Journal of Experimental and Theoretical Physics
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ZhETF, Vol. 117, No. 1, January 2000
(English translation - JETP, Vol. 90, No. 1, January 2000 available on-line at www.springer.com )

çÒÁ×ÉÔÁÃÉÑ, ÁÓÔÒÏÆÉÚÉËÁ
ëáîïîéþåóëïå ë÷áîôï÷áîéå ä÷õíåòîïê çòá÷éôáãéé
  5
ñÄÒÁ, ÞÁÓÔÉÃÙ, ÉÈ ×ÚÁÉÍÏÄÅÊÓÔ×ÉÑ
éúíåòåîéå ïôîïóéôåìøîïê ÷åòïñôîïóôé òáóðáäá φ→ηγ ÷ ëáîáìå η→π+π-π0
  22
áÔÏÍÙ, ÓÐÅËÔÒÙ, ÉÚÌÕÞÅÎÉÅ
÷ìéñîéå ðïìñòîïê óòåäù ïëòõöåîéñ îá íîïçïæïôïîîùå òåúïîáîóù ÷ äéðïìøîùè íïìåëõìáè
  29
óôïìëîï÷åîéñ üìåëôòïîï÷ ó íïìåëõìáíé, îáèïäñýéíéóñ ÷ ÷ïúâõöäåîîùè ëïìåâáôåìøîï-÷òáýáôåìøîùè óïóôïñîéñè
  35
TEMPERATURE DEPENDENCE OF THE FORMATION RATES OF HYDROGEN-HELIUM MESIC MOLECULES IN COLLISIONS OF SLOW HYDROGEN ATOMS WITH HELIUM
  51
÷ìéñîéå éîôåòæåòåîãéïîîùè üææåëôï÷ óðïîôáîîïçï éóðõóëáîéñ îá ðï÷åäåîéå é óðåëôòù òåúïîáîóîïê æìõïòåóãåîãéé ôòåèõòï÷îå÷ïçï áôïíá ÷ ðïìå óéìøîïê ÷ïìîù
  57
ðïìñòéúáãéñ ÷áëõõíá ÷ ÷ïäïòïäïðïäïâîïí òåìñôé÷éóôóëïí áôïíå: ó÷åòèôïîëáñ óôòõëôõòá
  67
ë÷áúéëìáóóéþåóëáñ æõîëãéñ çòéîá ÷ï ÷îåûîåí ðïìå é ðòïãåóóù òáóóåñîéñ îá íáìùå õçìù
  75
ðÌÁÚÍÁ, ÇÁÚÙ
÷ùîõöäåîîïå òáóóåñîéå íáîäåìøûôáíá-âòéììàüîá ÷ ðìáúíå ó éïîîï-ú÷õëï÷ïê ôõòâõìåîôîïóôøà
  90
ëïáçõìñãéñ úáòñöåîîùè þáóôéã ÷ ðùìå÷ïê ðìáúíå
  105
îÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ
äéæòáëãéïîîïå ïôòáöåîéå ó÷åôá ÷ èïìåóôåòéþåóëïí öéäëïí ëòéóôáììå ÷ ðòéóõôóô÷éé îåïâòáôéíïóôé ÷ïìî é æïòíõìá âòüççá-÷õìøæá äìñ óòåä ó îåïäéîáëï÷ùíé äìéîáíé ðòñíïê é ïâòáôîïê ÷ïìî
  115
ô×ÅÒÄÙÅ ÔÅÌÁ. óÔÒÕËÔÕÒÁ
íîïçïëòáôîïå íáìïõçìï÷ïå òáóóåñîéå îåêôòïîï÷ ðòé ðòïéú÷ïìøîïí úîáþåîéé âïòîï÷óëïçï ðáòáíåôòá
  122
æïôïæéúéþåóëéå ðòïãåóóù, óôéíõìéòï÷áîîùå ÷ îáîïðïòéóôïí ëòåíîéé íïýîùí ìáúåòîùí éúìõþåîéåí
  136
LOW-TEMPERATURE SPECIFIC HEAT STUDY OF SrCu2(BO3)2 WITH AN EXACTLY SOLVABLE GROUND STATE
  145
ô×ÅÒÄÙÅ ÔÅÌÁ. üÌÅËÔÒÏÎÎÙÅ Ó×ÏÊÓÔ×Á
÷úáéíïó÷ñúø ðòïóôòáîóô÷åîîùè é ÷òåíåîîùè îåõóôïêþé÷ïóôåê ÷ óéóôåíå ä÷õè îåìéîåêîùè ôïîëéè ðìåîïë
  149
îáòõûåîéå ðåòåîïòíéòõåíïóôé ÷ úáäáþå ëïîäï ÷ ÷ùóïëïôåíðåòáôõòîïí òáúìïöåîéé ó÷ïâïäîïê üîåòçéé
  162
ðï÷åòèîïóôîùå ðïìñòéôïîù ÷ äéüìåëôòéëå îá çòáîéãå ó íåôáììïí ÷ óëòåýåîîùè üìåëôòéþåóëïí é íáçîéôîïí ðïìñè
  175
ðåòåèïäù äéüìåëôòéë-ó÷åòèðòï÷ïäîéë-íåôáìì, éîäõãéòï÷áîîùå óðéîï÷ùíé æìõëôõáãéñíé, ÷ ðáòáíáçîéôîïê æáúå ìåçéòï÷áîîùè äéüìåëôòéëï÷
  182
æáúï÷ùå ðåòåèïäù ÷ ä÷õíåòîïê ÷éèòå÷ïê óéóôåíå ó äåæåëôáíé: íïäåìéòï÷áîéå íåôïäïí íïîôå-ëáòìï
  196
BOUND FERROMAGNETIC AND PARAMAGNETIC POLARONS AS AN ORIGIN OF THE RESISTIVITY PEAK IN FERROMAGNETIC SEMICONDUCTORS AND MANGANITES
  207
éóóìåäï÷áîéå íáçîéôîùè ó÷ïêóô÷ óìáâï÷úáéíïäåêóô÷õàýéè áîôéæåòòïíáçîéôîùè ãåðïþåë ó áìøôåòîéòï÷áîîùí ïâíåîîùí ÷úáéíïäåêóô÷éåí óï óðéîïí S=1/2 ðòé ðïíïýé ë÷áîôï÷ïçï íåôïäá íïîôå-ëáòìï
  218
óáíïïòçáîéúáãéñ ëòéôéþåóëïçï óïóôïñîéñ ÷ çòáîõìéòï÷áîîùè ó÷åòèðòï÷ïäîéëáè
  227
÷ìéñîéå íáçîéôîïçï ðïìñ îá ôåòíïóôéíõìéòï÷áîîõà éïîéúáãéà ðòéíåóîùè ãåîôòï÷ ÷ ðïìõðòï÷ïäîéëáè óõâíéììéíåôòï÷ùí éúìõþåîéåí
  243
òÁÚÎÏÅ
ðòïãåóó òåëïíâéîáãéé, óïðòï÷ïöäáàýéêóñ ôåìåðïòôáãéåê «ë÷áîôï÷ïê úáãåðìåîîïóôé»
  248
 
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