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 122, ÷ÙÐ. 4, ïËÔÑÂÒØ 2002
(áÎÇÌÉÊÓËÉÊ ÐÅÒÅ×ÏÄ - JETP, Vol. 95, No 4, October 2002 ÄÏÓÔÕÐÅÎ on-line ÎÁ www.springer.com )


ñÄÒÁ, ÞÁÓÔÉÃÙ, ÉÈ ×ÚÁÉÍÏÄÅÊÓÔ×ÉÑ

ï óõííéòï÷áîéé òáóèïäñýéèóñ òñäï÷ ôåïòéé ÷ïúíõýåîéê ÷ ë÷áîôï÷ïê íåèáîéëå é ôåïòéé ðïìñ
  675
ëïííåîôáòéê ë óôáôøå ä. é. ëáúáëï÷á é ÷. ó. ðïðï÷á
  696

áÔÏÍÙ, ÓÐÅËÔÒÙ, ÉÚÌÕÞÅÎÉÅ

ðòéíåîåîéå íïäåìé ïâÿåäéîåîîïçï áôïíá äìñ ïãåîëé ÷òåíåîé öéúîé ïôòéãáôåìøîùè íïìåëõìñòîùè éïîï÷ ïôîïóéôåìøîï á÷ôïïôýåðìåîéñ üìåëôòïîá
  700
íéëòïíáúåòîáñ çåîåòáãéñ îá ëïòòåìéòï÷áîîùè áôïíáè
  707
ôåïòåôéþåóëïå éóóìåäï÷áîéå òåáëãéê p+He\rightarrow H+He+ é p+He\rightarrow H+He+++e ðòé ó÷åòèíáìùè õçìáè òáóóåñîéñ ÷ïäïòïäá
  717
AMPLIFICATION OF SHORT LASER PULSES BY RAMAN BACKSCATTERING IN CAPILLARY PLASMAS
  723
çåîåòáãéñ âéæïôïîîïçï ó÷åôá ÷ ðïìñòéúáãéïîîï-þáóôïôîùè âåììï÷óëéè óïóôïñîéñè
  738
SEMICLASSICAL APPROACH TO STATES NEAR THE POTENTIAL BARRIER TOP
  746

ðÌÁÚÍÁ, ÇÁÚÙ

óôáôéóôéþåóëéå é äéîáíéþåóëéå éîôåîóé÷îïóôé áôïíîùè óðåëôòáìøîùè ìéîéê ÷ ðìáúíå
  765
äéîáíéëá íáëòïþáóôéã ÷ ðìáúíå ôìåàýåçï òáúòñäá ðïóôïñîîïçï ôïëá ÷ õóìï÷éñè íéëòïçòá÷éôáãéé
  778
ï ëéîåôéþåóëïí ïâïóîï÷áîéé ïâïâýåîîïê îåòá÷îï÷åóîïê ôåòíïäéîáíéëé íîïçïëïíðïîåîôîùè óéóôåí
  789
üìåëôòïíáçîéôîï éîäõãéòï÷áîîáñ ðòïúòáþîïóôø ÷ ÷ùóïëïôåíðåòáôõòîïê íáçîéôïáëôé÷îïê ðìáúíå
  805
÷ìéñîéå ðòéðï÷åòèîïóôîïçï üìåëôòïîîïçï óìïñ îá üîåòçåôéþåóëéê óðåëôò æïôïüìåëôòïîï÷
  814

îÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ

A LIQUID-LIQUID PHASE TRANSITION IN THE «COLLAPSING» HARD SPHERE SYSTEM
  820
DISCLINATION MOTION IN LIQUID CRYSTALLINE FILMS
  824
TEMPERATURE- AND FIELD-INDUCED TRANSITIONS IN FREE-STANDING FILMS OF AN ANTIFERROELECTRIC LIQUID CRYSTAL
  840

ô×ÅÒÄÙÅ ÔÅÌÁ. óÔÒÕËÔÕÒÁ

PRESSURE-INDUCED TRANSFORMATIONS AND OPTICAL PROPERTIES OF THE TWO-DIMENSIONAL TETRAGONAL POLYMER OF C60 AT PRESSURES UP TO 30 GPa
  849
æáúï÷ùå ðòå÷òáýåîéñ ÷ ðåòï÷óëéôáè TbBaCo2-xFexO5+γ
  863

ô×ÅÒÄÙÅ ÔÅÌÁ. üÌÅËÔÒÏÎÎÙÅ Ó×ÏÊÓÔ×Á

ôõîîåìøîïå íáçîéôïóïðòïôé÷ìåîéå æáúï÷ï-òáóóìïåîîùè íáîçáîéôï÷
  869
ëìáóóéþåóëéå é ë÷áîôï÷ùå üææåëôù ÷ äéîáíéëå íåúïóëïðéþåóëïçï íáçîéôá, éîäõãéòï÷áîîùå óðéîï÷ùí ôïëïí
  879
îåõóôïêþé÷ïóôø æòïîôá ðåòåíáçîéþé÷áîéñ ÷ áîéúïôòïðîùè ó÷åòèðòï÷ïäîéëáè
  886

îÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ

ìéîåêîùå é îåìéîåêîùå ëïìåâáîéñ é ÷ïìîù ÷ ïðôéþåóëéè éìé áëõóôéþåóëéè ó÷åòèòåûåôëáè (æïôïîîùè éìé æïîïîîùè ëòéóôáììáè)
  897
 
óÏÏÂÝÉÔØ Ï ÔÅÈÎÉÞÅÓËÉÈ ÐÒÏÂÌÅÍÁÈ