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ÈÍÔÎÐÌÀÖÈÎÍÍÛÉ ÁÞËËÅÒÅÍÜ «ÑÒÀÒÜÈ» No.46 21.11.2011 |
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Ñ 133.2 ÓÐÀÂÍÅÍÈß ÌÀÒÅÌÀÒÈ×ÅÑÊÎÉ ÔÈÇÈÊÈ. |
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1.Biktashev, V.N. Envelope Quasisolitons in Dissipative Systems with
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// Physical Review Letters.-2011.-Vol.107, No.13.-p.134101 .- Bibliogr.:13. |
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2.Filipuk, G. Generalized Hypergeometric Systems and the Fifth and Sixth Painleve Equations/ G.Filipuk
// Buletinul Academiei de
Stiinte a Republicii |
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4.Kobayashi, T. Low-Frequency Spin
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Ñ 138 ÃÅÎÌÅÒÐÈß. ÐÈÌÀÍÎÂÀ ÃÅÎÌÅÒÐÈß.
ÃÅÎÌÅÒÐÈß ËÎÁÀ×ÅÂÑÊÎÃÎ |
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Ñ 17 ÂÛ×ÈÑËÈÒÅËÜÍÀß ÌÀÒÅÌÀÒÈÊÀ. |
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6.Cabral, E.D. Electrical Control of
Magnetic Quantum Wells: |
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7.Furmaniak, S. The Influence of the Carbon
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9.Li, J. Diffusive Molecular Dynamics
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// Physical Review B.-2011.-Vol.84, No.5.-p.054103 .- Bibliogr.:30. |
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10.Mahmud,
K.W. Finite-Temperature Study of Bosons in a Two-Dimensional Optical Lattice/
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Ñ 322 ÒÅÎÐÈß ÎÒÍÎÑÈÒÅËÜÍÎÑÒÈ |
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13.Duplantier,
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16.Liu,
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18.Wojtak,
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19.Zheng,
S. From Supercurrents to Soft Terms/ S.Zheng, J.-H.Huang // Modern
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Ñ 323 ÊÂÀÍÒÎÂÀß ÌÅÕÀÍÈÊÀ |
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20.Berninger,
M. Universality of the Three-Body Parameter for Efimov
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21.Boyko,
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22.Castagnino,
M. New Bases for a General Definition for the Moving Preferred Basis/ M.Castagnino, S.Fortin //
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23.Mulken,
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Ñ 323.1 ÐÅËßÒÈÂÈÑÒÑÊÈÅ ÂÎËÍÎÂÛÅ
ÓÐÀÂÍÅÍÈß. ÓÐÀÂÍÅÍÈß ÒÈÏÀ ÁÅÒÅ-ÑÎËÏÈÒÅÐÀ. ÊÂÀÇÈÏÎÒÅÍÖÈÀË. |
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Ñ 323.2 ÇÀÊÎÍÛ ÑÎÕÐÀÍÅÍÈß È ÎÁÙÈÅ ÒÅÎÐÈÈ
ÐÅÀÊÖÈÉ. ÏÎËßÐÈÇÀÖÈÎÍÍÛÅ ÝÔÔÅÊÒÛ. ÈÍÂÀÐÈÀÍÒÍÎÅ ÐÀÇËÎÆÅÍÈÅ ÀÌÏËÈÒÓÄ |
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28.Iltan,
E.O. The Effect of Antisymmetric Tensor Unparticle Mediation on the Charged Lepton Electric
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G.-2011.-Vol.38, No.10.-p.105001 .- Bibliogr.:21. |
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29.Song,
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// Physical Review C.-2011.-Vol.84, No.2.-p.025501 .-
Bibliogr.:28. |
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Ñ 323.5 ÒÅÎÐÈß ÂÇÀÈÌÎÄÅÉÑÒÂÈß ×ÀÑÒÈÖ ÏÐÈ
ÂÛÑÎÊÈÕ ÝÍÅÐÃÈßÕ |
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30.Adeluyi,
A. Gluon Distributions in Nuclei Probed at Energies Available at the CERN
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Physical Review C.-2011.-Vol.84, No.2.-p.024916 .- Bibliogr.:46. |
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31.Becchi,
C.M. An Off-Shell IR Regularization Strategy in the Analysis of Collinear
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// Journal of Physics G.-2011.-Vol.38, No.10.-p.105004 .-
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32.Bluhm,
M. Shear and Bulk Viscosities of the Gluon Plasma in a Quasiparticle
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33.Kirkpatrick, J.M. Measurement
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34.Mohanty,
P. Evolution of Collectivity as a Signal of Quark Gluon Plasma Formation in
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Ñ 324 ÊÂÀÍÒÎÂÀß ÒÅÎÐÈß ÏÎËß |
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35.Antipin,
O. Constraints on Conformal Windows from Holographic Duals/ O.Antipin, K.Tuominen // Modern
