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