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 123, ÷ÙÐ. 5, íÁÊ 2003
(áÎÇÌÉÊÓËÉÊ ÐÅÒÅ×ÏÄ - JETP, Vol. 96, No 5, May 2003 ÄÏÓÔÕÐÅÎ on-line ÎÁ www.springer.com )


ñÄÒÁ, ÞÁÓÔÉÃÙ, ÉÈ ×ÚÁÉÍÏÄÅÊÓÔ×ÉÑ

ä÷éöåîéå óðéîá þáóôéã ÷ îåïäîïòïäîïí üìåëôòïíáçîéôîïí ðïìå
  883
HYPERNUCLEI AS CHIRAL SOLITONS
  891
éóóìåäï÷áîéå ðòïãåóóï÷ e+e-\to\pi+\pi-\pi+\pi- é e+e-\to\pi+\pi-\pi0\pi0 ÷ ïâìáóôé üîåòçéé \sqrt{s} = 0.98-1.38 çÜ÷ ÷ üëóðåòéíåîôáè óï óæåòéþåóëéí îåêôòáìøîùí äåôåëôïòïí
  899

áÔÏÍÙ, ÓÐÅËÔÒÙ, ÉÚÌÕÞÅÎÉÅ

ëïçåòåîôîïå ðìåîåîéå îáóåìåîîïóôé ÷ çáúå ÷ïúâõöäåîîùè áôïíï÷
  912
ëïíâéîáãéïîîïå üèï ðòé ÷ïúâõöäåîéé óòåäù ðòåäåìøîï ëïòïôëéíé éíðõìøóáíé
  919
ïâïâýåîîïå òåûåîéå íéìîá äìñ ëïòòåìñãéïîîùè üææåëôï÷ íîïçïëòáôîïçï òáóóåñîéñ ó÷åôá ó õþåôïí ðïìñòéúáãéé
  929
æòáëôáìù é èáïôéþåóëïå òáóóåñîéå áôïíï÷ ÷ ðïìå óôáãéïîáòîïê óôïñþåê ó÷åôï÷ïê ÷ïìîù
  946
üìåëôòïîîïå ÷ïúâõöäåîéå íáôòéãù ðòé äòåêæå éúâùôïþîùè üìåëôòïîï÷ þåòåú ô÷åòäùê ëóåîïî
  962
÷ïìîï÷ïäîïå òáóðòïóôòáîåîéå üìåëôòïíáçîéôîïçï éúìõþåîéñ ÷ ðïìùè íéëòïóôòõëôõòéòï÷áîîùè é æïôïîîï-ëòéóôáììéþåóëéè ÷ïìïëîáè
  975
üìåëôòïî ÷ ëõìïîï÷óëïí é éîôåîóé÷îïí îéúëïþáóôïôîïí ìáúåòîïí ðïìñè
  991
POLARITON EFFECT IN NONLINEAR PULSE PROPAGATION
  997

ðÌÁÚÍÁ, ÇÁÚÙ

éïîéúáãéïîîáñ æïëõóéòï÷ëá ëïòïôëïçï éîôåîóé÷îïçï ìáúåòîïçï éíðõìøóá é çåîåòáãéñ ëéìø÷áôåòîùè ðìáúíåîîùè ÷ïìî
  1006
ï òïìé ðòåäùíðõìøóá ðòé îáçòå÷å ô÷åòäïôåìøîùè íéûåîåê íïýîùí ðéëïóåëõîäîùí ìáúåòîùí éíðõìøóïí
  1019
ðïîäåòïíïôïòîùå üææåëôù ðòé ÷ïúäåêóô÷éé éîôåîóé÷îïê ÷ïìîù îáëáþëé îá üìåëôòïîîùå é ðìáúíåîîùå óçõóôëé
  1027

îÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ

TEMPERATURE PITCH VARIATIONS IN PLANAR CHOLESTERIC LAYERS: THE ROLE OF FLUCTUATIONS AND SURFACE ANCHORING
  1040

ô×ÅÒÄÙÅ ÔÅÌÁ. óÔÒÕËÔÕÒÁ

THEORETICAL INVESTIGATION OF THE RESONANT HYPER-RAMAN SCATTERING BY OPTICAL PHONONS
  1048

ô×ÅÒÄÙÅ ÔÅÌÁ. üÌÅËÔÒÏÎÎÙÅ Ó×ÏÊÓÔ×Á

1/Q-òáúìïöåîéå äìñ üîåòçåôéþåóëïçï óðåëôòá ë÷áîôï÷ùè ôïþåë
  1059
ïâîáòõöåîéå æïôïðòï÷ïäéíïóôé ÷ ó÷åòèôïîëéè íåôáììéþåóëéè ðìåîëáè ÷ ÷éäéíïê é éîæòáëòáóîïê ïâìáóôñè óðåëôòá
  1067
ôåïòåôéþåóëéê ðòïçîïú ïâõóìï÷ìåîîïçï ðï÷åòèîïóôøà óðéî-ðåòåïòéåîôáãéïîîïçï æáúï÷ïçï ðåòåèïäá ÷ îáîïëòéóôáììáè ÷aFe12O19
  1073
TIME REVERSAL SYMMETRY BREAKING IN CUPRATES INDUCED BY THE SPIRAL SPIN ORDER
  1082
íáçîéôîùå é óôòõëôõòîùå æáúï÷ùå ðåòåèïäù ÷ óåçîåôïíáçîåôéëå YMn2O5, éîäõãéòï÷áîîùå óéìøîùí íáçîéôîùí ðïìåí
  1090
òåúïîáîóîïå ôõîîåìéòï÷áîéå üìåëôòïîï÷, ÷úáéíïäåêóô÷õàýéè ó æïîïîáíé
  1096

îÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ

ó÷ïêóô÷á óìáâïëïììáðóéòõàýéè òåûåîéê îåìéîåêîïçï õòá÷îåîéñ ûòåäéîçåòá
  1106

òÁÚÎÏÅ

üëóôòåíáìøîïå <<òáóðõôù÷áîéå>> ë÷áîôï÷ïê ïðåòáãéé
  1113
 
óÏÏÂÝÉÔØ Ï ÔÅÈÎÉÞÅÓËÉÈ ÐÒÏÂÌÅÍÁÈ