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36.Arias,
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37.Giacosa,
F. Deviation from the Exponential Decay Law in Relativistic Quantum Field
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A.-2011.-Vol.26, No.30.-p.2247-2259 .- Bibliogr.:32. |
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Ñ 324.1ã ÊÀËÈÁÐÎÂÎ×ÍÛÅ ÒÅÎÐÈÈ ÏÎËß. ÑÏÎÍÒÀÍÍÎ-ÍÀÐÓØÅÍÍÛÅ
ÑÈÌÌÅÒÐÈÈ.ÌÎÄÅËÈ ÂÅËÈÊÎÃÎ ÎÁÚÅÄÈÍÅÍÈß |
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38.Khanna,
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39.Vyas,
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Ñ 324.1ä ÊÂÀÍÒÎÂÀß ÕÐÎÌÎÄÈÍÀÌÈÊÀ |
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40.Blanquier,
E. Standard Particles in the SU(3) Nambu-Jona-Lasinio
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41.Kim,
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43.Nahrgang,
M. Nonequilibrium Chiral
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44. |
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45.Pastore,
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46.Stoffers,
A. *g * *g * *> *p*0 Form Factor from Anti-de Sitter-Space/QCD
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// Physical Review C.-2011.-Vol.84, No.2.-p.025202 .- Bibliogr.:29. |
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Ñ 324.2 ÍÅËÎÊÀËÜÍÛÅ È ÍÅËÈÍÅÉÍÛÅ ÒÅÎÐÈÈ
ÏÎËß. ÒÅÎÐÈÈ Ñ ÂÛÑØÈÌÈ ÏÐÎÈÇÂÎÄÍÛÌÈ. ÒÅÎÐÈß Ñ ÈÍÄÅÔÈÍÈÒÍÎÉ ÌÅÒÐÈÊÎÉ |
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47.Avgoustidis,
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48.Blumenhagen,
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Ñ 324.3 ÀÊÑÈÎÌÀÒÈ×ÅÑÊÀß ÒÅÎÐÈß ÏÎËß. ÀÍÀËÈÒÈ×ÅÑÊÈÅ
ÑÂÎÉÑÒÂÀ ÌÀÒÐÈ×ÍÛÕ ÝËÅÌÅÍÒÎÂ È ÄÈÑÏÅÐÑÈÎÍÍÛÅ ÑÎÎÒÍÎØÅÍÈß |
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49.Grange,
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Ñ 325 ÑÒÀÒÈÑÒÈ×ÅÑÊÀß ÔÈÇÈÊÀ È ÒÅÐÌÎÄÈÍÀÌÈÊÀ
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50.Ayre,
G.N. On the Mechanism of Carbon Nanotube Formation:
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52.Billoire,
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56.Dupertuis,
M.A. Symmetries and the Polarized Optical Spectra of Exciton
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57.Goswami,
P. Effects of the Berry Phase and Instantons in
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59.Kaul,
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M. Energetics and Structure of Organic Molecules
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J. Surface Self-Diffusion Behavior of Individual Tungsten Adatoms
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Ñ 326 ÊÂÀÍÒÎÂÀß ÒÅÎÐÈß ÑÈÑÒÅÌ ÈÇ ÌÍÎÃÈÕ
×ÀÑÒÈÖ. ÊÂÀÍÒÎÂÀß ÑÒÀÒÈÑÒÈÊÀ |
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74.Bettelheim,
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J.J. Superfluid Vortex Front at T*>0: Decoupling
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86.Qi,
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106.Tavazza,
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Ñ 332 ÝËÅÊÒÐÎÌÀÃÍÈÒÍÛÅ ÂÇÀÈÌÎÄÅÉÑÒÂÈß |
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110.Giordano,
V.M. Inelastic x-Ray Scattering Study of Liquid Ga:
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113.Wegner,
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Ñ 341 ÀÒÎÌÍÛÅ ßÄÐÀ |
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116.Brida,
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118.Nortershauser,
W. Charge Radii and Ground State Structure of Lithium Isotopes: Experiment
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122.Van Dalen, E.N.E. Relativistic Description of Finite Nuclei
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Ñ 341 à
ÐÀÇËÈ×ÍÛÅ ÌÎÄÅËÈ ßÄÅÐ. |
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125.Adamian, G.G. Behavior of One-Quasiparticle Levels in Odd Isotonic Chains of Heavy
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128.Gambacurta,
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129.Giannatiempo,
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130.Inci,
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131.Jia,
L.Y. Generalized Density Matrix Reexamined: Microscopic Approach to
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132.Jolos,
