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Šú@“ú@F@‚Q‚O‚O‚U”N‚VŒŽ‚Q‚V“ú(–Ø)`‚Q‚X“ú(“y) |
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ƒvƒƒOƒ‰ƒ€(July/20/Ver.3jPDF@ @@ |
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P-01. |
@ácŽR ´•FA‘剮 –ž–¾A¼•À ˆº–çA‰ª–{ “O@PDF |
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Spin polarization and metal-insulator transition in strongly correlated 2D electron systems |
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P-02. |
@²“¡ ‘å•ãAŒü Œ«ˆêA‘ºì ’qA’Ò ‘¾•ãA_Œ´ _A•ŸŽR Š°@PDF |
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Pulsed-NMR studies of Two-dimensional 3He near Localization |
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P-03. |
@’Ò ‘¾•ãA‘ºì ’qAŒü@Œ«ˆêA¼–{ —m•½A_Œ´ _A•ŸŽR Š°@PDF |
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Heat capacity studies of new quantum phases at higher densities than the 4/7 phase in2D 3He on graphite |
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P-04. |
@¼–{ —m‰îA‰Ä–Ú ‹±•½AŽRŒû –¾AΖ{ ‰p•F@PDF |
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Heat capacity measurements of two-dimensional 3He near localization in high magnetic |
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P-05. |
@ˆÀ“c çŽõA‹v•Û Œ’@PDF |
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Spin-Wave Theory of the Multiple-Spin Exchange Model on a Triangular Lattice in aMagnetic Field |
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P-06. |
@ªŠÔ —TŽjA“c’† —SˆêAŽRŒû –¾AΖ{ ‰p•F@PDF |
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Magnetization of 4/7 Phase on 3He or 4He Monolayer Preplated Graphite in high magnetic fields |
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P-07. |
@“ì•” —Y—ºA¬À Œ\‰îA’†’Ò ’mA‘O–ì ‰x‹P@PDF |
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Spin Disordered State in the Quasi-Two-Dimensional Triangular AntiferromagnetNiGa2S4 |
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P-08. |
@¬À Œ\‰îA“ì•” —Y—ºA’†’Ò ’mAâˆä CA“a‘º GŽjA‘O–ì ‰x‹P@PDF |
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Single Crystal Study of S = 1 Heisenberg Triangular Antiferromagnet NiGa2S4 |
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P-09. |
@¬À Œ\‰îA’†’Ò ’mA‘O–ì ‰x‹P |
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A S = 3/2 Quasi-Two-Dimensional Ferromagnet |
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P-10. |
@Š}Œ´ •áA‹{ì ˜a–çA´… NOAŽ–ì“c ˆêŽi@PDF |
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Unconventional behavior of superconductivity near a spin liquid phase |
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P-11. |
@‰F“cì «•¶A‹ K”N@PDF |
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Suppression of horizontal charge ordering and coexistence of short-range chargemodulations in \theta-(BEDT-TTF)2MM'(SCN)4 |
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P-12. |
@’¬“c —mA’†’Ò ’mA‘O–ì ‰x‹PA“cŽR FA匴 r˜Y@PDF |
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Spin Liquid Behavior and Anomalous Hall Effect of the Frustrated Kondo Lattice Pr2Ir2O7 |
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P-13. |
@“c’† F‰ÀA”ª’J ‘S“TA²X–Ø –LA…è —²—Y@PDF |
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Magnetic Domain Structure of Nuclear Ordered Solid Helium 3 |
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P-14. |
@‰ª–{ ‰ÀŽqA‘匩 “N‹@PDF |
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Spin wave and Sound in High Field Phase of Solid 3He |
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P-15. |
@ˆøŒ´ rÆ@PDF |
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Effects of magnetic field in two-leg spin ladder with ring exchanges |
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P-16. |
@–쑺 ´‰pA•Iˆä ŒhŒá@PDF |
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Universality class of S=1/2 quantum spin ladder systems with four-spin exchange |
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P-17. |
@‚“‡ M–çA’|‰º ’¼AŽ›‘q çŒbŽqA–쌴 ŽÀA‚–Ø ‰p“T@PDF |
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Pressure?effect?on?NiS2?-?Mott?critical?point?and?quantum?critical?point |
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P-18. |
@‘å‹´ ‘ô–A“ˆä •×Aìã ‘¥—YA펟 Gˆê@PDF |
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Cellular dynamical mean field study of Mott transition in triangular lattice Hubbard model |
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P-19. |
@¥í —²A‹ K”NAŒÃè º@PDF |
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Metal-Insulator transition in the two-dimensional Hubbard model on an anisotropictriangular lattice |
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P-20. |
@ˆî—t Œª‰îAŒÃ‰ê ¹‹vA›½ ˆê˜YAìã ‘¥—Y@PDF |
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The effect of orbital fluctuations on the Mott transitions in the multiorbital Hubbardmodel |
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P-21. |
@“n•Ó ^mA¡“c ³rAŽO‘î ˜a³@PDF |
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Electronic states near quantum critical points of valence transition |
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P-22. |
@ŠÛŽR ŒMA‰ŠL ˆÀO@PDF |
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Quantum Phase Transition in Quasi one dimensional Strongly Correlated ElectronSystems with Interchain Hopping |
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P-23. |
@•š‰® —Y‹I@PDF |
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Effect of the dimensionality in spin- and superconducting-fluctuations |
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P-24. |
@ˆ¢•” —zAã“c “NlA–쑺 —³ŽiA‰œ“c —Yˆê@PDF |
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Interface Motion and Nucleation of 4He Crystal Induced by Acoustic Wave |
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P-25. |
@ˆ¢•” —zAã“c “NlA–쑺 —³ŽiA‰œ“c —Yˆê@PDF |
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Faraday Instability on solid-liquid interface of 4He |
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July/19/2006FƒAƒuƒXƒgƒ‰ƒNƒgŒfÚ |
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¨uŒ¤‹†‰ïvˆÄ“àƒy[ƒW‚Ö@ |