{"id":5676,"date":"2013-03-22T15:31:55","date_gmt":"2013-03-22T11:31:55","guid":{"rendered":"http:\/\/ellphi.lebedev.ru\/?p=5676"},"modified":"2013-04-05T15:03:34","modified_gmt":"2013-04-05T11:03:34","slug":"1979-en","status":"publish","type":"post","link":"http:\/\/preprints.lebedev.ru\/?p=5676","title":{"rendered":"1979 En"},"content":{"rendered":"<p><em> V.P. Frolov<\/em> ,    <em> E.M. Serebriany<\/em> ,<br \/>\n<strong> \u2116  2 <\/strong> QIUHTUU EFFECTS IN SYSTEMS WITH ACCELERATED MIRRORS<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-2.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id93396917'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id93396917\" style=\"display:none\">The problem of the vacuum state definition in a part of the Minkowski space bounded by the single or two spherically symmetric uniformly accelerated mirrors is considered. The Euclidean approach is need to get the explicit expressions for the corresponding causal Green&#8217;s functions. The vacuum stress-energy tensor is obtained and its properties are investigated.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> M.V. Fedorov<\/em> ,    <em> J.K. Moiver<\/em> ,<br \/>\n<strong> \u2116  19 <\/strong> THE QUANTUM THEORY OF STIMULATED PROCESSES IN THE FREE ELECTRON LASER IN THE REGION OF STRONG FIELD<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-19.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id1465465111'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id1465465111\" style=\"display:none\">The general quantum mechanical equations are derived for an electron in the fields of a spatially periodic magnet and a plane electromagnetic wave. The limits of applicability are found for calculations performed in lowest order perturbation theory. Approximate solutions to these equations are found for the cases of a weak electromagnetic wav and 31 strong eleotrc~magnetic wave. The gain coefficient calculated using the weak field solution is identical to the perturbation result but the limit of applicability includes a much larger region.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> A.D. Sakharov<\/em> ,<br \/>\n<strong> \u2116  28 <\/strong> Baryon asymmetry of the universe.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-28.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> A.D. Linde<\/em> ,<br \/>\n<strong> \u2116  38 <\/strong> \u0421LASSICAL YANG-MILIS COLUTIONS CONDENSATION OF, W MESONS AND SYMMETRY OF COMPOSITION OF SUPERDENSE MATTER<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-38.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id256951997'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id256951997\" style=\"display:none\">leads to the condensation of W mesons. Asaconsequence of this phase transition, densities of all types of right and left leptons (bar\u0443ons) in superdense matter become equal to each other.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> D.S. Chernavskii<\/em> ,    <em> R.I. Volkov<\/em> ,<br \/>\n<strong> \u2116  39 <\/strong> ON THE POSSIBILITY OF USING THE PROTEOLYTIC AND LEPOLYTIC ENZYMES IN THE THERAPY OF MALIGNANT DISEASES<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-39.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id1166412156'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id1166412156\" style=\"display:none\">The aim of this report is an investigation of  simple, qualitative consequencese of the membrane model of regulation of cell division [l]. It is shown that the differences in the structural organization of plasma membranes of normal and tumour rails aunt lead to the selective damages of tumour calls by proteolytic and lipolytio enzymes.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> A.L. Kalyazin<\/em> ,    <em> V.N. Sazonov<\/em> ,    <em> S.V. Zatsopin<\/em> ,<br \/>\n<strong> \u2116  47 <\/strong> A SELECTIVE ACTION OF LAGER RADTATION IN DENSE MEDIUM<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-47.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> S.I. Syrovatskii<\/em> ,    <em> V.D. Kuznetsov<\/em> ,<br \/>\n<strong> \u2116  52 <\/strong> On the possibility of radioobservations of current sheets on the sun.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-52.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> A.K. Kalashnikov<\/em> ,    <em> S.E. Konstein<\/em> ,<br \/>\n<strong> \u2116  67 <\/strong> HIERARCHY OF IHTERACTIONS AND MASS RELATIONS IN ASYMPTOTICALLY FREE E6 MODEL OF UNIFIED IN\u0422ER\u0410C\u0422ION<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-67.