the laser. Electric current was passed through special &#13;
contacts connected to the semiconductor, and electrons and hole were injected into the &#13;
structure. The layered structure forms a waveguide through which gap plasmon modes can &#13;
propagate, undergoing reflections from silver layers at waveguide boundaries — like light &#13;
does in the Fabry&amp;nbsp;&amp;ndash;&amp;nbsp;Perot interferometer. The device can generate laser radiation with &#13;
wavelength of about 1500&amp;nbsp;nm while being less that a quarter of wavelength thick. The &#13;
diffraction limit is overcome both because the wavelength in a dielectric is shorter than &#13;
that in vacuum and also because photons are transformed into surface plasmons in metal &#13;
layers. The generation of laser light was recorded even at room temperature despite the &#13;
fact that the device is more efficient if it is cooled considerably. Nanolasers may find &#13;
applications in, for example, computers to transfer signals between components of &#13;
microelectronic circuits and thus greatly speed up their work.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1364/OE.17.011107&#13;
"&gt;&lt;i&gt;Optics Express&lt;/i&gt; &lt;b&gt;17&lt;/b&gt; 11107 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/9/#4</link>
      <guid>http://ufn.ru/en/news/2009/9/#4</guid>
      <pubDate>Mon, 31 Aug 2009 20:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Massive compact galaxy in early Universe</title>
      <description>P. van Dokkum (Yale University, USA) and his colleagues measured on the 8-meter Gemini &#13;
telescope the dispersion of stellar velocities in the 1255-0 galaxy. The galaxy is observed at &#13;
redshift &lt;i&gt;z=2,186&lt;/i&gt;, i.e. in the epoch when the age of the Universe was a mere 3 billion years. &#13;
However, with the mass of the galaxy &amp;asymp;&amp;nbsp;10&lt;sup&gt;11&lt;/sup&gt; mass of the Sun, stars in it move with velocity &#13;
dispersion of 510&lt;sup&gt;+165&lt;/sup&gt;&lt;sub&gt;-95&lt;/sub&gt;&amp;nbsp;km&amp;nbsp;s&lt;sup&gt;-1&lt;/sup&gt;, which is approximately 2.5 times greater than the &#13;
velocity dispersion in typical present-day galaxies. The size of the galaxy 1255-0 is however, six &#13;
times smaller than that of present-day elliptical galaxies of the same mass. It is not clear so far &#13;
what mechanism formed such dense galaxies and what was their evolution path. It is conceivable that &#13;
in the time since such galaxies were formed, they merged with other surrounding galaxies and acted &#13;
as seeds of very dense central regions of today's giant galaxies. It is also possible that central &#13;
supermassive black holes formed very early in such galaxies.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nature08220"&gt;&lt;i&gt;Nature&lt;/i&gt; &lt;b&gt;460&lt;/b&gt; 717 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/9/#5</link>
      <guid>http://ufn.ru/en/news/2009/9/#5</guid>
      <pubDate>Mon, 31 Aug 2009 20:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Mass of the &amp;Omega;&lt;sup&gt;-&lt;/sup&gt;&lt;sub&gt;b&lt;/sub&gt;-baryon</title>
      <description>The CDF collaboration at the Tevatron accelerator has measured the mass of the &#13;
&amp;Omega;&lt;sup&gt;-&lt;/sup&gt;&lt;sub&gt;b&lt;/sub&gt;-baryon consisting of a b-quark and two s-quarks. The existence of a doubly &#13;
strange particle &amp;Omega;&lt;sup&gt;-&lt;/sup&gt;&lt;sub&gt;b&lt;/sub&gt; is predicted by the Standard model of elementary particles; &#13;
it has first been observed by the D0 collaboration and announced in August 2008. These &#13;
particles was created in the CDF experiment in p-anti-p collisions at the center-of-mass &#13;
energy of 1.96 TeV and were identified at the confidence level of 5.5&amp;sigma; through the &#13;
chain of decays to lighter particles: &amp;Omega;&lt;sup&gt;-&lt;/sup&gt;&lt;sub&gt;b&lt;/sub&gt;&amp;rarr;J/&amp;Psi;&amp;Omega;&lt;sup&gt;-&lt;/sup&gt;, &#13;
J/&amp;Psi;&amp;rarr;&amp;mu;&lt;sup&gt;+&lt;/sup&gt;&amp;mu;&lt;sup&gt;-&lt;/sup&gt;, &#13;
&amp;Omega;&lt;sup&gt;-&lt;/sup&gt;&amp;rarr;&amp;Lambda;K^&lt;sup&gt;-&lt;/sup&gt;, &#13;
&amp;Lambda;&amp;rarr;p&amp;pi;&lt;sup&gt;-&lt;/sup&gt;. On the whole, approximately &#13;
5&amp;times;10&lt;sup&gt;11&lt;/sup&gt;  p-anti-p collisions were studied and 16&lt;sup&gt;+6&lt;/sup&gt;&lt;sub&gt;-4&lt;/sub&gt; production events &#13;
of the &amp;Omega;&lt;sup&gt;-&lt;/sup&gt;&lt;sub&gt;b&lt;/sub&gt;-baryon were recorded. The resulting mass of 6054.4&amp;plusmn;6.8(stat.)&amp;plusmn;0.9(syst.)&amp;nbsp;MeV differs from the value 6165&amp;plusmn;10(stat.)&amp;plusmn;13(syst.)&amp;nbsp;MeV reported by &#13;
the D0. The results of the D0 and CDF are statistically incompatible and neither &#13;
experiment found any special features near the mass measured in the other experiment. Such &#13;
features could be an evidence that in fact the two experiments observed different &#13;
particles. Furthermore, the rate of creation of &amp;Omega;&lt;sup&gt;-&lt;/sup&gt;&lt;sub&gt;b&lt;/sub&gt;-baryons in the CDF experiment &#13;
was found to be lower than in the D0. The causes of these discrepancies have not yet been &#13;
identified. Russian scientists from JINR and ITEP take part in the CDF Collaboration.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0905.3123"&gt;arXiv:0905.3123v1 [hep-ex]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/8/#1</link>
      <guid>http://ufn.ru/en/news/2009/8/#1</guid>
      <pubDate>Fri, 31 Jul 2009 20:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Novel magnetic effect</title>
      <description>Researchers at the National Institute of Standards and Technologies (NIST, USA) and the Institute of &#13;
Solid State Physics (Chernogolovka, Russia) have discovered that the magnetic ordering in &#13;
ferromagnets longer range under certain conditions than was earlier expected. They &#13;
studied heterostructures consisting of a thin ferromagnetic film coated with a grid of &#13;
antiferromagnetic compound FeMn. They used the technique of magnetooptical visualization which makes &#13;
it possible to follow in real time the formation, growth and disappearance of magnetic domains. The &#13;
antiferromagnetic grid creates the pinning effect — the ferromagnetic magnetization gets pinned in &#13;
certain directions. It was assumed that the magnetic interaction of this type should penetrate into &#13;
ferromagnetic films to a depth of at most several tens of nanometers beneath the FeMn film. In fact &#13;
the structure of domain walls (domain boundaries) in the ferromagnetic film was sensitive to this &#13;
influence even at a distance of 50&amp;nbsp;&amp;micro;m from the nearest FeMn strip, which is greater by three &#13;
orders of magnitude than the expected penetration range. One possible explanation of this effect is &#13;
the topological stability of the domains in the upper grid of the antiferromagnetic; however, &#13;
further investigation is required to fully clarify the phenomenon discovered. The results of the &#13;
experiment are important for designing magnetic storage devices with high density of data recording.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevB.79.144435"&gt;&lt;i&gt;Phys. Rev.&lt;/i&gt; &lt;b&gt;B 79&lt;/b&gt; 144435 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/8/#2</link>
      <guid>http://ufn.ru/en/news/2009/8/#2</guid>
      <pubDate>Fri, 31 Jul 2009 20:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Quantum walks</title>
      <description>Researchers at the Bonn University were able to implement the algorithm of quantum random &#13;
walks suggested by R.&amp;nbsp;Feynman, for neutral cesium atoms in the potential field of two &#13;
overlapping optical lattices. Standing waves formed by two laser beams created a &#13;
one-dimensional periodic potential barrier of height k&lt;sub&gt;B&lt;/sub&gt;&amp;times;80&amp;nbsp;&amp;micro;K where k&lt;sub&gt;B&lt;/sub&gt; is &#13;
the Boltzmann constant. Cesium atoms possessed thermal energy k&lt;sub&gt;B&lt;/sub&gt;&amp;times;10&amp;nbsp;&amp;micro;K and &#13;
could exist in two states of hyperfine splitting of levels each of which was &#13;
quantum-correlated with one of the directions of atomic displacement to the left or to the &#13;
right; the permeability of the barrier depended on the internal state of the atom owing to &#13;
a certain polarization of laser beams. The “step” of an atom in the lattice was &#13;
initiated by switching the polarization, after which the position of the atom could be &#13;
determined using its fluorescent emission. In contrast to the classical random walk that &#13;
takes place, for example, in diffusion, in the quantum case momentum imparted to the atom &#13;
transferred it to a state of quantum superposition of two possible directions of motion. &#13;
The next pulse created a new configuration of the atomic wave function which included a &#13;
superposition of the states of the preceding steps. The experiment implemented up to &lt;i&gt;N=24&lt;/i&gt; steps. The observation of the final positions of trapped atoms showed that their &#13;
displacements could indeed be regrarded as quantum walking in which the summary &#13;
displacement proportional to &lt;i&gt;N&lt;/i&gt;. In the case of decoherence at each step of quantum walking the &#13;
characteristics of walking tended to the classical law &lt;i&gt;N&lt;sup&gt;&amp;frac12;&lt;/sup&gt;&lt;/i&gt;. The quantum &#13;
walk algorithm has already been implemented earlier in a number of systems but the &#13;
experiment of М.&amp;nbsp;Karski and his coworkers outlined above is the closest to the original &#13;
one suggested by R.&amp;nbsp;Feynman.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1174436"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;325&lt;/b&gt; 174 (2009) &lt;/a&gt;;&#13;
&lt;a href="http://arxiv.org/abs/0907.1565"&gt;arXiv:0907.1565v1 [quant-ph]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/8/#3</link>
      <guid>http://ufn.ru/en/news/2009/8/#3</guid>
      <pubDate>Fri, 31 Jul 2009 20:00:03 GMT</pubDate>
    </item>
    <item>
      <title>A single-molecule optical transistor</title>
      <description>J.&amp;nbsp;Hwang and his colleagues at the Swiss Federal Institute of Technology (ETH Zurich) &#13;
designed a transistor using a single molecule of dibenzanthanthrene dye impregnated into a &#13;
crystalline matrix of an organic compound tetradecane. When the molecule was cooled by &#13;
