öÕÒÎÁÌ üËÓÐÅÒÉÍÅÎÔÁÌØÎÏÊ É ôÅÏÒÅÔÉÞÅÓËÏÊ æÉÚÉËÉ
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öüôæ, ôÏÍ 146, ÷ÙÐ. 3, óÅÎÔÑÂÒØ 2014
(áÎÇÌÉÊÓËÉÊ ÐÅÒÅ×ÏÄ - JETP, Vol. 119, No 3, September 2014 ÄÏÓÔÕÐÅÎ on-line ÎÁ www.springer.com )


áÔÏÍÙ, ÍÏÌÅËÕÌÙ, ÏÐÔÉËÁ

óðåëôò éïîï÷ ðòé ÷ïúâõöäåîéé ëìáóôåòîïçï ðõþëá ìáúåòîùí éíðõìøóïí
  420
÷ùòïöäåîéå îéúëïþáóôïôîùè òåúïîáîóï÷ ÷ ëéòáìøîïí áîéúïôòïðîï ðòï÷ïäñýåí ãéìéîäòå, úáðïìîåîîïí íåôáíáôåòéáìïí
  429
üìåëôòïïðôéþåóëéå ó÷ïêóô÷á ïäîïíåòîùè æïôïîîùè ëòéóôáììï÷ îá ïóîï÷å ïòçáîéþåóëïçï óåçîåôïüìåëôòéëá é ëòáóéôåìñ
  439
K-SHELL X-RAY INTENSITY RATIOS AND VACANCY TRANSFER PROBABILITIES OF Pt, Au, AND Pb BY A SIMPLE METHOD
  448
äåúéîôåçòáãéñ ëìáóôåòï÷ ArN, KrN é ( N2)N ðòé óôïìëîï÷åîéé ó ëïìåâáôåìøîï-÷ùóïëï÷ïúâõöäåîîùíé íïìåëõìáíé SF6
  455
LOADING OF A KRYPTON MAGNETO-OPTICAL TRAP WITH TWO HOLLOW LASER BEAMS IN A ZEEMAN SLOWER
  464
ROBUST STATIONARY DISTRIBUTED DISCORD IN THE JORDAN-WIGNER FERMION SYSTEM UNDER PERTURBATIONS OF THE INITIAL STATE
  471
óïìéôïîïðïäïâîïå òáóðòïóôòáîåîéå ûéòïëïðïìïóîùè ôåòáçåòãå÷ùè éíðõìøóï÷ ÷ óéóôåíå ôõîîåìøîùè ðåòåèïäï÷
  483

ñÄÒÁ, ÞÁÓÔÉÃÙ, ÐÏÌÑ, ÇÒÁ×ÉÔÁÃÉÑ É ÁÓÔÒÏÆÉÚÉËÁ

íõìøôéòáúíåòîïå çòá÷éôáãéïîîïå ÷úáéíïäåêóô÷éå. ëòé÷ùå ÷òáýåîéñ çáìáëôéë
  500
îï÷ùå éúíåòåîéñ üîåòçåôéþåóëéè óðåëôòï÷ ðòïôïîï÷ é ñäåò çåìéñ ëïóíéþåóëéè ìõþåê ÷ùóïëéè üîåòçéê ðòé ðïíïýé ëáìïòéíåôòá ÷ üëóðåòéíåîôå ðáíåìá
  513

ô×ÅÒÄÙÅ ÔÅÌÁ É ÖÉÄËÏÓÔÉ

áîïíáìøîáñ óöéíáåíïóôø é íåôáììéúáãéñ äåêôåòéñ é ÷ïäïòïäá ðòé ÷ùóïëéè äá÷ìåîéñè
  518
áîéúïôòïðéñ ôåðìïðòï÷ïäîïóôé íïîïëòéóôáììéþåóëéè îáîïðìåîïë é îáîïðòï÷ïäï÷ ðòé îéúëéè ôåíðåòáôõòáè
  525
ON THE THEORY OF POINT DEFECT RECOMBINATION IN CRYSTALS
  540