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> N.G. Basov<\/em> ,    <em> I.G. Zubarev<\/em> ,<br \/>\n<strong> \u2116  73 <\/strong> POWERFUL LASER SYSTEMS WITH PHASE CONJUGATION BY SMB3 MIRROR<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-73.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> V.V. Kornsev<\/em> ,    <em> V.V. Krutov<\/em> ,    <em> S.L. Mandelstam<\/em> ,    <em> B.. Sylwester<\/em> ,    <em> S.P. Tindo<\/em> ,    <em> A.N. Urniv<\/em> ,    <em> B.. Valichek<\/em> ,    <em> I.A. Zhitnik<\/em> ,<br \/>\n<strong> \u2116  76 <\/strong> SOLAR FLARE X-RAY SPECTRA FOR INITIAL AND FINAL PHASE<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-76.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> D.I. Khomskii<\/em> ,    <em> K.I. Kugel<\/em> ,<br \/>\n<strong> \u2116  79 <\/strong> Orbital degeneracy and some two-spin models.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-79.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> M.M. Chernyavsky<\/em> ,    <em> N.V. Maslennikova<\/em> ,    <em> G.I. Orlova<\/em> ,    <em> M.I. Tretyakova<\/em> ,<br \/>\n<strong> \u2116  81 <\/strong> Cluster production in pN-interaction at 400 gev.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-81.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> N.A. Bobrova<\/em> ,    <em> S.I. Syrevatskii<\/em> ,<br \/>\n<strong> \u2116  85 <\/strong> TR\u0410RING-MODE INSTABILITY OF ONE-DIMENSIONAL FORCE-FREE MAGNETIC FIELD<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-85.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id859826676'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id859826676\" style=\"display:none\">THE TEARING-CODE INSTABILITY OF ONE-DIMENTIONAL FCTCE-FREE AAGNETIO FIELD IS INVESTIGATED. THE DEPENDENCE OF THE GROWTH RATE ON WAVE NUNBER AND MAGNETIC REYNELDS NUMBER AND THE EXACT LIMIT OF INSTABILITY, WHICH TAKES INTO ACCOUNT THE DIFFERENCE IN PHASE OF THE PERTURBETTIOUS ON THE NEXT RESONANCE SURFACES, ARE FOUND. IT IS ALSO SHOWN THAT IN WEAKLY NONIDEAL SYSTEM (WHEN CONDUCTIVITY IS HIGH SMALL PERTURBATIONS.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> M.M. Chernyavsky<\/em> ,    <em> A.A. Komar<\/em> ,    <em> G.I. Orlova<\/em> ,    <em> N.A. Salmanova<\/em> ,    <em> M.I. Tretyakova<\/em> ,<br \/>\n<strong> \u2116  93 <\/strong> Productiob of short-lived particles in nuclear emulsion by -mesons at 200 gev\/c.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-93.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> M.V. Fedorov<\/em> ,    <em> J.K. McIver<\/em> ,<br \/>\n<strong> \u2116  99 <\/strong> THE CLASSICAL THE ORY OF SATURATION IN THE FREE-ELECTRON LASER<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-99.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id1746350156'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id1746350156\" style=\"display:none\">The classical equations of action for electron ia the free-electron laser are investigated for the case when the electromagnetic field can not be considered weak. Expressions are found for the emitted energy of the electron and the gain per pass of the laser. Those expressions are identical with those derived free the relativistic quantum mechanical equations.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> A.I. Nikishov<\/em> ,<br \/>\n<strong> \u2116  100 <\/strong> \u0421\u041e\u041d\u0415RENT EFFEKT OF BREMSSTRAHLUNG AMORPHOUS SOLIDS<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-100.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> A.I. Korotchenko<\/em> ,    <em> N.I. Popov<\/em> ,    <em> A.A. Samokhin<\/em> ,    <em> A.B. Uspensky<\/em> ,<br \/>\n<strong> \u2116  103 <\/strong> On the manifestation of spinodal singularities in radiation-induced vaporization of liquids.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-103.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> E.S. Fradkin<\/em> ,    <em> D.M. Gitman<\/em> ,<br \/>\n<strong> \u2116  106 <\/strong> Problems of quantum electrodynamics with intensive field.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-106.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> E.S. Fradkin<\/em> ,    <em> D.M. Gitman<\/em> ,<br \/>\n<strong> \u2116  107 <\/strong> Problem of quantum electrodynamiks with intensive field. (Appendix).