liquid helium to a temperature of 1.4&amp;nbsp;K, its effective cross section of interaction with a &#13;
photon increased to the value of the cross section of focused laser beams used in the &#13;
experiment. One of the beams served as the “gate” of the transistor, controlling the &#13;
quantum state of the molecule. Depending on what energy level the molecule was on, it &#13;
scattered the second, more powerful beam differently and this allowed the control over the &#13;
passage of the beam through the molecule; this is an analogy to how current is controlled &#13;
in a conventional electron transistor. In the future such photonic devices may become a &#13;
viable alternative to electronic systems owing to high speed and low heat production, for &#13;
instance for building optical computers.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nature08134"&gt;&lt;i&gt;Nature&lt;/i&gt; &lt;b&gt;460&lt;/b&gt; 76 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/8/#4</link>
      <guid>http://ufn.ru/en/news/2009/8/#4</guid>
      <pubDate>Fri, 31 Jul 2009 20:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Generation of gamma radiation very close to a black hole</title>
      <description>Joint observations using gamma and radio telescopes allowed astronomers to establish that &#13;
the high-energy gamma radiation of the M87 galaxy is generated in the immediate vicinity &#13;
of a supermassive black hole. The giant elliptic galaxy M87 is the central galaxy of the &#13;
Virgo galaxy cluster and is located at a distance of 50 million light years from the &#13;
Earth. A black hole with a mass of about 3&amp;times;10&lt;sup&gt;9&lt;/sup&gt; solar masses is found at the &#13;
center of the M87 galaxy. Matter falls onto the black hole from the accretion disk and &#13;
produces high-power electromagnetic flares in various frequency ranges and ejecting &#13;
relativistic plasma jets thrown to distances of thousands of light years. Currently gamma &#13;
telescopes have low resolving power and are incapable of pinpointing the exact area within &#13;
the galaxy from which the highest energy radiation is emitted. It proved possible to &#13;
overcome this difficulty since gamma flares are accompanied by simultaneous radio &#13;
flares. When a gamma flare ends, charged particles continue to move along the jet and &#13;
therefore the radio emission intensity continues to rise for considerably longer but gamma &#13;
and radio flares start practically at the same time and therefore must be produced  in &#13;
the same source which was identifiable in view of very high resolution of the &#13;
radiotelescopes. Gamma flares from the nucleus of the M87 galaxy were recorded for two &#13;
years using the atmospheric Cerenkov detectors VERITAS, H.E.S.S. and MAGIC, and radio &#13;
flares were observed in parallel, using an array of ten VEBA radiotelescopes of the National &#13;
Radio Observatory (NRAO). It was established by radio observation that flares are generated &#13;
at a distance from the central black hole not bigger than 50 times the radius of its event &#13;
horizon. These observational data can help improve the theoretical models of jet formation &#13;
and clarify the mechanisms of generation of emission.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1175406"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;325&lt;/b&gt; 444 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/8/#5</link>
      <guid>http://ufn.ru/en/news/2009/8/#5</guid>
      <pubDate>Fri, 31 Jul 2009 20:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Landau levels in graphene</title>
      <description>Researchers at the National Institute of Standards and Technology (NIST) and Georgia &#13;
Institute of Technology carried out for the first time direct measurements of Landau &#13;
levels in a graphene specimen using a scanning tunneling microscope. Landau levels are &#13;
defined as discrete quantum energy levels of electrons moving on cyclotron orbits in &#13;
magnetic field. The velocity of free electrons in graphene (i.e. in a one atom thick &#13;
carbon layer) is almost independent of their energy; in other words, the law of dispersion &#13;
resembles that of massless particles. As shown in theoretical papers, this implies that energy&#13;
spacings between consecutive Landau levels are not all equal as they are in ordinary metals &#13;
and in two-dimensional electron gas. It was also predicted that at the zero level the &#13;
energy of electrons is zero regardless of the strength of the applied magnetic field. &#13;
Graphene films were studied on a silicon carbide SiC substrate in high vacuum at ultralow &#13;
temperature. Conductivity was measured as a function of applied voltage using a microscope &#13;
needle. About 20 Landau levels were detected by recording conductivity peaks. The &#13;
experiment showed that in agreement with theoretical expectations, Landau levels in &#13;
graphene are not equidistant and energy at the zero level is permanently zero.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1171810"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;324&lt;/b&gt; 924 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/7/#1</link>
      <guid>http://ufn.ru/en/news/2009/7/#1</guid>
      <pubDate>Tue, 30 Jun 2009 20:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Collective quantum tunneling in nanowires</title>
      <description>A.&amp;nbsp;Bezryadin and his colleagues at the University of Illinois discovered the effect of &#13;
quantum tunneling of an entire bunch consisting of about &amp;asymp;10&lt;sup&gt;5&lt;/sup&gt; electrons. Since the number &#13;
of simultaneously tunneling electrons was so considerable, this process can be called the &#13;
macroscopic quantum tunneling. Tunneling took place owing to a phase slip in a &#13;
superconducting wire (of a diameter of about one nanometer) from a state with higher &#13;
electric current to a state with lower electric current. Excess energy is released in this &#13;
quantum transition as heat, the wire warms up and transfers from superconducting to normal &#13;
state. It is likely that the discovered effect of macroscopic tunneling will find applications for &#13;
quantum calculations.&#13;
&#13;
Sources: &lt;a href="http://dx.doi.org/doi:10.1038/nphys1276"&gt;&lt;i&gt;Nature Physics&lt;/i&gt; &lt;b&gt;5&lt;/b&gt; 503 (2009)&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/7/#2</link>
      <guid>http://ufn.ru/en/news/2009/7/#2</guid>
      <pubDate>Tue, 30 Jun 2009 20:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Acoustic lasers</title>
      <description>P.M.&amp;nbsp;Walker and his coworkers at the Nottingham University (UK) and the V.Ye.&amp;nbsp;Loshkarev &#13;
Institute of Semiconductor Physics in Kiev (Ukraine) designed a coherent source of sound &#13;
waves working in the teraherz frequency range. A collimated beam of phonons with &#13;
wavelength of about one nanometer is generated in layered semiconductor structure &#13;
(superlattice) with specially selected spacings between fifty alternating layers of &#13;
gallium arsenide and aluminum arsenide. Each layer is only several atoms thick. The new &#13;
device is given a name saser (sound laser). The generation mechanism is based on strong &#13;
electron-phonon coupling in semiconducting layers. Electrons in the upper layer are &#13;
excited by nanosecond pulses of a conventional laser and emit phonons. Phonons are &#13;
reflected at interfaces between layers and returned to the upper layer where they again &#13;
interact with electrons; this leads to synchronization and coherence of the emitted sound &#13;
pulses. Sound lasers have already been created before but they used other principles &#13;
for sound generation and worked at much lower frequencies — in the GHz range. The &#13;
acoustic emission of the new saser at frequencies on the order of one THz may find many &#13;
useful applications.&#13;
&#13;
Sources: &lt;a href="http://dx.doi.org/10.1103/PhysRevB.79.245313"&gt;&lt;i&gt; Phys. Rev.&lt;/i&gt; &lt;b&gt;B 79&lt;/b&gt; 245313 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/7/#3</link>
      <guid>http://ufn.ru/en/news/2009/7/#3</guid>
      <pubDate>Tue, 30 Jun 2009 20:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Gamma-ray burst during the reionization epoch</title>
      <description>The BAT gamma telescope of the Swift space observatory detected a remotest cosmic &#13;
gamma-ray burst GRB&amp;nbsp;090423. Immediately after detection of the gamma burst, x-ray and &#13;
optical afterglow was observed by several telescopes and certain features of its spectrum &#13;
led to the determination of the red shift of the burst: &lt;i&gt;z&amp;nbsp;&amp;asymp;&amp;nbsp;8,2&lt;/i&gt;. The host galaxy of &#13;
the burst GRB&amp;nbsp;090423 has not yet been identified. Judging by the shape of the burst, it &#13;
belongs to the class of long gamma-ray bursts produced by explosions of a special class of &#13;
supernovas known as hypernovas. The burst GRB&amp;nbsp;090423 flared up at the epoch when the age &#13;
of the Universe was only about 600 million years. However, its properties (total energy &#13;
output, peak luminosity and shape of the light curve) do not differ from those of typical &#13;
gamma bursts that arrive from intermediate and small red-shift sources, which points to &#13;
similarity in the processes involved in explosions of early and contemporary stars. The &#13;
burst GRB&amp;nbsp;090423 took place at the reionization stage which ended only at &lt;i&gt;z&amp;nbsp;&amp;asymp;&amp;nbsp;6&lt;/i&gt;; &#13;
hence, observing gamma-ray bursts at high red shifts can help in understanding the physics &#13;
of reionization processes and star formation in the early Universe. In particular, the &#13;
conjecture that the rate of gamma burst generation follows that of star formation is found &#13;
to be wrong because if it were true, the probability of observing gamma-ray bursts with &#13;
redshifts &lt;i&gt;z&amp;nbsp;&amp;gt;&amp;nbsp;8&lt;/i&gt; would be very low. A possible hypothesis is that a relatively higher number of very massive stars were formed during early cosmological epochs than are now, and that &#13;
the UV radiation of these stars could be the source of reionization of the Universe.&#13;
&#13;
Sources: &lt;a href="http://arxiv.org/abs/0906.1578"&gt;arXiv:0906.1578v2 [astro-ph.CO]&lt;/a&gt;;&#13;
&#13;
