öÕÒÎÁÌ üËÓÐÅÒÉÍÅÎÔÁÌØÎÏÊ É ôÅÏÒÅÔÉÞÅÓËÏÊ æÉÚÉËÉ
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ïÂÝÁÑ ÉÎÆÏÒÍÁÃÉÑ Ï ÖÕÒÎÁÌÅ
úÏÌÏÔÙÅ ÓÔÒÁÎÉÃÙ
áÄÒÅÓÁ ÒÅÄÁËÃÉÉ
óÏÄÅÒÖÁÎÉÅ ÖÕÒÎÁÌÁ
óÏÏÂÝÅÎÉÑ ÒÅÄÁËÃÉÉ
ðÒÁ×ÉÌÁ ÄÌÑ Á×ÔÏÒÏ×
úÁÇÒÕÚÉÔØ ÓÔÁÔØÀ
ðÒÏ×ÅÒÉÔØ ÓÔÁÔÕÓ ÓÔÁÔØÉ


öüôæ, ôÏÍ 126, ÷ÙÐ. 5, îÏÑÂÒØ 2004
(áÎÇÌÉÊÓËÉÊ ÐÅÒÅ×ÏÄ - JETP, Vol. 99, No 5, November 2004 ÄÏÓÔÕÐÅÎ on-line ÎÁ www.springer.com )


çÒÁ×ÉÔÁÃÉÑ, ÁÓÔÒÏÆÉÚÉËÁ

íáëòïóëïðéþåóëáñ óéóôåíá õòá÷îåîéê üêîûôåêîá-íáëó÷åììá äìñ óéóôåíù ÷úáéíïäåêóô÷õàýéè þáóôéã ó òáúîùíé íáóóáíé
  1027

ñÄÒÁ, ÞÁÓÔÉÃÙ, ÉÈ ×ÚÁÉÍÏÄÅÊÓÔ×ÉÑ

RADIATIVE CORRECTIONS TO DEEP INELASTIC ELECTRON - DEUTERON SCATTERING. THE CASE OF TENSOR-POLARIZED DEUTERON
  1034

áÔÏÍÙ, ÓÐÅËÔÒÙ, ÉÚÌÕÞÅÎÉÅ

òåúïîáîóù ÷ òáóóåñîéé üìåëôòïîï÷ íïìåëõìáíé
  1051
ðéëïóåëõîäîïå ÷ùîõöäåîîïå ëïíâéîáãéïîîïå òáóóåñîéå ÷ ëòéóôáììáè
  1073
ïðôéþåóëïå ÷ùðòñíìåîéå ÷ õçìåòïäîùè îáîïðìåîëáè
  1083
îåëìáóóéþåóëéê ó÷åô ðòé ë÷áúéóéîèòïîîïí ðáòáíåôòéþåóëïí óáíïðòåïâòáúï÷áîéé þáóôïôù
  1089
ðïìñòéúáãéïîîïå ôïòíïúîïå éúìõþåîéå ôñöåìùè úáòñöåîîùè þáóôéã ÷ ðïìéëòéóôáììå
  1101
ïóïâåîîïóôé òåæòáëãéé îåïâùëîï÷åîîïçï ìõþá ÷ çåìéëïéäáìøîïê óòåäå ó âïìøûéí ûáçïí óðéòáìé
  1109

ðÌÁÚÍÁ, ÇÁÚÙ

ëïíðòåóóéñ ó÷éóôï÷ùè ÷ïìî ÷ ðìáúíå ó îåóôáãéïîáòîùí íáçîéôîùí ðïìåí
  1123

îÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ

çåîåòáãéñ óðéòáìøîïóôé ÷ ïäîïòïäîï-÷éîôï÷ùè ÷éèòå÷ùè ðïôïëáè
  1133
îåðáòáíåôòéþåóëïå íáóûôáâîïå õòá÷îåîéå óïóôïñîéñ é áððòïëóéíáãéñ P-\rho-T-äáîîùè ÷âìéúé ëòéôéþåóëïê ôïþëé ðáòïïâòáúï÷áîéñ öéäëïóôåê
  1146
äéææõúéñ é ëìáóôåòéúáãéñ ïóåäáàýåê ðòéíåóé ÷ óìõþáêîùè çéäòïäéîáíéþåóëéè ðïôïëáè
  1153
èáïôéþåóëïå òáóóåñîéå, ôòáîóðïòô é æòáëôáìù ÷ ðòïóôïí çéäòïäéîáíéþåóëïí ðïôïëå
  1167
úáëïîù ðïäïâéñ äìñ óëïòïóôé, ôåíðåòáôõòù é ëïíðïîåîô ôåîúïòá òåêîïìøäóá ÷ ðòéóôåîïþîïê ïâìáóôé ôõòâõìåîôîïçï ðïçòáîéþîïçï óìïñ îá ðòïîéãáåíïê ðï÷åòèîïóôé
  1180
ôåòíïíåèáîéþåóëéê üææåëô ÷ ãéìéîäòéþåóëé-çéâòéäîïí îåíáôéþåóëïí öéäëïí ëòéóôáììå
  1192

ô×ÅÒÄÙÅ ÔÅÌÁ. óÔÒÕËÔÕÒÁ

éîäõãéòï÷áîîùå îåïäîïòïäîïóôñíé æáúï÷ùå ðåòåèïäù ÷ôïòïçï òïäá ÷ íïäåìé ðïôôóá îá éåòáòèéþåóëéè òåûåôëáè
  1198
òïìø äåæåëôï÷ ÷ æïòíéòï÷áîéé íîïçïäïíåîîïçï óïóôïñîéñ ìåçëïðìïóëïóôîùè áîôéæåòòïíáçîåôéëï÷ ó íáçîéôïõðòõçéí ÷úáéíïäåêóô÷éåí
  1209

ô×ÅÒÄÙÅ ÔÅÌÁ. üÌÅËÔÒÏÎÎÙÅ Ó×ÏÊÓÔ×Á

íáçîéôîùê íïíåîô ë÷áäòáôîùè äöïúåæóïîï÷óëéè SIS-óåôïë. óáíïïòçáîéúï÷áîîáñ ëòéôéþîïóôø
  1221
òåúïîáîóîïå ôõîîåìéòï÷áîéå ÷ ó÷åòèðòï÷ïäñýéè ðåòåèïäáè ó òáúìéþîïê óéííåôòéåê ðáòáíåôòá ðïòñäëá
  1232
SYMMETRY-BREAKING SOLUTIONS OF THE GINZBURG-LANDAU EQUATION
  1249
STATIC AND DYNAMIC CHARGE INHOMOGENEITY AND CRYSTAL-FIELD FLUCTUATIONS FOR 4f IONS IN HIGH-Tc CUPRATES
  1267
 
óÏÏÂÝÉÔØ Ï ÔÅÈÎÉÞÅÓËÉÈ ÐÒÏÂÌÅÍÁÈ