<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-107.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id347859876'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id347859876\" style=\"display:none\">This paper in a continustion of the previous article with the same title. We present an extension of the Wick technique to the case of unstable vacuum, find various green functions in extermal field and also calculate cartein radiative effects in constant electris field.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> O.K. Kalashnikov<\/em> ,    <em> V.V. Klimov<\/em> ,<br \/>\n<strong> \u2116  117 <\/strong> Polarization tensor in QCD for finite temperature and density.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-117.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> M.V. Fedorov<\/em> ,    <em> J.K. McIver<\/em> ,<br \/>\n<strong> \u2116  129 <\/strong> MULTIPHOTON STIMULITED COMPTON SCATTERING<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-129.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id543113858'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id543113858\" style=\"display:none\">The processes of multiphoton Compton scattering of relativistic electrons are considered in a special one-dimensional geometry. The multiphoton parameter and the energy distribution of scattered electrons are found. The nonlinear behaviour of the gains of the two external electromagnetic waves is investigated in the saturation region. The multiphoton parameter is shown to be of order of one and the perturbation theory is shown to be inapplicable at very weak fields. For saturation of the gains much stronger fields are required which however are much weaker than those which are necessary for appearance of multiphoton processes in the spontaneous Coup ton scattering [I].<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> S.I. Syrovatskii<\/em> ,    <em> B.V. Somov<\/em> ,<br \/>\n<strong> \u2116  152 <\/strong> Physical driving forces and models of coronal responses.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-152.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> B.V. Somov<\/em> ,    <em> S.I. Syrovatskii<\/em> ,<br \/>\n<strong> \u2116  153 <\/strong> Magnetically drivenotions in solar corona.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-153.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id283807487'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id283807487\" style=\"display:none\">Abstract. Solution of the nonlinear MHD problem of plasma flow In an increasing dipolar magnetic field ia obtained in the approximation for a strong field. The distributions of plasma velocity, displacement, and density are oalculated. The situation when the magnetic dipole is &#8216;increased&#8217; by rapid process of magnetic reconnection or current aheet rupture is illustrated* Possible applications are diacussed in connection with plasma ejections from chromosphere in \u043eorone.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> E.S. Fradkin<\/em> ,<br \/>\n<strong> \u2116  174 <\/strong> QUANTZATION AND THE S-MATRIX IN GRAVITY AND SUPERGRAVITY. ASYMPTOTICAL FREEDOM.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-174.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> V.G. Gyrzadyan<\/em> ,    <em> L.M. Ozernoy<\/em> ,<br \/>\n<strong> \u2116  176 <\/strong> ACCRETI0N AND RADIATION S\u0420TECTRUM \u041eF THE GAS DEBRIS OF A STAR DISRUPTED BY TIDAL FORCES OF A MAS8IVE BLACK HOLE<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-176.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> L.N. Bulaevsky<\/em> ,    <em> A.I. Buzdin<\/em> ,    <em> M.. Kulic<\/em> ,<br \/>\n<strong> \u2116  184 <\/strong> HELICAL ORDER OP SPINS IN THE SUPERCONDUCTOR: SPIN-WAVE SPECTRUM, SPECIFIC HEAT AND SOUND ATTENUATION IN THE HELICAL SUPERCONDUCTING PHASE.<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-184.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id872680030'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id872680030\" style=\"display:none\">In the present work we consider theoretically the compounds where the superconducting phase with helical order of localized of magnetic moments exists down to zero temperature. In the systems under consideration namely the superconductivity causes the helical order i.e. without Cooper pairing we would observe the ferromagnetic order of localized spins. The low temperatures properties of superconducting helical phase (HS-phase) are investigated in the spin wave approximation. We show that mean field approximation describes well the HS-phase at low temperatures. We found the spin-wave spectrum and its contribution to the specific heat. The sound attenuztion in the HS-phase is calculated and we show that the absorption is sharply anisotropic and reaches its maximum value at the sounds propogation along the helical axis.