&lt;a href="http://arxiv.org/abs/0906.1577"&gt;arXiv:0906.1577v2 [astro-ph.CO]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/7/#4</link>
      <guid>http://ufn.ru/en/news/2009/7/#4</guid>
      <pubDate>Tue, 30 Jun 2009 20:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Exoplanet in the M31 galaxy</title>
      <description>More than 300 planets outside the Solar system have been found by now from the periodic &#13;
fluctuations of brightness or trajectories of stars. Eight more planets were found by &#13;
observing microlensing at lensing stars which gravitationally focus radiation of more &#13;
remote source stars on the line of sight. Planets gravitationally affect the light curve &#13;
in the course of the passing of the lens across the source star as background, warping this &#13;
curve in a certain manner. A number of papers analyzed the likelihood of this type of &#13;
detection of planets in the nearest neighbor galaxies. G.&amp;nbsp;Ingrosso (University of Salento, &#13;
Italy), A.F.&amp;nbsp;Zakharov (ITEP and JINR, Russia) and their coworkers carried out a new &#13;
theoretical study of the strategy of searching for new planets in other galaxies. They &#13;
predicted the characteristics of corrections to the light curve and found other parameters &#13;
of lensing events involving planets, and also gave Monte Carlo predictions of the &#13;
probabilities of specific observations with telescopes working with mirrors of different &#13;
diameters. Thus this lensing technique can detect planets in other galaxies only 20 times &#13;
more massive than the Earth. The authors of the paper analyzed earlier observations of &#13;
lensing of stars in the galaxy M31 (Andromeda galaxy) and noticed that one of the stars of &#13;
the M31 may have already displayed the signs of a planet. It was assumed earlier that a &#13;
binary lensing star consisting of a pair of ordinary stars may have been responsible for &#13;
the microlensing event РА-99-N2 recorded in 2004. However, according to G.&amp;nbsp;Ingrosso, &#13;
A.F.&amp;nbsp;Zakharov &#13;
et al the satellite of the main star is only 6.34 times more massive than Jupiter. This mass is &#13;
approximately one half of the mass of the lightest stars — brown dwarfs — so that the satellite &#13;
can be treated as a planet.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0906.1050v1"&gt;arXiv:0906.1050v1 [astro-ph.SR]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/7/#5</link>
      <guid>http://ufn.ru/en/news/2009/7/#5</guid>
      <pubDate>Tue, 30 Jun 2009 20:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Rydberg atom in a molecule</title>
      <description>V.&amp;nbsp;Bendkowsky and her coworkers at the Universities of Stuttgart and Oklahoma prepared and &#13;
then investigated Rb&lt;sub&gt;2&lt;/sub&gt; molecules in which one of the rubidium atoms is in a Rydberg state &#13;
with the outer electron in the s-state and &lt;i&gt;n&amp;nbsp;=&amp;nbsp;34-40&lt;/i&gt; while the second atom remains in the ground state. The bonding between these atoms is caused by the scattering of the &#13;
Rydberg electron on the electrons of the second atom. As Enrico Fermi established in 1934 &#13;
the interaction potential in this sort of scattering of low-energy electrons may be &#13;
attractive (negative scattering length). Since the frequency of the electron in the &#13;
Rydberg atom is much higher than the characteristic frequency of interaction, &#13;
the wave function is practically undistorted by scattering. The molecules obtained have a &#13;
lifetime before decay of about 18&amp;nbsp;&amp;micro;s and are about 100&amp;nbsp;nm in size, which is 1900 times the Bohr radius. The molecules were created by laser-excitation  of rubidium atoms in a &#13;
Ioffe&amp;nbsp;&amp;ndash;&amp;nbsp;Pritchard magnetic trap at a temperature of 3.5&amp;nbsp;&amp;micro;K. Oscillation spectra of &#13;
molecules were measured in the ground and first excited states. The results obtained  are &#13;
in good agreement with the results of theoretical calculations. The researchers expressed &#13;
hope that similar molecules may soon be created with the Rydberg electron in p-state, as well as a &#13;
three-atom molecule and a molecule belonging to a class of what is known as trylobite &#13;
molecules in which the Rydberg electron has a high angular momentum. &#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nature07945"&gt;&lt;i&gt;Nature&lt;/i&gt; &lt;b&gt;458&lt;/b&gt; 1005 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/6/#1</link>
      <guid>http://ufn.ru/en/news/2009/6/#1</guid>
      <pubDate>Sun, 31 May 2009 20:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Superconductivity of europium</title>
      <description>Atoms of bivalent rare-earth element europium at normal atmospheric pressure possess high &#13;
magnetic moments; this is an obstacle to europium's transition to superconducting state. &#13;
However, researchers of the Washington University in St.&amp;nbsp;Louis J.S.&amp;nbsp;Schilling and &#13;
М.&amp;nbsp;Debessai established that europium becomes weak Van Vleck paramagnetic under pressure of &#13;
80&amp;nbsp;GPa and acquires superconducting properties. Its superconducting transition temperature &#13;
is &lt;i&gt;T&lt;sub&gt;c&lt;/sub&gt;&amp;nbsp;=&amp;nbsp;1,8&lt;/i&gt;&amp;nbsp;K, and &lt;i&gt;T&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt; grows linearly with increasing pressure, reaching &lt;i&gt;T&lt;sub&gt;c&lt;/sub&gt;&amp;nbsp;=&amp;nbsp;2,75&lt;/i&gt;&amp;nbsp;K at 1142&amp;nbsp;GPa. Eu specimens were studied in a diamond anvil cell. The &#13;
superconducting transition was identified by measuring electric conductivity and &#13;
electric susceptibility in ac field. Electron levels of europium get distorted under &#13;
high pressure so it is transformed from a bivalent to a trivalent element. A similar &#13;
effect has already been observed in Americium that also becomes Van Vleck paramagnetic and &#13;
superconducting under pressure (&lt;i&gt;T&lt;sub&gt;c&lt;/sub&gt;&amp;nbsp;=&amp;nbsp;0,79&lt;/i&gt;&amp;nbsp;K). Europium is the 53rd element which &#13;
manifested superconducting properties in elemental state, and the 23rd element in which &#13;
superconductivity arises only on application of high pressure. &#13;
&#13;
Sources: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.102.197002"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;102&lt;/b&gt; 197002 (2009) &lt;/a&gt;; &#13;
&lt;a href="http://arxiv.org/abs/0903.1808"&gt;arXiv:0903.1808v1 [cond-mat.supr-con]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/6/#2</link>
      <guid>http://ufn.ru/en/news/2009/6/#2</guid>
      <pubDate>Sun, 31 May 2009 20:00:02 GMT</pubDate>
    </item>
    <item>
      <title>“Incandescent lamp” made of a nanotube</title>
      <description>B.C.&amp;nbsp;Regan and colleagues at the California NanoSystems Institute at UCLA (Los-Angeles) &#13;
studied the incandescence of current-heated carbon nanotube. This experiment allowed them &#13;
to  test Planck's law of radiation almost to the limit of applicability of thermodynamics. &#13;
Two gold contacts were lithographically attached to the ends of a nanotube &#13;
placed over a hole in the silicon substrate in vacuum. The multilayer carbon nanotube was about 100 &#13;
atoms thick. When electric current was passed through it, it heated up and began to glow. &#13;
The emission wavelength was on the order of the nanotube length and much larger than the &#13;
tube thickness. The radiation spectrum of nanotube emission was studied at different &#13;
temperatures (different currents) by using a microscope and a set of optical filters. The &#13;
classical thermodynamics used together with Max Planck's quantum hypothesis to derive the &#13;
spectrum of blackbody radiation is applicable only to macroscopic systems consisting of a &#13;
very large number of particles. The spectrum of thermal emission of a nanotube was &#13;
nevertheless found after corrections for geometric factors to be in good agreement with &#13;
the Planck formula. A nanotube has microscopic dimensions but is still large enough for a &#13;
statistical description. At the same time, quantum properties of a microscopic system &#13;
already manifest themselves sufficiently well. This experiment therefore dealt with the &#13;
properties at the borderline between the thermodynamic and quantum regimes.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.102.187402"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;102&lt;/b&gt; 187402 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/6/#3</link>
      <guid>http://ufn.ru/en/news/2009/6/#3</guid>
      <pubDate>Sun, 31 May 2009 20:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Topological Hall effect in MnSi</title>
      <description>A number of neutron scattering experiments provided indirect evidence that the distribution of &#13;
electron spins in the compound MnSi contains a nontrivial topological structure composed of &#13;
quasiparticles known as skyrmions. Skyrmions are described by chiral soliton models suggested by &#13;
Tony Skyrme in 1961. It is assumed that topological excitations we call skyrmions arise in MnSi due &#13;
to the spin-orbital interaction and form a lattice composed of three helices. Two independent &#13;
groups of experimenters carried out new experiments that confirm this picture. М.&amp;nbsp;Lee and his &#13;
colleagues in the USA and Japan studied the Hall effect in a specimen of MnSi under pressure of &#13;
6-12&amp;nbsp;kbar. They found an additional contribution to conductivity detected at the magnetic field in &#13;
the interval 0.1-0.45&amp;nbsp;T, which is not typical of the conventional Hall effect. In the model with &#13;
skyrmions this contribution is known as the topological Hall effect. In another experiment &#13;
A.&amp;nbsp;Neubauer and his colleagues in Germany also studied the Hall effect in MnSi, but in a different &#13;
segment of the phase diagram of this compound. Similar features of the Hall effect were discovered &#13;
and could be explained in terms of skyrmion distribution. &#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.102.186601"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;102&lt;/b&gt; 186601 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/6/#4</link>
      <guid>http://ufn.ru/en/news/2009/6/#4</guid>
      <pubDate>Sun, 31 May 2009 20:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Refined Hubble constant</title>
