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q = 6 state vector Potts model phase transition properties of
】 Basis _l mouth 2 +; 4R4 b \l +21 _21l +3 llu, 【2 21 + \l +2 \R = \+4 l +4 Port 2 \】 【2】 +2 U11 +22】 2 \Document:: 1: POTTSPB. . Animprovedur. xtelinlatticecaugetheory, ProcZJ] CambridgePhilosSee, 1952 (4 : 106127.2] WUFYThepott8modd [JRex,ugg boots günstig, ModPhys, 1982 (54): 2352673] HEXH, xlANDC, SONGYXAnimprovedvaria-tionaltreatmentoflatticegaugethmfies [J'PhysLettB, 1985,tory burch shoes,153 (6),, 417 - 421 [4] ZHENGXT, CHEN. rL,stivali ugg, xlANDCOnfurtherimprovenaentofthevariationaltner [~-dinlatticegaugethe a ([JPhysLettB, 1985.154:166172 [5] WUCM.ZHAOPYThephasestructureofZ (N) latricegaugetheorieyvariationalcumulantexpansion [JConmmnTheorPhys, t991). 13:393-404 【6] YANGJMSecondorderphasetransitiOIL ~ inZ {2) gaagetheorybyvariationalcumulantexpansion [JCA) InF [IUt] TheorPh, vs. 1990,ugg stivali,14:111-118 [7JANGLI: ~ qG-XIN, CHENTlAN-LUNVariationalcumulantexpansionOnSU (2) xSU (2) chiraln ~ xlel [J] CommunTheorPhys, 1994,21 (3): 341348 [8: MAWJ, CHENTLVariational-cumulantexpansiononthefive- stateclockntodel [J]. 0munTheorPh, I993, 20:171180 [9TOBGCHNIKJPropertiesoftheq-stateclock Ⅻ) [】 dfor = 45, and6l 【¨ PhvsRex, B. 1982,26:6201621110 ISONGYX, DAIYBA mouth Ⅲ schemeforenumeradt ~ goonnecteddiagramsonthelattice [J] JMathPh ,tory burch,1990,61:2015-2026. [Editor: Li Ling Chu]
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