öÕÒÎÁÌ üËÓÐÅÒÉÍÅÎÔÁÌØÎÏÊ É ôÅÏÒÅÔÉÞÅÓËÏÊ æÉÚÉËÉ |
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öüôæ, ôÏÍ 148, ÷ÙÐ. 3, óÅÎÔÑÂÒØ 2015
(áÎÇÌÉÊÓËÉÊ ÐÅÒÅ×ÏÄ - JETP,
Vol. 121, No 3, September 2015
ÄÏÓÔÕÐÅÎ on-line ÎÁ www.springer.com
)
áÔÏÍÙ, ÍÏÌÅËÕÌÙ, ÏÐÔÉËÁ
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ELECTRON ATTACHMENT TO THE SF6 MOLECULE
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435
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òáóóåñîéå üìåëôòïíáçîéôîùè éíðõìøóï÷ îá íåôáììéþåóëéè îáîïóæåòáè ó õþåôïí ðìáúíïîîùè éîôåòæåòåîãéïîîùè üææåëôï÷
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444
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ï ëïíðåîóáãéé ó÷åôï÷ïçï óä÷éçá þáóôïôù òáäéïïðôéþåóëïçï ó÷þ-òåúïîáîóá ÷ ïðôéþåóëé ïòéåîôéòï÷áîîùè ýåìïþîùè áôïíáè ó ìáúåòîïê îáëáþëïê
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453
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ñÄÒÁ, ÞÁÓÔÉÃÙ, ÐÏÌÑ, ÇÒÁ×ÉÔÁÃÉÑ É ÁÓÔÒÏÆÉÚÉËÁ
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HAWKING RADIATION OF SPIN-1 PARTICLES FROM A THREE-DIMENSIONAL ROTATING HAIRY BLACK HOLE
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466
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NUCLEON QCD SUM RULES IN THE INSTANTON MEDIUM
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470
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ðÏÒÑÄÏË, ÂÅÓÐÏÒÑÄÏË É ÆÁÚÏ×ÙÅ ÐÅÒÅÈÏÄÙ × ËÏÎÄÅÎÓÉÒÏ×ÁÎÎÙÈ ÓÒÅÄÁÈ
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õóéìåîéå íáçîéôïåíëïóôîïçï üææåëôá ÷ï ÷îåûîåí üìåëôòéþåóëïí ðïìå ÷ ðìåîëáè Lax Bi1-x FeO3
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485
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áîïíáìøîïå ÷ìéñîéå äïâá÷ïë Sm îá íáçîéôîùå ó÷ïêóô÷á éîôåòíåôáììéäï÷ (Nd1-x Smx Dy)(FeCo)B
ëÁÂÌÏ× å.î., ïÓÐÅÎÎÉËÏ×Á ï.ç., ëÁÂÌÏ× ä.å., ðÉÓËÏÒÓËÉÊ ÷.ð., ÷ÁÌÅÅ× ò.á., ëÏÒÏÌÅ× ä.÷., òÅÚÞÉËÏ×Á é.é., ëÕÎÉÃÙÎÁ å.é., ôÁÌÁÎÃÅ× á.ä., äÍÉÔÒÉÅ× á.é., íÏÒÇÕÎÏ× ò.â.
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493
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ïðôéþåóëéå é íáçîéôïïðôéþåóëéå üææåëôù ÷ íïîïëòéóôáììáè Hg1-x Cdx Cr2 Se4 (0\leq x\leq 1)
óÕÈÏÒÕËÏ× à.ð., ôÅÌÅÇÉÎ á.÷., âÅÂÅÎÉÎ î.ç., úÁÊÎÕÌÌÉÎÁ ò.é., íÏÓÔÏ×ÝÉËÏ×Á å.÷., ÷ÉÇÌÉÎ î.á., çÁÎØÛÉÎÁ å.á., úÙËÏ× ç.ó., æÅÄÏÒÏ× ÷.á., íÅÎÝÉËÏ×Á ô.ë., âÕÞËÅ×ÉÞ á.á.
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503
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óðéî-óðéîï÷áñ ëïòòåìñãéïîîáñ äìéîá ÷ ä÷õíåòîïí æòõóôòéòï÷áîîïí íáçîåôéëå é åå ó÷ñúø ó äïðéòï÷áîéåí
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514
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üÌÅËÔÒÏÎÎÙÅ Ó×ÏÊÓÔ×Á Ô×ÅÒÄÙÈ ÔÅÌ
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ôåíðåòáôõòîáñ úá÷éóéíïóôø üìåëôòïîîïê óôòõëôõòù La2 CuO4 ÷ íîïçïüìåëôòïîîïí ðïäèïäå LDA+GTB
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526
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áäóïòâãéñ, äéææõúéñ é éîôåòëáìñãéñ áôïíï÷ ýåìïþîùè íåôáììï÷ îá ðï÷åòèîïóôé ( 0001) ôïðïìïçéþåóëïçï éúïìñôïòá Bi2 Se3: éóóìåäï÷áîéå ab initio
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535
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PSEUDOSPIN S=1 FORMALISM AND SKYRMION-LIKE EXCITATIONS IN THE THREE-BODY CONSTRAINED EXTENDED BOSE-HUBBARD MODEL
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549
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áîéúïôòïðîùê óðéî-ïòâéôáìøîùê üææåëô ûôáòëá ÷ ëõâéþåóëéè ðïìõðòï÷ïäîéëáè âåú ãåîôòá éî÷åòóéé
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564
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NONEQUILIBRIUM KINETICS OF THE ELECTRON-PHONON SUBSYSTEM OF A CRYSTAL IN A STRONG ELECTRIC FIELD AS A BASE OF THE ELECTROPLASTIC EFFECT
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573
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SURFACE STATES IN A 3D TOPOLOGICAL INSULATOR: THE ROLE OF HEXAGONAL WARPING AND CURVATURE
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584
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óÔÁÔÉÓÔÉÞÅÓËÁÑ, ÎÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ, ÆÉÚÉËÁ <<ÍÑÇËÏÊ ÍÁÔÅÒÉÉ>>
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ëòéôéþåóëéå ôïþëé ðáòï÷ íåôáììï÷
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597
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HEATING A PLASMA BY A BROADBAND STREAM OF FAST ELECTRONS: FAST IGNITION, SHOCK IGNITION, AND Gbar SHOCK WAVE APPLICATIONS
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605
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ïòéåîôáãéïîîáñ äéîáíéëá æåòòïîåíáôéþåóëïçï öéäëïçï ëòéóôáììá ÷ï ÷òáýáàýåíóñ íáçîéôîïí ðïìå
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617
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îåìéîåêîùå ÷ïìîù îá ó÷ïâïäîïê ðï÷åòèîïóôé äéüìåëôòéþåóëïê öéäëïóôé ÷ îáëìïîîïí üìåëôòéþåóëïí ðïìå
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630
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