      <description>240 Cepheid variables and several supernova explosions of class Ia in remote galaxies were &#13;
observed using the Hubble Space Telescope (HST) which made it possible to improve the &#13;
accuracy of the Hubble constant by a factor of more than two, reaching the level of &amp;asymp;5%. &#13;
Some of the observed Cepheids (variable stars with a known period vs. luminosity curve) &#13;
were located in the same galaxies as six of supernovas of class Ia; this made it possible &#13;
to carry out direct joint calibration of various distance units. The team also recorded &#13;
Cepheids in the galaxy NGC&amp;nbsp;4258 which contains cosmic masers. Using the geometry of the maser &#13;
emission, the distance to the galaxy was measured with sufficient accuracy. Furthermore, &#13;
the Hubble telescope measured the parallax of ten Cepheids in our Galaxy. This led to &#13;
further refinement of the accuracy of calibration of distance measurement. The importance &#13;
of calibration is illustrated by the fact that the relative accuracy of the Hubble diagram &#13;
for supernovas of class Ia is less than 1% &#13;
but the presence of systematic errors does not yet permit reaching the same accuracy in measuring &#13;
the absolute value of the Hubble constant. Likewise the observation of baryonic oscillations in the spectrum &#13;
of microwave background radiation does not yet reach better accuracy without the assumption &#13;
that the Universe is flat plus the hypothesis that the parameter of the equation of state of dark &#13;
energy is &lt;i&gt;w&amp;nbsp;=&amp;nbsp;p/(&amp;rho; c&lt;sup&gt;2&lt;/sup&gt;)&amp;nbsp;=&amp;nbsp;–1&lt;/i&gt; (the cosmological constant). According to the new HST &#13;
data, the refined value of the Hubble constant is &lt;i&gt;H&lt;sub&gt;0&lt;/sub&gt;&amp;nbsp;=&amp;nbsp;74,2&amp;nbsp;&amp;plusmn;&amp;nbsp;3,6&lt;/i&gt;&amp;nbsp;km&amp;nbsp;s&lt;sup&gt;-1&lt;/sup&gt;Mpc&lt;sup&gt;-1&lt;/sup&gt;. Together with the WMAP data over the last five years this gives &lt;i&gt;w&amp;nbsp;=&amp;nbsp;–1,12&amp;nbsp;&amp;plusmn;&amp;nbsp;0,12&lt;/i&gt;. &#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0905.0695v1"&gt;arXiv:0905.0695v1 [astro-ph.CO]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/6/#5</link>
      <guid>http://ufn.ru/en/news/2009/6/#5</guid>
      <pubDate>Sun, 31 May 2009 20:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Unusual elementary particle</title>
      <description>The CDF collaboration detected an unusual particle in an experiment on the &#13;
Tevatron accelerator; so far this particle could not be classified in terms of the &#13;
accepted quark recipe of building mesons and baryons. The researchers selected &#13;
B&lt;sup&gt;+&lt;/sup&gt;&amp;nbsp;&amp;rarr;&amp;nbsp;J/&amp;psi;&amp;phi;K&lt;sup&gt;+&lt;/sup&gt; decays. It was found that the intermediate state of &#13;
the decays are new particles Y(4140) with a mass of about 4140&amp;nbsp;MeV. The &#13;
experimenters recorded 14&amp;plusmn;5 such events at statistical significance of 3.8 &#13;
standard deviations. The assumption that Y(4140) is one of the states of the &#13;
system of c-anti-c quarks met with serious difficulties in describing the &#13;
observed characteristics of the decays; the structure of the new particle is &#13;
still unclear. There is a possibility that Y(4140) is a hadronic molecule, a &#13;
hybrid particle that includes gluons as its components, or that Y(4140) is a new &#13;
four-quark state. The Y(4140) particle is another in a series of exotic &#13;
particles discovered in recent years (see &lt;a href="http://ufn.ru/en/news/2007/12/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;50&lt;/b&gt; 1289 (2007)&lt;/a&gt;).&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0903.2229"&gt;arXiv:0903.2229v1 [hep-ex]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/5/#1</link>
      <guid>http://ufn.ru/en/news/2009/5/#1</guid>
      <pubDate>Thu, 30 Apr 2009 20:00:01 GMT</pubDate>
    </item>
    <item>
      <title>The Efimov effect for four particles</title>
      <description>In 2006 H.-C. Nagerl and coworkers at the University of Insbruck in Austria &#13;
observed for the first time  bound quantum states of three cesium atoms (see &#13;
&lt;a href="http://ufn.ru/en/news/2006/4/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;49&lt;/b&gt; 438 (2006)&lt;/a&gt;). The object of study was the Bose&amp;nbsp;&amp;ndash;&amp;nbsp;Einstein &#13;
condensate in which the intensity of interaction between atoms was controlled by &#13;
the magnetic field and the bound states were identified by determining &#13;
recombination losses. The effect of formation of trimers, predicted by &#13;
V.I.&amp;nbsp;Efimov in a theoretical paper in 1970, can arise even in the absence of &#13;
bound paired states of atoms. After this discovery, in 2007-2008 two groups of &#13;
researchers made a theoretical prediction that a similar effect is possible for &#13;
four particles too; furthermore, some observational evidence of formation of &#13;
bound quartets was found among the data of the first experiment. H.-C.&amp;nbsp;Nagerl &#13;
and his colleagues carried out a new experiment using a technique completely &#13;
reproducing that of the earlier experiment. The presence of bound quantum states &#13;
of four particles was demonstrated unambiguously. The range of applicability of &#13;
the Efimov effect was thus extended to quartets of atoms. In contrast to &#13;
trimers, bound quartets form only a pair of universal states and not an infinite &#13;
sequence. The  data obtained in this work will be used to test principally important &#13;
aspects of quantum mechanics.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.102.140401"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;102&lt;/b&gt; 140401 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/5/#2</link>
      <guid>http://ufn.ru/en/news/2009/5/#2</guid>
      <pubDate>Thu, 30 Apr 2009 20:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Doubly magic nucleus &lt;sup&gt;24&lt;/sup&gt;О</title>
      <description>Nuclei of the unstable oxygen isotope &lt;sup&gt;24&lt;/sup&gt;О having a large excess of neutrons &#13;
were studied at the GSI laboratory (Darmschtadt, Germany). It was found that &#13;
these nuclei are doubly magic, i.e. that their proton and neutron shells are &#13;
completely filled, despite a strong distorsion of level structure at the &#13;
nucleus stability boundary. A beam of &lt;sup&gt;24&lt;/sup&gt;О nuclei was generated &#13;
in the accelerator by sending &lt;sup&gt;48&lt;/sup&gt;Ca nuclei into a target. This process &#13;
created three &lt;sup&gt;24&lt;/sup&gt;О nuclei per second which then collided with a carbon &#13;
target, losing one neutron each. The form of the momentum distribution of the &#13;
resulting &lt;sup&gt;23&lt;/sup&gt;О nuclei made it possible to determine the structure of nucleon &#13;
shells in &lt;sup&gt;24&lt;/sup&gt;О nuclei. It was confirmed that &lt;sup&gt;24&lt;/sup&gt;О are indeed doubly &#13;
magic nuclei with spherically symmetric shells. The study of &lt;sup&gt;24&lt;/sup&gt;О isotopes &#13;
is important for nuclear astrophysics because they may be born in supernova &#13;
explosions; these nuclei may also be present in the crust of neutron stars.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.102.152501"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;102&lt;/b&gt; 152501 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/5/#3</link>
      <guid>http://ufn.ru/en/news/2009/5/#3</guid>
      <pubDate>Thu, 30 Apr 2009 20:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Optical Maxwell's demon</title>
      <description>J.J.&amp;nbsp;Thorn and his colleagues at the Oregon University created an optical &#13;
barrier that lets through atoms of &lt;sup&gt;87&lt;/sup&gt;Rb in one direction only. Two almost &#13;
parallel laser beams separating a dipole atomic trap into two parts were focused near its center. &#13;
The frequency of one of the beams differed from the resonance frequency of transition between &#13;
sublevels of hyperfine splitting in &lt;sup&gt;87&lt;/sup&gt;Rb. This beam created a potential barrier whose &#13;
permeability for an atom depends on its state: atoms on the lower subsevel pass through the beam &#13;
unobstracted while the potential created by the barrier for the excited atoms is repulsive. The &#13;
frequency of the second laser equals the frequency of transition between the sublevels. If an atom &#13;
in the ground state crosses the second beam and passes from one side of the trap to the other, it &#13;
absorbs a photon from the second beam and after this is unable to pass through the barrier in the &#13;
opposite direction. As a result, atoms accumulate on only one side of the barrier. This system of &#13;
beams which operates as an atomic diode is an analog of Maxwell's demon. By analogy to Maxwell's &#13;
thought experiment, it is possible to experimentally check how entropy is transferred between the &#13;
parts of the system in the case of the optical barrier. The reduction in entropy caused by the &#13;
displacement of atoms to one side of the trap is compensated for by the production of entropy when &#13;
photons are scattered. Furthermore, this technique is of interest for developing new ways of laser &#13;
cooling of atoms.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0903.3635v1"&gt;arXiv:0903.3635v1 [physics.atom-ph]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/5/#4</link>
      <guid>http://ufn.ru/en/news/2009/5/#4</guid>
      <pubDate>Thu, 30 Apr 2009 20:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Superconductivity in SrFe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt;</title>
      <description>Scientists at the Tokyo Institute of Technology discovered that after the &#13;
compound SrFe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt; was treated with steam, it become a superconductor with &#13;
the temperature of superconducting transition &lt;i&gt;T&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt;&amp;nbsp;&amp;asymp;&amp;nbsp;25&amp;nbsp;К. The &#13;
compound SrFe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt; belongs to a class of new layered iron-based &#13;
superconductors. Its intense study began in 2007 (see &lt;a href="http://ufn.ru/en/articles/2008/12/b/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;51&lt;/b&gt; 1201 (2008)&lt;/a&gt;). However, superconductivity arises in these compounds only when they are &#13;