R.V. Parity Splitting and E1/E2 Branching in the Alternating Parity Band of
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133.Kanada-En'yo,
Y. Proton Dominance in the 2*+&sub(2) *> 0*+&sub(1) Transition of
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Ñ 341 à1
ÌÀÒÅÌÀÒÈ×ÅÑÊÈÅ ÌÅÒÎÄÛ Â ÒÅÎÐÈÈ ßÄÐÀ. |
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136.Abramkina,
V. Quadrupole Collectivity in the Two-Body Random
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Ñ 341 à2
ÃÈÃÀÍÒÑÊÈÅ ÐÅÇÎÍÀÍÑÛ. |
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137.Daoutidis,
I. Impact of the Nuclear Symmetry Energy on the Pygmy Dipole Resonance/ I.Daoutidis, S.Goriely //
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138.Inakura,
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139.Savran,
D. Fragmentation and Systematics of the Pygmy
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Ñ 341 å ßÄÅÐÍÀß ÀÑÒÐÎÔÈÇÈÊÀ./ñì.òàêæå Ñ 63/ |
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140.Matic,
A. High-Precision *2*8Si(p, t)*2*6Si Reaction to Determine *2*2Mg(*a,
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Ñ 341.1 ÐÀÄÈÎÀÊÒÈÂÍÎÑÒÜ |
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141.Concharov,
M. Probing the Nuclides *1*0*2Pd, *1*0*6Cd, and *1*4*4Sm for Resonant Neutrinoless Double-Electron Capture/ M.Concharov,
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142.Flechard,
X. Measurement of the *b-*n Correlation Coefficient a&sub(*b*n)
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143.Grigorenko, L.V. Two-Neutron
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144.Huber,
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145.Raduta,
C.M. Description of the 2*n*n*b*b Decay Within a Gauge Restored of a Fully
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146.Santhosh,
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147.Scott,
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148.Zhang,
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Ñ 341.2 ÑÂÎÉÑÒÂÀ ÀÒÎÌÍÛÕ ßÄÅÐ |
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149.Bhowall,
S. Development of Collective Structures Over Noncollective
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150.Fortune,
H.T. The Puzzle of *3*2Mg/ H.T.Fortune // Physical
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151.Heusler,
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152.Hwang,
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B.P. Single-Neutron Energies Outside *1*3*6Xe/ B.P.Kay,
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154.Mane,
E. Ground-State Spins and Moments of &sup(72,74,76,78)Ga
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157.Procter,
M.G. Lifetime Measurements in the Transitional Nucleus *1*3*8Gd/ M.G.Procter, [a.o.] // Physical
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158.Sheng,
Z. Systematic Calculations on Cluster Radioactivity Half-Lives/ Z.Sheng, [a.o.] // Journal of
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159.Singh,
P. Highly Deformed High-Spin Band in *1*2*5I/ P.Singh,
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160.Zimmerman,
W.R. Further Evidence for the Broad 2*+&sub(2)
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Ñ 341.3 ÄÅËÅÍÈÅ ßÄÅÐ |
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161.Younes,
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Ñ 342 ÏÐÎÕÎÆÄÅÍÈÅ ×ÀÑÒÈÖ È ÃÀÌÌÀ-ÊÂÀÍÒÎÂ
×ÅÐÅÇ ÂÅÙÅÑÒÂÎ |
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162.Schwartz,
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Ñ 342 ã2
ÂÇÀÈÌÎÄÅÉÑÒÂÈÅ ÍÅÉÒÐÎÍÎÂ Ñ ÊÎÍÄÅÍÑÈÐÎÂÀÍÍÛÌÈ ÑÐÅÄÀÌÈ. ÌÀÃÍÈÒÍÛÅ ÂÇÀÈÌÎÄÅÉÑÒÂÈß. |
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163.Baidya,
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164.Brown,
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165.Kim,
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166.Panarin, J. Effects of
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167.Xu,
Z. Local-Moment Magnetism in Superconducting FeTe&sub(0.35)Se&sub(0.65) as Seen Via Inelastic Neutron
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Ñ 342 ã3 ÓËÜÒÐÀÕÎËÎÄÍÛÅ ÍÅÉÒÐÎÍÛ. |
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168.Zimmer,
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Ñ 343 ßÄÅÐÍÛÅ ÐÅÀÊÖÈÈ |
