Calculation on U(1) Lattice Gauge Theory at Finite Temperature

ZHENG Xi-Te; REN Xue-Zao

Chinese Physics C> 1993, Vol. 17> Issue(2) : 134-139

Calculation on U(1) Lattice Gauge Theory at Finite Temperature

ZHENG Xi-Te ^, ,
REN Xue-Zao

Department of Physics,Chengdu University of Science and Technology,610065Department of Physics,Xichang Teacher's College,Sichuan,615022

Abstract
HTML
Reference
Related

PDF

Abstract：
The order parameter for the U(1) lattice gauge model at finite temperature with N_{τ_{=1 is calculated by using the variational-cumulant expansion method.The result is in agreement with the Monte Carlo simulations.The specific simplification in the case of N_{τ_{=1 is discussed.The relationship between the variational method and the accumulation point method for determing the parameters introduced into the cumulant expansion is clarified.}}}}

References

[1]

B. Svetitsky, Phys. Rep., 132(1936), 1.[2]X. T. Zheng and C.-1 Tan, Chinese Phys. Lett., 5(1988), 457. C.-I Tan and X. T. Zheng, Phys. Rev. D39(1989), 623.[3]郑希特,刘备书,高能物理与核物理.14(1990),892,[4]X. T. Zheng, C.-I Tan and T. L. Chen, Phys. Rev., D26(1982), 2843.[5]W. Kerler, Phys. Rev. Get:., 60(1988), 1906. W. Kerler and L. Schulke, Phys. Lett., B201(1988), 123.[6]王杰、谭祖国、郑希特,高能物理与核物理,12(1938),329,[7]N. Bilic, H. Gansterer and S. Sanielevici, Phys,Lett.,B193(1987), 35.