doped with certain impurities or under high pressures. H.&amp;nbsp;Hosono and his &#13;
coworkers exposed a film of pure (undoped) SrFe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt; to moist atmospheric &#13;
air which resulted in the samples becoming superconducting. Checking &#13;
demonstrated that exposure to individual components of air (nitrogen, oxygen &#13;
or carbon dioxide) without H&lt;sub&gt;2&lt;/sub&gt;O did not produce such changes. So far the &#13;
exact mechanism of the effect of H&lt;sub&gt;2&lt;/sub&gt;O remains unclear. It is suggested that &#13;
either oxygen atoms of water molecules penetrate the structure of the crystal &#13;
SrFe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt;, or that strontium atoms bind to the OH group and form atomic &#13;
vacancies. Superconductivity arises in response to application of water in some &#13;
other (not iron-based) layered compounds too but neutron diffraction studies established that &#13;
interlayer spacings in SrFe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt; do not grow in response to water treatment but are reduced. It &#13;
was also found that the superconductivity of SrFe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt; caused by water is strongly anisoropic &#13;
in magnetic field (&lt;i&gt;T&lt;sub&gt;c&lt;/sub&gt;&lt;/i&gt; depends on the field orientation) — in contrast to the almost &#13;
isotropic superconductivity of SrFe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt; doped with cobalt atoms.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0903.3710"&gt;arXiv:0903.3710v1 [cond-mat.supr-con]&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/5/#5</link>
      <guid>http://ufn.ru/en/news/2009/5/#5</guid>
      <pubDate>Thu, 30 Apr 2009 20:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Search for the Higgs boson</title>
      <description>New constraints on the possible mass of the Higgs boson have been established by combining the data &#13;
of two experiments CDF and D0 conducted at the Tevatron accelerator of the Enrico Fermi National &#13;
Accelerator Laboratory. It was obtained earlier at the CERN electron-positron collider that the &#13;
Higgs boson mass is greater than 114&amp;nbsp;GeV. On the other hand, theoretical calculations for processes &#13;
involving the Higgs boson produced the upper bound on its mass as 185&amp;nbsp;GeV. Systematic searches are &#13;
conducted nowadays for the Higgs boson in the possible mass range of 114-185&amp;nbsp;GeV and certain &#13;
intervals within this range have already been excluded (see &lt;a href="http://ufn.ru/en/news/2008/9/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;51&lt;/b&gt; 979 (2008) &lt;/a&gt;). According to the &#13;
data of CDF and D0, the Higgs boson cannot have the mass in the range between 160 and 170 at a &#13;
probability of 95%. &#13;
In addition, the mass of the W boson has been measured in the D0 experiment with record accuracy: &#13;
80,401&amp;nbsp;&amp;plusmn;&amp;nbsp;0,044&amp;nbsp;GeV. Improved accuracy of measuring the W boson mass may help in Higgs searches &#13;
by improving the knowledge of boundaries of possible mass ranges and the accuracy in calculations &#13;
of reactions involving the Higgs boson.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0903.4001"&gt;http://arxiv.org/abs/0903.4001&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/4/#1</link>
      <guid>http://ufn.ru/en/news/2009/4/#1</guid>
      <pubDate>Tue, 31 Mar 2009 20:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Increasing the luminescence efficiency of carbon nanotubes</title>
      <description>F.&amp;nbsp;Papadimitrakopoulos and his coworkers at the University of Connecticut found a way to enhance the &#13;
luminescence efficiency of single-wall carbon nanotubes up to a record-high level of 20%. &#13;
The luminance of nanotubes is limited by defects on their surface, such as absorbed oxygen &#13;
molecules. Earlier attempts of suspending nanotubes in solutions produced luminescence efficiency of &#13;
at most 0.5%. &#13;
In the new experiment nanotubes were coated with a layer of a compound FC12 — an analog of flavin &#13;
mononucleotide (its composition is not very different from that of vitamin B). As this coating was &#13;
added, FC12 molecules self-organized themselves into a tube coaxial with the carbon nanotube; this &#13;
process automatically removed extraneous molecules from the nanotube surface. The luminescent glow &#13;
of nanotubes is caused by irradiating them with IR light or by electric excitation. Carbon nanotubes &#13;
with high-efficiency luminescence may lead to numerous useful applications, e.g. in nanoscale &#13;
photodetectors and in biological sensors.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1166265"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;323&lt;/b&gt; 1319 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/4/#2</link>
      <guid>http://ufn.ru/en/news/2009/4/#2</guid>
      <pubDate>Tue, 31 Mar 2009 20:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Cooling of nanotubes</title>
      <description>P.&amp;nbsp;Avouris and colleagues at the IBM Research Center and researchers at Duke University (USA) &#13;
discovered that heat can be dissipated from carbon nanotubes into the substrate in contact with it &#13;
even if no chemical bonding exists between the two. The experiment was conducted with nanotubes on &#13;
silicon oxide substrate in a configuration resembling that of the field transistor. Thermal &#13;
vibrations were recorded by Raman spectroscopy techniques. Heat transfer from nanotubes is caused by &#13;
electric interaction between charges: electrons in a nanotube interact with charges induced by &#13;
electric fields of the substrate, energy is transferred to substrate charges close to its surface, &#13;
and thermal vibrations then travel deeper into the specimen. This effect is important for solving &#13;
the problem of cooling of microelectronic devices based on using carbon nanotubes.&#13;
&#13;
Source: &lt;a href="http://physicsworld.com/cws/article/news/38051"&gt;physicsworld.com&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/4/#3</link>
      <guid>http://ufn.ru/en/news/2009/4/#3</guid>
      <pubDate>Tue, 31 Mar 2009 20:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Stochastic resonance in digital electronics</title>
      <description>W.&amp;nbsp;Ditto (Arizona University) and his colleagues have discovered that the work of a logic &#13;
gate can be stabilized by a certain level of stochastic noise. Noise typically constitutes &#13;
a disruptive factor for the functioning of electronic devices, for instance, it may cause &#13;
unpredictable switching of the state in logic elements. In fact, stochastic resonance &#13;
emerges in some nonlinear systems so that it becomes possible to separate the useful &#13;
signal  by increasing the level of broadband noise because then the sum of signal and &#13;
noise exceeds a certain threshold value (on stochastic resonance see &lt;a href="http://ufn.ru/en/articles/1999/1/d/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;42&lt;/b&gt; 37 (1999) &lt;/a&gt;&#13;
and &lt;a href="http://ufn.ru/en/articles/2009/3/c/"&gt;&lt;i&gt;Uspekhi. fiz. nauk&lt;/i&gt; &lt;b&gt;179&lt;/b&gt; 266 (2009) (in Russian) &lt;/a&gt;). Stochastic resonance manifests itself, for example, in the case of &#13;
alternating climate cycles and in neuron systems. Arizona State University researchers &#13;
mathematically modeled a logic gate with two rectangular signals plus a noise signal fed in &#13;
as input; they found that as noise level increases the logic gate begins to function &#13;
predictably and this stability survives in a sufficiently broad range of noise amplitudes. &#13;
The theoretical predictions were supported by the study of an electronic analog of the &#13;
nonlinear system in question. Another useful property of the designed logic gate was the &#13;
possibility of reversing its logic by sending a control signal.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.102.104101"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;102&lt;/b&gt; 104101 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/4/#4</link>
      <guid>http://ufn.ru/en/news/2009/4/#4</guid>
      <pubDate>Tue, 31 Mar 2009 20:00:04 GMT</pubDate>
    </item>
    <item>
      <title>X-ray observations of the pulsar PSR J0108-1431</title>
      <description>The space X-ray observatory Chandra detected the oldest of the currently known isolated pulsars &#13;
(those not in binary systems) emitting in the X-ray range. Radio observations established that the &#13;
pulsar PSR&amp;nbsp;J0108-1431 is about 170 million years old. The unexpected result was the very high &#13;
luminosity of the pulsar despite its old age and slow rotation rate (at a period of about 0.8&amp;nbsp;s). &#13;
Approximately 0.4%&#13;
of energy connected with the slowdown is transformed into X-ray radiation. The pulsar &#13;
PSR&amp;nbsp;J0108-1431 &#13;
lies at a diatance of 770 light years and moves at a speed of about &#13;
200&amp;nbsp;km&amp;nbsp;s&lt;sup&gt;-1&lt;/sup&gt;. What continues &#13;
to remain unclear is the mechanism of X-ray emission. It is possible that two components are &#13;
present in the radiation, one generated in the magnetosphere of the pulsar and the other close to &#13;
the pulsar poles.&#13;
&#13;
Sources: &lt;a href="http://arxiv.org/abs/0803.0761"&gt;http://arxiv.org/abs/0803.0761&lt;/a&gt;,&#13;
&lt;a href="http://chandra.harvard.edu/press/09_releases/press_022609.html"&gt;http://chandra.harvard.edu/press/09_releases/press_022609.html&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/4/#5</link>
      <guid>http://ufn.ru/en/news/2009/4/#5</guid>
      <pubDate>Tue, 31 Mar 2009 20:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Dark matter in dwarf galaxies</title>
      <description>The Hubble Space telescope was used to study 29 dwarf galaxies in the core of the Perseus &#13;
galaxy cluster lying at a distance of 250 million light years from the Earth. In contrast to &#13;
the neightbouring spiral galaxies, dwarf galaxies have smooth regular shape without &#13;
visible signs of decay caused by tidal gravitational forces exerted by the cluster core and other &#13;
galaxies. This is an indication that the dwarf galaxy masses are sufficiently large to resist tidal &#13;