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169.Arai,
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170.Giusti,
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171.Hager,
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173.Sakaguchi,
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174.Uddin,
M.S. Formation of the Isomeric Pair *1*9*4Ir&sup(m,g)
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Ñ 343 à ÒÅÎÐÈß
ßÄÅÐÍÛÕ ÐÅÀÊÖÈÉ. ÐÀÇËÈ×ÍÛÅ ÌÎÄÅËÈ: ÑÒÀÒÈÑÒÈ×ÅÑÊÀß, ÎÏÒÈ×ÅÑÊÀß, ÐÅÇÎÍÀÍÑÍÀß |
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175.Aritomo,
Y. Dynamical Model of Surrogate Reactions/ Y.Aritomo,
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176.Sharma,
M.K. Fusion Excitation Functions of *6*4Ni+&sup(112-132)Sn Reactions Studied on the Dynamical Cluster-Decay
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177.Yarmukhamedov, R. Connection
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Ñ 343 à2 ÒÅÎÐÈß
ßÄÅÐÍÛÕ ÐÅÀÊÖÈÉ ÏÐÈ ÂÛÑÎÊÈÕ ÝÍÅÐÃÈßÕ (Å>1ÃÝÂ) |
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178.Berz,
B. Fourier Harmonics of High-p&sub(T) Particles
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179.Chaudhuri,
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Ñ 343 å ßÄÅÐÍÛÅ ÐÅÀÊÖÈÈ Ñ ÒßÆÅËÛÌÈ ÈÎÍÀÌÈ
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Ñ 344.1 ÌÅÒÎÄÛ È ÀÏÏÀÐÀÒÓÐÀ ÄËß
ÐÅÃÈÑÒÐÀÖÈÈ ÝËÅÌÅÍÒÀÐÍÛÕ ×ÀÑÒÈÖ |
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201.Fasoli, M. Band-Gap
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Ñ 344.4á ÌÅÒÎÄÛ ÏÐÈÃÎÒÎÂËÅÍÈß ÒÎÍÊÈÕ
ÏËÅÍÎÊ. |
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202.Chaudhuri,
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Ñ 345 ÓÑÊÎÐÈÒÅËÈ ÇÀÐßÆÅÍÍÛÕ ×ÀÑÒÈÖ |
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209.Lassagne,
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Ñ 346 ÝËÅÌÅÍÒÀÐÍÛÅ ×ÀÑÒÈÖÛ |
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210.Abazov,
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Ñ 346.1 ÍÅÉÒÐÈÍÎ |
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216.De Barros, N.F. Solar Neutrino-Electron Scattering as
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Ñ 346.2 ÍÓÊËÎÍÛ È ÀÍÒÈÍÓÊËÎÍÛ |
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218.Ayala, A. Three-Hadron Angular Correlations in High-Energy Proton-Proton
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Ñ 346.3 *m-ÌÅÇÎÍÛ |
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223.Sugiyama, J. Magnetic and
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Ñ 346.4 *p-ÌÅÇÎÍÛ |
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224.Abreu,
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Ñ 346.5 Ê-ÌÅÇÎÍÛ È ÃÈÏÅÐÎÍÛ |
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225.Caruso,
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Ñ 346.6 ÐÅÇÎÍÀÍÑÛ È ÍÎÂÛÅ ×ÀÑÒÈÖÛ |
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227.Flambaum,
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Ñ 349.1 ÄÅÉÑÒÂÈÅ ÈÇËÓ×ÅÍÈÉ ÍÀ ÌÀÒÅÐÈÀËÛ. |
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228.Mani, R.G. Observation of
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Ñ 350 ÏÐÈËÎÆÅÍÈß ÌÅÒÎÄΠßÄÅÐÍÎÉ ÔÈÇÈÊÈ Â
ÑÌÅÆÍÛÕ ÎÁËÀÑÒßÕ |
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230.Athalye,
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231.Horsewill,
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232.Lue,
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233.Sakai, H.
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234.Sauer,
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Ñ 353 ÔÈÇÈÊÀ ÏËÀÇÌÛ |
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236.Killer,
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Ñ 393 ÔÈÇÈÊÀ ÍÈÇÊÈÕ ÒÅÌÏÅÐÀÒÓÐ |
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239.Casula,
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240.Garate,
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Ñ 393 è ÂÛÑÎÊÎÒÅÌÏÅÐÀÒÓÐÍÀß
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245.Muniz, R.A. Method for
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Ö 841 ÝËÅÊÒÐÎÍÍÛÅ ÖÈÔÐÎÂÛÅ ÂÛ×ÈÑËÈÒÅËÜÍÛÅ
ÌÀØÈÍÛ |
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249.Yoshida,
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Ö 846 ÎÏÒÈÊÎ-ÝËÅÊÒÐÎÍÍÛÅ
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