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> V.V. Dodonov<\/em> ,    <em> E.V. Kurmyshev<\/em> ,    <em> V.I. Man&#8217;ko<\/em> ,<br \/>\n<strong> \u2116  187 <\/strong> HIGH ENERGY AND COSMIC RAYS PHYSICS<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-187.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> T.G. Listina<\/em> ,    <em> U.I. Safronova<\/em> ,    <em> A.S. Shlapzeva<\/em> ,<br \/>\n<strong> \u2116  201 <\/strong> ATOMIC CALCULATIONS USING PERTURBATION THEORY ON POWERS OF I\/2 FOR FOUR-ELECTRON SYSTEM<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-201.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <\/p>\n<p><em> A.P. Gus&#8217;kov<\/em> ,    <em> A.I. Korotchenko<\/em> ,    <em> A.A. Samokhin<\/em> ,<br \/>\n<strong> \u2116  203 <\/strong> RESPONSE OF RAPIDLY EVAPORATING LIQUIDS TO THEKMAL AND HYDRODYNAMIC PERTURBATIONS<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-203.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>  <a class=\"spoiler_link_show\" href=\"javascript:void(0)\" onclick=\"wpSpoilerToggle(document.getElementById('id208340746'), this, '|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|', '|\u0421\u043a\u0440\u044b\u0442\u044c \u0430\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044e|')\">|\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f|<\/a>\n<div class=\"spoiler_div\" id=\"id208340746\" style=\"display:none\">A linear response of the steady-state evaporation process Is investigated, for liquids absorbing intense radiation. Thermal and hydrodynamic perturbations are considered. In the ease of the thermal perturbation due to intensity modulation the vaporization pressure response shows a resonant behaviour with respect to the modulation frequency. The hydrodynamic (ripplonlike) perturbation results In differential vapour recoil which Plays an essential role in the stability problem of evaporating liquid surface.<br\/><br\/> ---------------------------<\/div>\n<\/p>\n<p><em> V.P. Frolov<\/em> ,    <em> E.M. Serebriany<\/em> ,<br \/>\n<strong> \u2116  205 <\/strong> QUANTUM EFFECTS IN SYSTEMS WITH ACCELEBRATED MIRRORS. II.ELECTROMAGNETIC FIELDS<br \/>\n<a href=\"http:\/\/preprints.lebedev.ru\/wp-content\/uploads\/2013\/03\/1979-205.djvu\" target=\"_blank\">\u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442<\/a>   <\/p>\n","protected":false},"excerpt":{"rendered":"<p>V.P. Frolov , E.M. Serebriany , \u2116 2 QIUHTUU EFFECTS IN SYSTEMS WITH ACCELERATED MIRRORS \u0421\u043a\u0430\u0447\u0430\u0442\u044c \u043f\u0440\u0435\u043f\u0440\u0438\u043d\u0442 |\u0410\u043d\u043d\u043e\u0442\u0430\u0446\u0438\u044f| The problem of the vacuum state definition in a part of the Minkowski space bounded by the single or two spherically symmetric uniformly accelerated mirrors is considered. The Euclidean approach is need to get the explicit expressions [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[8],"tags":[],"_links":{"self":[{"href":"http:\/\/preprints.lebedev.ru\/index.php?rest_route=\/wp\/v2\/posts\/5676"}],"collection":[{"href":"http:\/\/preprints.lebedev.ru\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"http:\/\/preprints.lebedev.ru\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"http:\/\/preprints.lebedev.ru\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"http:\/\/preprints.lebedev.ru\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=5676"}],"version-history":[{"count":0,"href":"http:\/\/preprints.lebedev.ru\/index.php?rest_route=\/wp\/v2\/posts\/5676\/revisions"}],"wp:attachment":[{"href":"http:\/\/preprints.lebedev.ru\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=5676"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"http:\/\/preprints.lebedev.ru\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=5676"},{"taxonomy":"post_tag","embeddable":true,"href":"http:\/\/preprints.lebedev.ru\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=5676"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}