destruction. This invisible mass is that of dark matter (hidden mass). The mass-to-luminance ratio &#13;
of the investigated dwarf galaxies reaches &amp;asymp;120 solar units. It has thus been established &#13;
that dwarf galaxies of elliptic galaxies in cluster cores as well as dwarf spheroidals of the &#13;
Local group of galaxies contain a relatively high amount of dark matter.&#13;
&#13;
Sources: &lt;a href="http://arxiv.org/abs/0811.3197 "&gt;http://arxiv.org/abs/0811.3197 &lt;/a&gt;, &lt;a href="http://hubblesite.org/newscenter/archive/releases/2009/11/full/ "&gt;http://hubblesite.org/newscenter/archive/releases/2009/11/full/ &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/4/#6</link>
      <guid>http://ufn.ru/en/news/2009/4/#6</guid>
      <pubDate>Tue, 31 Mar 2009 20:00:06 GMT</pubDate>
    </item>
    <item>
      <title>Conductivity of graphene</title>
      <description>In the experiments carried out so far the conductivity of graphene (one-atom thick carbon &#13;
layer) was measured on a substrate and no data was available on graphene conductivity in &#13;
vacuum, that is, when the structure of graphene is not disturbed by the influence of &#13;
substrate charges (see e.g. &lt;a href="http://ufn.ru/en/articles/2008/7/h/"&gt;&lt;i&gt;Phys. Usp.&lt;/i&gt; &lt;b&gt;51&lt;/b&gt; 744 (2008) &lt;/a&gt;). Theoretical investigation of this &#13;
characteristic is not easy since the effective electrodynamic coupling constant &amp;alpha;&lt;sub&gt;g&lt;/sub&gt; &#13;
in graphene is approximately 300 times greater than the fine structure constant &amp;alpha;&amp;nbsp;=&amp;nbsp;1/137, so perturbations theory cannot be used. J.E.&amp;nbsp;Drut and Т.А.&amp;nbsp;Lahde developed a new theoretical approach for calculating electron properties of graphene. They applied a &#13;
numerical “lattice” computation technique resembling methods used in quantum &#13;
chromodynamics where the coupling constant is also large. Computations revealed how the &#13;
energy gap in the graphene electron spectrum changes depending on where graphene is &#13;
placed. It was shown that conductivity is affected by the coupling constant &amp;alpha;&lt;sub&gt;g&lt;/sub&gt;. &#13;
For graphene on SiO&lt;sub&gt;2&lt;/sub&gt; substrate the authors obtained &amp;alpha;&lt;sub&gt;g&lt;/sub&gt;&amp;nbsp;&amp;asymp;&amp;nbsp;0.79 so graphene &#13;
is conducting. As &amp;alpha;&lt;sub&gt;g&lt;/sub&gt; increases beyond the critical value &amp;alpha;&lt;sub&gt;g&lt;/sub&gt;&lt;sup&gt;cr&lt;/sup&gt;&amp;nbsp;=&amp;nbsp;1.11&amp;nbsp;&amp;plusmn;&amp;nbsp;0.06, graphene turns into insulator. For instance, in vacuum &amp;alpha;&lt;sub&gt;g&lt;/sub&gt;&amp;nbsp;&amp;asymp;&amp;nbsp;2.16 and &#13;
graphene is insulator. The validity of the formulated theoretical predictions can be &#13;
tested in future experiments.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.102.026802"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;102&lt;/b&gt; 026802 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/3/#1</link>
      <guid>http://ufn.ru/en/news/2009/3/#1</guid>
      <pubDate>Sat, 28 Feb 2009 21:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Type-1.5 superconductors</title>
      <description>V.V.&amp;nbsp;Moshchalkov and his colleagues in Belgium and Switzerland confirmed experimentally &#13;
that the two-component superconductor MgB&lt;sub&gt;2&lt;/sub&gt; possesses superconducting properties of both &#13;
type-1 and type-2 and consequently proposed to refer to it as superconductor of &#13;
intermediate type-1.5. They studied the spatial distribution of superconducting vortices &#13;
in a single crystal of MgB&lt;sub&gt;2&lt;/sub&gt; as it was cooled and went into superconducting state in external &#13;
magnetic field perpendicular to the specimen surface. It was found that vortices are not &#13;
uniformly spread but form denser patterns of spider web or ribbon-like shape. This implies &#13;
that at small distances vortices repel one another like they do in type-2 superconductors &#13;
but attract one another at larger distances like they do in type-1 superconductors. This &#13;
phenomenon is theoretically explained in terms of two weakly coupled order parameters in &#13;
superconducting MgB&lt;sub&gt;2&lt;/sub&gt; so that MgB&lt;sub&gt;2&lt;/sub&gt; manifests a combination of the properties of two &#13;
superconductors with different ratios &amp;xi;/&amp;lambda; (coherence length to penetration &#13;
length) typical of type-1 and type-2 superconductors. Measurement results are in good &#13;
agreement with the predictions of numerical modeling of vortex dynamics and calculations &#13;
in terms of the Ginzburg&amp;nbsp;&amp;ndash;&amp;nbsp;Landau two-component theory.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0902.0997"&gt;http://arxiv.org/abs/0902.0997&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/3/#2</link>
      <guid>http://ufn.ru/en/news/2009/3/#2</guid>
      <pubDate>Sat, 28 Feb 2009 21:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Entangled state of mechanical oscillators</title>
      <description>J.D.&amp;nbsp;Jost and his colleagues at the US National Institute of Standards and Technology &#13;
(NIST) for the first time entangled two mechanical systems — two oscillators consisting &#13;
of pairs of ions &lt;sup&gt;9&lt;/sup&gt;Be&lt;sup&gt;+&lt;/sup&gt;—&lt;sup&gt;24&lt;/sup&gt;Mg&lt;sup&gt;+&lt;/sup&gt; in a potential well. First all four ions were &#13;
trapped into a potential well in which the internal degrees of freedom of two &lt;sup&gt;9&lt;/sup&gt;Be&lt;sup&gt;+&lt;/sup&gt; &#13;
ions got entangled. Then two laser beams were used to modify the shape of the potential &#13;
well and the ions were separated into two pairs of &lt;sup&gt;9&lt;/sup&gt;Be&lt;sup&gt;+&lt;/sup&gt;—&lt;sup&gt;24&lt;/sup&gt;Mg&lt;sup&gt;+&lt;/sup&gt; of size &#13;
&amp;asymp;4&amp;nbsp;&amp;micro;m the separation between the pairs was 0.24&amp;nbsp;mm. These pairs of ions resemble &#13;
macroscopic springs with weights at their ends. Laser pulses forced the internal state of &#13;
entanglement in each pair to transfer to the mechanical oscillations of ions in the pair &#13;
relative to one another. This resulted in the formation of two pairs of ions entangled &#13;
over mechanical oscillational degrees of freedom.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0901.4779v1"&gt;http://arxiv.org/abs/0901.4779v1&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/3/#3</link>
      <guid>http://ufn.ru/en/news/2009/3/#3</guid>
      <pubDate>Sat, 28 Feb 2009 21:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Powerful gamma-ray burst</title>
      <description>NASA's Fermi Gamma-ray Space Telescope recorded a space gamma-ray burst of extraordinary &#13;
power, designated GRB&amp;nbsp;080916С. The optical afterglow of the burst was observed with the &#13;
GROND detector of the 2.2&amp;nbsp;m telescope, as well as with other telescopes. The source of the &#13;
burst was probably a supernova explosion in a remote galaxy with red shift of &lt;i&gt;z&amp;nbsp;=&amp;nbsp;4.35&amp;nbsp;&amp;plusmn;&amp;nbsp;0.15&lt;/i&gt;; consequently, GRB&amp;nbsp;080916С belongs to the 5% &#13;
of the remotest recorded gamma-ray bursts. It is assumed that violent energy releases &#13;
resulting in gamma-ray bursts take the form of narrow jets. It was established from the &#13;
variability of gamma emission that the Lorentz factor of a burst exceeds 1090. If we &#13;
assume for the sake of comparison that the emission is isotropic, the energy released in &#13;
the explosion comes to 6.5&amp;nbsp;&amp;times;&amp;nbsp;10&lt;sup&gt;54&lt;/sup&gt;&amp;nbsp;erg, or roughly 9000 times the energy of &#13;
ordinary supernovas. This allows classifying the gamma-ray burst GRB&amp;nbsp;080916С to have &#13;
record-high energy. As observed with some other bursts, high energy photons arrive with &#13;
certain time delay relative to photons from the low energy part of the spectrum. This may &#13;
indicate that emission from different parts of the spectrum is generated in different &#13;
conditions at different stages of the explosion, or in different regions of the jet-carried ejecta.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0902.0761"&gt;http://arxiv.org/abs/0902.0761&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/3/#4</link>
      <guid>http://ufn.ru/en/news/2009/3/#4</guid>
      <pubDate>Sat, 28 Feb 2009 21:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Coherence of electrons in photosynthesis</title>
      <description>It was earlier assumed that the energy transfer between electrons of different molecules in protein &#13;
complexes responsible for photosynthesis proceeds classically (via Coulomb collisions). However, &#13;
data were obtained in 2007 that electrons in protein molecules are quantum-coherent, so energy is &#13;
transferred by a wave mechanism. The 2007 experiment required prolonged irradiation of molecules by &#13;
laser light which resulted in their degradation and destruction; furthermore, the spectra could be &#13;
obtained only at select points of protein complexes. I.&amp;nbsp;Mercer (of University College Dublin, &#13;
Ireland) and his colleagues in Great Britain worked out a new and perfected technique which made it &#13;
possible to clarify details of energy transfer in photosynthesis. By using irradiation with a train &#13;
of short  laser pulses with different wavelengths Mercer et al obtained a two-dimensional spectrum &#13;
of protein complexes and were able to build a spatio-temporal picture of the processes. Thus the new &#13;
experiment has confirmed that electrons transfer energy in a coherent manner.&#13;
&#13;
Sources: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.102.057402"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;102&lt;/b&gt; 057402 (2009) &lt;/a&gt;; &lt;a href="http://focus.aps.org/story/v23/st5"&gt;http://focus.aps.org/story/v23/st5&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/3/#5</link>
      <guid>http://ufn.ru/en/news/2009/3/#5</guid>
      <pubDate>Sat, 28 Feb 2009 21:00:05 GMT</pubDate>
    </item>
    <item>
      <title>Casimir&amp;nbsp;&amp;ndash;&amp;nbsp;Lifshitz force in repulsion mode</title>
      <description>In 1961 E.M.&amp;nbsp;Lifshitz, I.Ye.&amp;nbsp;Dzyaloshinskii and L.P.&amp;nbsp;Pitaevskii, &lt;i&gt;Adv.&amp;nbsp;Phys.&lt;/i&gt; &lt;b&gt;10&lt;/b&gt; 165 (1961) &#13;