[1]	JIANG Jun-Qin . Third Order Result of the 0++ Glueball Wave Function for U(1) Improved Lattice Gauge Theory in Three-Dimensions. Chinese Physics C, 2005, 29(5): 447-450.
[2]	JIANG Jun-Qin . Mass Gap and Glueball Wave Function for U(1) Improved Lattice Gauge Theory in Three-Dimensions. Chinese Physics C, 2005, 29(2): 115-118.
[3]	LIU Jin-Ming , LI Jie-Ming , GUO Shuo-Hong . Glueball Mass in Improved SU(3) Lattice Hamiltonian in 2+1 Dimensional. Chinese Physics C, 2001, 25(5): 383-387.
[4]	JIANG JunQin . Study of the Vacuum State for 2+1 Dimensional SU(2) Lattice Gauge Field Theory. Chinese Physics C, 2000, 24(10): 922-926.
[5]	Jiang Junqin , Luo Xiangqian . Calculation of the Vector Meson Mass in 1+1 Dimensional Lattice QCD by Using the Improved Hamiltonian. Chinese Physics C, 1999, 23(7): 644-649.
[6]	Jiang Junqin , Luo Xiangqian , Guo Shuohong , Liu Jinming . Calculation of the Vacuum Wave Function in 2+1 Dimensional U(1) Gauge Theory by Using the Improved Lattice Hamiltonian. Chinese Physics C, 1999, 23(12): 1152-1157.
[7]	Ren Xuezao , Zhu Yunlun , Chen Ying . Analytical study of Lattice U(1) and U(1)-Higgs Models at Finite Temperature With Symanzik Action. Chinese Physics C, 1998, 22(6): 492-498.
[8]	Wu Jimin . A Discussion About Recent Numerical Results From the Calculation of the Glueball Masses on Lattice Gauge Theory. Chinese Physics C, 1996, 20(10): 894-899.
[9]	Liu Wensheng , Cui Jianying , Yang Jinmin , Wan Lingde . The Phase Tansitions in Abelian Lattice Gauge Theories at Finite Temperature:An Analytical Analysis. Chinese Physics C, 1994, 18(11): 996-1002.
[10]	SHEN Kun , QIU Zhongping . Vertex Correction at Finite Temperature and Decoupling Transition in (2+1) Dimensional Chiral Gross-Neveu Model. Chinese Physics C, 1993, 17(11): 993-1001.
[11]	ZHENG Xi-Te , LIU Bei-Shu . ANALYTICAL TREATMENT OF SU(2)-HIGGS SYSTEM ON LATTICE AT FINITE TEMPERATURE. Chinese Physics C, 1990, 14(10): 892-899.
[12]	ZHENG Bo , GUO Shuo-Hong . A SOLVABLE (1+1)-DIMENSIONAL LATTICE U(1) GAUGE MODEL. Chinese Physics C, 1990, 14(3): 282-285.
[13]	ZHENG Wei-Hong , GUO Shuo-Hong . THE VARIATIONAL CALCULATION OF MASS GAP IN 2+1 DIMENSIONAL SU(2) LGT. Chinese Physics C, 1989, 13(1): 83-86.
[14]	LUO Xiang-Qian , CHEN Qi-Zhou , GUO Shuo-Hong . VACUUM OF 2+1 DIMENSIONAL SU(2) LGT WITH FERMIONS AND SPONTANEOUS CHIRAL SYMMETRY BREAKING. Chinese Physics C, 1989, 13(4): 328-333.
[15]	WANG Jie , YAN Zu-Guo , ZHENG Xi-Te . ANALYTICAL STUDY OF U(1)-HIGGS SYSTEM ON A LATTICE. Chinese Physics C, 1988, 12(3): 329-335.
[16]	LIU Jin-Ming , ZHENG Wei-Hong , GUO Shuo-Hong . THE MASS GAP IN 2+1 DIMENSIONAL SU(3) LATTICE CAUGE THEORY. Chinese Physics C, 1988, 12(3): 420-424.
[17]	WU Ji-Min , ZHAO Pei-Ying . ANALYTIC CALCULATION FOR GLUON CONDENSATION IN SU (2) LATTICE GAUGE THEORY. Chinese Physics C, 1987, 11(1): 64-67.
[18]	CHEN Hao , GUO Shuo-Hong . ADLER-BELL-JACKIW ANOMALY IN LATTICE GAUGE THEORY. Chinese Physics C, 1986, 10(6): 666-676.
[19]	LIU Jin-Ming , ZHENG Bo , GUO Shuo-Hong . QUARK MASS RENORMALIZATION IN LATTICE GAUGE THEORY (Ⅱ) BARYON MASS CALCULATION. Chinese Physics C, 1986, 10(1): 116-119.
[20]	WANG Qin-Mou . THERMODYNAMICAL PROPERTIES OF GAUGE THEORIES AT FINITE TEMPERATURE AND CHEMICAL POTENTIAL. Chinese Physics C, 1986, 10(1): 24-31.

Access

Get Citation

ZHENG Xi-Te and REN Xue-Zao. Calculation on U(1) Lattice Gauge Theory at Finite Temperature[J]. Chinese Physics C, 1993, 17(2): 134-139.

ZHENG Xi-Te and REN Xue-Zao. Calculation on U(1) Lattice Gauge Theory at Finite Temperature[J]. Chinese Physics C, 1993, 17(2): 134-139. shu

RIS(for EndNote,Reference Manager,ProCite)

BibTex

Txt

Milestone

Received: 1900-01-01
Revised: 1900-01-01

Article Metric

Article Views(2889)
PDF Downloads(511)
Cited by(0)

Policy on re-use

To reuse of subscription content published by CPC, the users need to request permission from CPC, unless the content was published under an Open Access license which automatically permits that type of reuse.

通讯作者: 陈斌, bchen63@163.com

1.
沈阳化工大学材料科学与工程学院沈阳 110142

Calculation on U(1) Lattice Gauge Theory at Finite Temperature

ZHENG Xi-Te ^,
REN Xue-Zao

Corresponding author: ZHENG Xi-Te,

Department of Physics,Chengdu University of Science and Technology,610065Department of Physics,Xichang Teacher's College,Sichuan,615022

Received Date: 1900-01-01
Accepted Date: 1900-01-01
Available Online: 1993-02-05

Abstract: The order parameter for the U(1) lattice gauge model at finite temperature with N_{τ_{=1 is calculated by using the variational-cumulant expansion method.The result is in agreement with the Monte Carlo simulations.The specific simplification in the case of N_{τ_{=1 is discussed.The relationship between the variational method and the accumulation point method for determing the parameters introduced into the cumulant expansion is clarified.}}}}