Journal of Experimental and Theoretical Physics
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ZhETF, Vol. 137, No. 2, February 2010
(English translation - JETP, Vol. 110, No. 2, February 2010 available on-line at www.springer.com )

áÔÏÍÙ, ÍÏÌÅËÕÌÙ, ÏÐÔÉËÁ
ë ÷ïðòïóõ ï ðòéçïôï÷ìåîéé ðåòåðõôáîîùè ðáò ðïìñòéúáãéïîîùè ëõâéôï÷ ÷ þáóôïôîï-îå÷ùòïöäåîîïí òåöéíå
  211
ELECTRIC FIELD ENHANCEMENT BETWEEN TWO PARALLEL CYLINDERS DUE TO PLASMONIC RESONANCE
Vorobev P.
ID:20  DJVU (71.5K) PDF (192.7K)

  220
òáóþåô ÷ïúâõöäåîîùè óïóôïñîéê íïìåëõì ðòé ðïíïýé íåôïäá ôåïòéé æõîëãéïîáìá ðìïôîïóôé ó ïòâéôáìøîï-úá÷éóéíùí îåáäéáâáôéþåóëéí ïâíåîîùí ñäòïí
  226
ñÄÒÁ, ÞÁÓÔÉÃÙ, ÐÏÌÑ, ÇÒÁ×ÉÔÁÃÉÑ É ÁÓÔÒÏÆÉÚÉËÁ
éúìõþåîéå áëóéïîï÷ ÷ïäïòïäïðïäïâîùí áôïíïí ÷ ó÷åòèóéìøîïí íáçîéôîïí ðïìå
  241
÷ïúíïöîïå ïâÿñóîåîéå ëïòòåìñãéê íåöäõ óïâùôéñíé ðïäúåíîùè äåôåëôïòï÷, úáòåçéóôòéòï÷áîîùè ÷ ðåòéïä ÷óðùûëé SN 1987A
  250
äéóðåòóéñ îåêôòéîï ÷ úáòñäï÷ï-óéííåôòéþîïê ðìáúíå
  259
áëëòåãéñ üëúïôéþåóëïê íáôåòéé îá þåòîõà äùòõ òåêóîåòá - îïòäóôòåíá
  268
ðÏÒÑÄÏË, ÂÅÓÐÏÒÑÄÏË É ÆÁÚÏ×ÙÅ ÐÅÒÅÈÏÄÙ × ËÏÎÄÅÎÓÉÒÏ×ÁÎÎÙÈ ÓÒÅÄÁÈ
òá÷îï÷åóîùå úîáþåîéñ é äéîáíéëá óõííáòîïçï íáçîéôîïçï íïíåîôá óéóôåí íáçîéôîùè äéðïìåê
  277
îåòá÷îï÷åóîáñ ëòéôéþåóëáñ òåìáëóáãéñ óôòõëôõòîï îåõðïòñäïþåîîùè óéóôåí ÷ ëïòïôëï÷òåíåîîïí òåöéíå: òåîïòíçòõððï÷ïå ïðéóáîéå é ëïíðøàôåòîïå íïäåìéòï÷áîéå
  287
ðòï÷ïäéíïóôø ä÷õíåòîïê íïäåìé óôòõëôõòîï áîéúïôòïðîïçï ëïíðïúéôá
  301
÷ìéñîéå õäáòîï-÷ïìîï÷ïçï óöáôéñ äï 65 çðÁ îá ëòéóôáììéþåóëõà óôòõëôõòõ é ó÷åòèðòï÷ïäñýéå ó÷ïêóô÷á MgB2
  311
üÌÅËÔÒÏÎÎÙÅ Ó×ÏÊÓÔ×Á Ô×ÅÒÄÙÈ ÔÅÌ
áîïíáìéé ðïìñòéôïîîïê äéîáíéëé ïäîïíåòîïçï íáçîéôîïçï æïôïîîïçï ëòéóôáììá ó áîôéæåòòïíáçîéôîùí ôéðïí íåöóìïå÷ïçï õðïòñäïþåîéñ ÷ ðïóôïñîîïí ÷îåûîåí üìåëôòéþåóëïí ðïìå
  318
NUCLEAR QUADRUPOLE SPIN-LATTICE RELAXATION IN Bi4 Ge3 O12 SINGLE CRYSTALS DOPED WITH ATOMS OF d OR f ELEMENTS. CRYSTAL FIELD EFFECTS IN COMPOUNDS EXHIBITING ANOMALOUS MAGNETIC PROPERTIES
  336
üìåëôòïîîùê óðåëôò é ôåðìïåíëïóôø ôñöåìùè æåòíéïîï÷ ÷ óëïûåîîïê æáúå áîôéæåòòïíáçîéôîùè éîôåòíåôáììéäï÷
  341
GATE-TUNABLE BANDGAP IN BILAYER GRAPHENE
  361
TWO-DIMENSIONAL ANDERSON-HUBBARD MODEL IN THE DMFT+ Σ APPROXIMATION
  368
ó÷åòèðòï÷ïäñýéê ôïë ÷ çéâòéäîùè óôòõëôõòáè ó áîôéæåòòïíáçîéôîïê ðòïóìïêëïê
  380
óÔÁÔÉÓÔÉÞÅÓËÁÑ, ÎÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ, ÆÉÚÉËÁ <<ÍÑÇËÏÊ ÍÁÔÅÒÉÉ>>
÷ìéñîéå ëòïóóëïòòåìñãéê íåöäõ îåïäîïòïäîïóôñíé ðáòáíåôòï÷ éúïôòïðîïê óòåäù îá óðåëôò é úáôõèáîéå õðòõçéè ÷ïìî
  390
äéîáíéëá îáíáçîéþåîîïóôé éúïìéòï÷áîîïê éúéîçï÷óëïê ãåðïþëé
  406
 
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