(see also &lt;a href="http://ufn.ru/ru/articles/1961/3/b/"&gt;&lt;i&gt;Uspekhi. fiz. nauk&lt;/i&gt; &lt;b&gt;73&lt;/b&gt; 381 (1961) (in russian) &lt;/a&gt;) formulated the conditions at which the Casimir&amp;nbsp;&amp;ndash;&amp;nbsp;Lifshitz &#13;
force between two plates becomes repulsive: it is necessary that the dielectric &#13;
permittivity of the intermediate dielectric layer be lower than that of one of the plates &#13;
but higher than that of the other. The Casimir&amp;nbsp;&amp;ndash;&amp;nbsp;Lifshitz force in repulsion mode was &#13;
measured in a number of experiments but only at distances not larger than several nm where &#13;
the Casimir effect works in the Van der Waals mode and the contribution of intermolecular &#13;
forces is large. F.&amp;nbsp;Capasso, J.&amp;nbsp;Munday and A.&amp;nbsp;Parsegian were the first to conduct detailed &#13;
measurements of the Casimir&amp;nbsp;&amp;ndash;&amp;nbsp;Lifshitz force at distances from 20 to 300&amp;nbsp;nm in which the &#13;
effect of repulsion stemming from the distortion of the spectrum of zero quantum &#13;
oscillations is directly measurable. They observed the interaction between a sphere &#13;
40&amp;nbsp;&amp;micro;m in diameter coated with a thing gold layer and a quatz plate in liquid &#13;
bromobenzene. Using a small sphere instead of the second plate proved to be very &#13;
convenient as this removed the need in the complicated procedure of setting the plates &#13;
parallel to one another at a small separating distance. Moreover, this method allows &#13;
determining the force from the velocity of the sphere, and determining this velocity by &#13;
measuring the displacement of the beam of light reflected from the sphere. Preliminary calibration &#13;
was carried out far from the quartz plate (where the Casimir effect is very low): various velocities &#13;
of motion through the liquid were put in correspondence with hydrodynamic forces. The measured force &#13;
of repulsion of the sphere from the plate was in good agreement with calculations in terms of the &#13;
Lifshitz&amp;nbsp;&amp;ndash;&amp;nbsp;Dzyaloshinskii&amp;nbsp;&amp;ndash;&amp;nbsp;Pitaevskii theory. The quartz plate was replaced in the control experiment &#13;
with a gold plate; as was expected, in this case the sphere was attracted to the plate.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nature07610"&gt;&lt;i&gt;Nature&lt;/i&gt; &lt;b&gt;457&lt;/b&gt; 170 (2009) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/2/#1</link>
      <guid>http://ufn.ru/en/news/2009/2/#1</guid>
      <pubDate>Sat, 31 Jan 2009 21:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Symmetry of energy gap in Ba&lt;sub&gt;0.6&lt;/sub&gt;K&lt;sub&gt;0.4&lt;/sub&gt;Fe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt;</title>
      <description>Experiments show that the energy gap in high-temperature cuprate superconductors (the &#13;
bonding energy of a Cooper pair) has different signs on different regions of the Fermi &#13;
surface. Angle-resolved photoelectron spectroscopy has not confirmed the existence of a &#13;
similar asymmetry of the energy gap in iron-based superconductors such as &#13;
Ba&lt;sub&gt;0.6&lt;/sub&gt;K&lt;sub&gt;0.4&lt;/sub&gt;Fe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt;. In fact, however, these superconductors cannot be &#13;
described in terms of the Bardeen&amp;nbsp;&amp;ndash;&amp;nbsp;Cooper&amp;nbsp;&amp;ndash;&amp;nbsp;Schrieffer theory in which the gap is assumed to &#13;
be symmetrical. A hypothesis was advanced that the result is negative because the &#13;
spectroscopic techniques used to study these materials are not sensitive to the phase of &#13;
the wave function of electrons that carries the symmetry information. A.D.&amp;nbsp;Christianson &#13;
and his colleagues conducted new studies of the energy gap in Ba&lt;sub&gt;0.6&lt;/sub&gt;K&lt;sub&gt;0.4&lt;/sub&gt;Fe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt; by &#13;
using inelastic neutron scattering which makes it possible to measure the phase. The characteristic &#13;
effect on the magnetic moments of neutrons established that the symmetry of the gap in &#13;
Ba&lt;sub&gt;0.6&lt;/sub&gt;K&lt;sub&gt;0.4&lt;/sub&gt;Fe&lt;sub&gt;2&lt;/sub&gt;As&lt;sub&gt;2&lt;/sub&gt; differs from the d-symmetry in cuprate superconductors and is most &#13;
likely of the type s&amp;plusmn; in which case electrons split into groups with the opposite phase of the &#13;
wave function. In this case the pairing of electrons is created through antiferromagnetic &#13;
fluctuations.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1038/nature07625"&gt;&lt;i&gt;Nature&lt;/i&gt; &lt;b&gt;456&lt;/b&gt; 930 (2008) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/2/#2</link>
      <guid>http://ufn.ru/en/news/2009/2/#2</guid>
      <pubDate>Sat, 31 Jan 2009 21:00:02 GMT</pubDate>
    </item>
    <item>
      <title>Stability of coherence of laser light</title>
      <description>М.&amp;nbsp;Bellini (University of Florence, Italy) and his coworkers confirmed a theoretical &#13;
prediction of R. Glauber (1963) stating that removal of individual photons from a laser &#13;
beam leaves the beam in coherent quantum state. A laser beam was passed through two &#13;
optical splitters. The first splitter split the beam in two and their interference gave &#13;
the measure of the degree of coherence. One of these beams was sent through the second &#13;
splitter with very little splitting efficiency which allowed the authors to single out individual &#13;
photons from this beam. These photons were recorded by a detector that could be triggered &#13;
by single photons. In accord with R.&amp;nbsp;Glauber's theoretical prediction it was found that &#13;
extraction of individual photons did not destroy the coherence of the laser beam. &#13;
Furthermore, М.&amp;nbsp;Bellini and his coworkers developed a technique for adding single photons &#13;
to a beam; in this manner they confirmed that the operations of extracting and injecting &#13;
of photons are noncommutive.&#13;
&#13;
Source: &lt;a href="http://physicsworld.com/cws/article/news/37106"&gt;http://physicsworld.com/cws/article/news/37106&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/2/#3</link>
      <guid>http://ufn.ru/en/news/2009/2/#3</guid>
      <pubDate>Sat, 31 Jan 2009 21:00:03 GMT</pubDate>
    </item>
    <item>
      <title>Quantum cascade laser</title>
      <description>K.J.&amp;nbsp;Franz (Princeton University) and his colleagues were the first to discover in 2007 &#13;
that the quantum cascade laser they built generated, in addition to the "normal" beam, a &#13;
laser beam at the second frequency but of lower power (see &lt;i&gt;Appl. Phys. Lett.&lt;/i&gt; &lt;b&gt;90&lt;/b&gt;, 091104 (2007)). The lasing area of the laser in question consists of tens of layers of various &#13;
semiconductors, each only a few atomic layers thick. Later the same team of researchers obtained &#13;
further interesting results. It was found that the radiations at the two frequencies are in &#13;
anticorrelation which is caused by a "competition" for charge carriers that can take part in the &#13;
radiation at both the principal and the second frequency: as temperature increases, the output &#13;
power of the second beam grows while that of the first one decreases. A possible explanation of the &#13;
discovered effect was also suggested. It is assumed that the second beam is generated by electrons &#13;
with momenta &lt;i&gt;k&amp;nbsp;=&amp;nbsp;p&amp;nbsp;/&amp;nbsp;$\hbar$  &amp;nbsp;&amp;asymp;&amp;nbsp;3.6&amp;nbsp;&amp;times;&amp;nbsp;10&lt;sup&gt;8&lt;/sup&gt;&amp;nbsp;m&lt;sup&gt;-1&lt;/sup&gt;&lt;/i&gt; in nonequilibrium states while &#13;
quasi-nonequilibrium electrons with zero momenta are responsible for the first beam. Lasers emitting &#13;
via the new mechanism may find useful practical applications. The nearest task facing the &#13;
researchers is to suppress the emission of the laser beam at the principal frequency so as to &#13;
achieve emission of the second type only. &#13;
&#13;
Sources: &lt;a href="http://dx.doi.org/10.1038/nphoton.2008.250"&gt;&lt;i&gt;Nature Photonics&lt;/i&gt; &lt;b&gt;3&lt;/b&gt; 930 (2008)&lt;/a&gt;; &lt;a href="http://engineering.princeton.edu/news/laser_08"&gt;http://engineering.princeton.edu/news/laser_08&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/2/#4</link>
      <guid>http://ufn.ru/en/news/2009/2/#4</guid>
      <pubDate>Sat, 31 Jan 2009 21:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Fast-moving stars</title>
      <description>A group of astronomers led by R.&amp;nbsp;Sahai using NASA's Hubble Space Telescope  found 14 young &#13;
stars moving at huge velocities through the interstellar gas and creating a bow shock &#13;
&amp;asymp;10&lt;sup&gt;11&lt;/sup&gt;-10&lt;sup&gt;12&lt;/sup&gt;&amp;nbsp;km in size, leaving behind a trace of glowing gas. The &#13;
shock wave is produced by the collision of the powerful stellar wind with the surrounding &#13;
gas. The stars were found to be fairly young — not older than a million years or so — &#13;
and have masses not more than eight time the solar mass. Hubble's observations yielded the &#13;
shape and structure of shock waves. The stars move at about 180000&amp;nbsp;km&amp;nbsp;h&lt;sup&gt;-1&lt;/sup&gt;, which is &#13;
roughly five times higher than the characteristic velocities of ordinary young stars. It &#13;
is assumed that these stars get such high velocities from slingshot ejection out of a stellar &#13;
cluster in a close flyby, or from gravitational interaction between two binary stars or a &#13;
binary and a single star, or when the second component of a pair exploded as a supernova. Such &#13;
fast-moving stars were first detected by the IRAS telescope at the end of the 1980s; however, the stars observed then by the IRAS were considerably more massive.&#13;
&#13;
Source: &lt;a href="http://hubblesite.org/newscenter/archive/releases/2009/03/full/"&gt;http://hubblesite.org/newscenter/archive/releases/2009/03/full/&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/2/#5</link>
      <guid>http://ufn.ru/en/news/2009/2/#5</guid>
      <pubDate>Sat, 31 Jan 2009 21:00:05 GMT</pubDate>
    </item>
    <item>
      <title>New measurements of the fine structure constant</title>
      <description>Using a combined method based on the Bloch oscillations effect and atom interferometry, &#13;
М.&amp;nbsp;Cadoret and his coworkers in France were able to measure the fine structure constant with &#13;