ðÏÒÑÄÏË, ÂÅÓÐÏÒÑÄÏË É ÆÁÚÏ×ÙÅ ÐÅÒÅÈÏÄÙ × ËÏÎÄÅÎÓÉÒÏ×ÁÎÎÙÈ ÓÒÅÄÁÈ

íáçîéôîùå ó÷ïêóô÷á é íåèáîéúí æïòíéòï÷áîéñ îåóëïíðåîóéòï÷áîîïçï íáçîéôîïçï íïíåîôá áîôéæåòòïíáçîéôîùè îáîïþáóôéã æåòòéçéäòéôá âáëôåòéáìøîïçï ðòïéóèïöäåîéñ
  546
ïóïâåîîïóôé òáóóåñîéñ æïîïîï÷ ôåðìï÷ùè þáóôïô é æåòòïíáçîéôîùå ó÷ïêóô÷á ÷áòéóôïòîïê ëåòáíéëé ZnO
  557
EFFECT OF VORTEX PINNING BY POINT DEFECTS ON THE LOWER CRITICAL FIELD IN LAYERED SUPERCONDUCTORS
  563
÷ìéñîéå íáçîéôïõðòõçïçï ÷úáéíïäåêóô÷éñ îá ôåòíïäéîáíéëõ æåòòïíáçîåôéëï÷: íïäåìéòï÷áîéå íåôïäïí óðéî-òåûåôïþîïê äéîáíéëé
  574
÷éèòå÷áñ óôòõëôõòá é áîéúïôòïðéñ üìåëôòïóïðòïôé÷ìåîéñ ÷ íïîïëòéóôáììáè Bi2 Sr1.65 La0.35 CuO6+δ
  586
áäóïòâãéñ é äéææõúéñ ÷ïäïòïäá îá ðï÷åòèîïóôé óðìá÷á PdTa
  594
CRYSTAL AND MAGNETIC PROPERTIES OF THE NEW COPPER-SODIUM BORATE CuNaB3 O62 O
  607
ôåðìï÷ïå òáóûéòåîéå äéóåìåîéäá îéïâéñ ÷ âáúéóîïê ðìïóëïóôé ðòé îéúëéè ôåíðåòáôõòáè
  618
üìáóôïüìåëôòéþåóëéê üææåëô ÷ îåõðïòñäïþåîîïê ïäîïòïäîïê îåðòï÷ïäñýåê óòåäå ðòé ãåîôòïóéííåôòéþîùè ÷îåûîéè ÷ïúäåêóô÷éñè
  624

üÌÅËÔÒÏÎÎÙÅ Ó×ÏÊÓÔ×Á Ô×ÅÒÄÙÈ ÔÅÌ

KINEMATIC SPIN-FLUCTUATION MECHANISM OF HIGH-TEMPERATURE SUPERCONDUCTIVITY
  631
íáçîéôîï-òåúïîáîóîáñ üäó ÷ ôïîëéè ðìåîëáè íáîçáîéôá
  645
ä÷áöäù äéææåòåîãéáìøîïå óåþåîéå îåõðòõçïçï íáçîéôîïçï òáóóåñîéñ îåêôòïîï÷ ÷ ðáòáíáçîéôîïê æáúå LaCoO3
  651
EFFECT OF ELECTRON-PHONON INTERACTIONS ON RAMAN LINE AT FERROMAGNETIC ORDERING
  657

óÔÁÔÉÓÔÉÞÅÓËÁÑ, ÎÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ, ÆÉÚÉËÁ <<ÍÑÇËÏÊ ÍÁÔÅÒÉÉ>>

÷ìéñîéå ïòâéôáìøîïçï ä÷éöåîéñ îá ëïììáðó ëïìøãå÷ùè ÷éèòåê ÷ áëëòåãéïîîïí ðïôïëå
  663
 
óÏÏÂÝÉÔØ Ï ÔÅÈÎÉÞÅÓËÉÈ ÐÒÏÂÌÅÍÁÈ