a relative accuracy of 4,6&amp;times;10&lt;sup&gt;-9&lt;/sup&gt;. Other recent superhigh-precision experiments &#13;
for &amp;alpha; directly measured only the the anomalous magnetic moment of the electron &#13;
after which &amp;alpha; was calculated using the formulas of quantum electrodynamics. In the &#13;
experiment of М.&amp;nbsp;Cadoret and his colleagues, measurements of &amp;alpha; were more direct &#13;
(did not need the assumption of validity of QED formulas) as they used recoil pulses from atoms in &#13;
periodic potential. Rubidium atoms were illuminated by two oppositely directed laser beams with &#13;
slightly different frequencies; atoms absorbed photons from one beam and then re-emitted them into &#13;
the other beam. The frequency difference was compensated for by the Doppler effect on moving atoms, &#13;
and its measurement yielded the value of &amp;alpha;. The agreement with the results obtained in other &#13;
experiments and with theoretical QED achieved the test of this theory at currently the highest &#13;
accuracy. &#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0810.3152v1"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;101&lt;/b&gt; 230801 (2008) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/1/#1</link>
      <guid>http://ufn.ru/en/news/2009/1/#1</guid>
      <pubDate>Wed, 31 Dec 2008 21:00:01 GMT</pubDate>
    </item>
    <item>
      <title>Light pulse in optical filament</title>
      <description>The controversy concerning the momentum of light in a transparent medium remains the object of debate &#13;
for nearly a hundred years. The problem of choosing between the expressions given by &#13;
H.&amp;nbsp;Minkowski and M.&amp;nbsp;Abraham lies in the ambiguity of dividing the total momentum into that of &#13;
the field and that of the medium, and in the need to take into account the action exerted &#13;
by the electromagnetic field on the medium when light is emitted or absorbed (see &lt;a href="http://ufn.ru/ru/articles/1976/1/e/"&gt;&lt;i&gt;Uspekhi Fiz. Nauk&lt;/i&gt; &lt;b&gt;118&lt;/b&gt; 175 (1976)&lt;/a&gt; (in Russian)). Chinese researchers W.&amp;nbsp;She, J.&amp;nbsp;Yu и R.&amp;nbsp;Feng carried out a new experiment which &#13;
confirmed Abraham's expression. Optical filament 1.5 mm in length and half a micron in &#13;
diameter was suspended vertically in a hermetically sealed vessel. Light from two lasers &#13;
was sent downward through the filament. The first laser, at wavelength 650&amp;nbsp;nm and power &#13;
output 0.5&amp;nbsp;mW served to illuminate the fiber and facilitate observing its motion which was &#13;
photographed 10&amp;nbsp;times/min through a lens installed in the wall of the vessel. When a &#13;
light pulse from the second laser at wavelength 980&amp;nbsp;nm and variable power output of 0 to &#13;
79&amp;nbsp;mW emerged from the lower end of the filament, it imparted to it a momentum and the &#13;
upward-directed recoil caused filament bending. This behavior confirmed Abraham's &#13;
expression for momentum: if Minkowski's approach were correct, there would be a downward &#13;
stretching load on the filament. The experiment was successful owing to the small weight &#13;
of the filament: the recoil momentum compensated for the weight of the free end segment of the &#13;
filament. The experiment confirmed the theoretical evaluation which predicted this &#13;
compensation to occur at laser power output of about 4&amp;nbsp;mW. A not very different result was &#13;
observed when the second laser worked in continuous, not pulsed, mode.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0806.2442"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;101&lt;/b&gt; 243601 (2008) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/1/#2</link>
      <guid>http://ufn.ru/en/news/2009/1/#2</guid>
      <pubDate>Wed, 31 Dec 2008 21:00:02 GMT</pubDate>
    </item>
    <item>
      <title>The Magnus effect for light</title>
      <description>Е.&amp;nbsp;Hasman and his colleagues at the Technion-Israel Institute of Technology have been the &#13;
first to observe in the adiabatic mode the spin Hall effect for photons, also known as the &#13;
optical Magnus effect. This effect was observed earlier but only in the nonadiabatic case of &#13;
strong nonuniformity when a particle's trajectory is stopped abruptly. The spin Hall &#13;
effect for photons consists in the interaction between the spin of a particle and the &#13;
curvature of its trajectory, resulting in an additional force affecting the trajectory of &#13;
motion. Hasman et al studied propagation of laser light along a glass cylinder. The beam &#13;
went through total internal reflections and its trajectory was twisted into a helix along &#13;
the surface. Measured at the exit face of the cylinder were the beam direction and &#13;
the Stokes parameters. The experiment carried out in the Technion confirmed the detailed &#13;
theory of the optical Magnus effect, based on the dynamic effect of the geometric Berry &#13;
phase.&#13;
&#13;
Source: &lt;a href="http://arxiv.org/abs/0810.2136"&gt;&lt;i&gt;Nature Photonics&lt;/i&gt; &lt;b&gt;2&lt;/b&gt; 748 (2008) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/1/#3</link>
      <guid>http://ufn.ru/en/news/2009/1/#3</guid>
      <pubDate>Wed, 31 Dec 2008 21:00:03 GMT</pubDate>
    </item>
    <item>
      <title>The Lamb shift in solids</title>
      <description>The Lamb shift of atomic energy levels stems from the interaction between electrons and &#13;
virtual electron-positron pairs created in the vacuum. Typically it is not possible to &#13;
observe the Lamb shift in solids since energy levels in them form broad bands. However, &#13;
A.&amp;nbsp;Wallraff and his coworkers from Switzerland and Canada were able to measure the Lamb &#13;
shift of the microscopic quantum bit (qubit) in a resonator. The qubit consisted of two &#13;
tiny pieces of superconductor connected by two tunnel junctions. This system is known as transmon. &#13;
The energy levels of the transmon are dictated by the distribution of Cooper pairs in &#13;
superconductors. A transmon was placed in a microwave resonator where it could absorb and emit &#13;
photons of certain frequencies. By virtue of its shape, the transmon possessed a large dipole &#13;
moment; also, a special resonator configuration was chosen so as to enhance the effect of &#13;
interaction with virtual photons. The Stark effect contributed only negligible corrections because &#13;
it it was felt only outside the area of resonance with virtual photons. As a result, the observed &#13;
Lamb shift of transmon's energy levels was approximately 1.4% &#13;
of the energy difference between the neighboring levels, which is 10,000 times greater &#13;
than the Lamb shift in the hydrogen atom outside the resonator. The Lamb shift results in &#13;
decoherence of the qubit state. The experiment conducted by A.&amp;nbsp;Wallraff and his colleagues &#13;
provides a recipe for avoiding undesirable decoherence in future quantum computers: choose &#13;
device configurations that are not in resonance with virtual photons.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1126/science.1164482"&gt;&lt;i&gt;Science&lt;/i&gt; &lt;b&gt;322&lt;/b&gt; 1357 (2008) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/1/#4</link>
      <guid>http://ufn.ru/en/news/2009/1/#4</guid>
      <pubDate>Wed, 31 Dec 2008 21:00:04 GMT</pubDate>
    </item>
    <item>
      <title>Stimulated emission of surface plasmon polaritons</title>
      <description>Surface plasmons and plasmon polaritons constitute electromagnetic pulses in the electron &#13;
gas, localized or moving along the metal-dielectric interface, respectively. These &#13;
quasiparticles are strongly absorbed in the range of optical frequencies and have short &#13;
propagation length, which create problems for possible practical applications. It was &#13;
suggested that the problem may be solved by using optically active impurities. &#13;
М.А.&amp;nbsp;Noginov (Norfolk University, USA) and his coworkers were able for the first time to use &#13;
this technique and achieve both the compensation of losses of surface plasmon polaritons &#13;
and the observation of their stimulated emission which is similar to the stimulated &#13;
emission of photons in lasers. A 32 to 82&amp;nbsp;nm thick silver layer was  deposited onto a face &#13;
of a grass prism. The silver layer was coated with a polymer film doped with dye &#13;
molecules. Excitation of surface plasmon polaritons was produced by light pulses first on &#13;
the side of the prism (for the sake of calibration needed to measure the reflection &#13;
profile &lt;i&gt;R(&amp;theta;)&lt;/i&gt;) and then on the side of the polymer film. The dye molecules absorbed &#13;
photons and emitted surface plasmon polaritons. The threshold for polariton emission and &#13;
the spectrum of polaritons agreed with theoretical predictions for a laser-like radiation. &#13;
This experimental study may lead to useful applications in creating novel metamaterials &#13;
and plasmon nanodevices.&#13;
&#13;
Source: &lt;a href="http://dx.doi.org/10.1103/PhysRevLett.101.226806"&gt;&lt;i&gt;Phys. Rev. Lett.&lt;/i&gt; &lt;b&gt;101&lt;/b&gt; 226806 (2008) &lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/1/#5</link>
      <guid>http://ufn.ru/en/news/2009/1/#5</guid>
      <pubDate>Wed, 31 Dec 2008 21:00:05 GMT</pubDate>
    </item>
    <item>
      <title>A very hot white dwarf</title>
      <description>The space telescope FUSE detected a white dwarf KPD&amp;nbsp;0005+5106 with record-high surface &#13;
temperature of 200,000&amp;deg;С. At this temperature, and object is visible in the UV &#13;
range of spectrum. White dwarfs (their internal pressure is sustained by the degenerate &#13;
electron gas) evolve from massive stars after the thermonuclear fuel inside them is &#13;
exhausted. High temperatures can be produced only immediately after the white dwarf is &#13;
formed, before it starts to cool down, so the observation of a white dwarf with a &#13;
temperature of 200,000&amp;deg;С is a very rare event.&#13;
&#13;
Source: &lt;a href="http://www.space.com/scienceastronomy/081212-hot-star.html"&gt;http://www.space.com/scienceastronomy/081212-hot-star.html&lt;/a&gt;</description>
      <link>http://ufn.ru/en/news/2009/1/#6</link>
      <guid>http://ufn.ru/en/news/2009/1/#6</guid>
      <pubDate>Wed, 31 Dec 2008 21:00:06 GMT</pubDate>
    </item>
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