Calculation of Anomalous Dimension of Three-Gluon Tensor Operators

DUAN HuaiYu; LIU JuePing

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《中国物理C》（英文）编辑部

2024年10月30日

Chinese Physics C> 2000, Vol. 24> Issue(7) : 642-648

Calculation of Anomalous Dimension of Three-Gluon Tensor Operators

DUAN HuaiYu ^, ,
LIU JuePing

Department of Physics,Wuhan University,Wuhan 430072,China

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Abstract：
The renormalization coefficient matrix and anomalous dimension matrix of two three gluon tensor operator Ωαβ1=Gαa,μ Gμb,ν Gνβc f_abc and Ωαβ2=gαβ Gσa,μ Gμb,v Gνc,σ f_abc,which are closely related to the glueball current operator with quantum number J^PC=1^－+, were calculated. The divergent terms of amputated three point Green function of Ωαβi (nonzero momentum transfer) in Lorentz gauge were calculated explicitly up to g2s order,and no other gauge invaraiant operators were found to mix with them. Defining αβ1=Ωαβ 1-14Ωαβ2, the physical part of renormalization coefficient matrix of αβ1 in minimum subtraction scheme with space dimension D=4+2 is Z1=1+g 2s C A(4 π)276+O(g4s). The Physical part of anomalous dimension matrix of αβ1 is gauge invariant, and γ1=g2 sCA(4π)273

References

[1]	. Wilson K G .Phys.Rev.,196 9,197:14 992. LU WenTao,LIU JuePing.Chin .Phys.Lett.,1996 ,13:3403. Joglekar S D ,Lee B W .Ann.Phys.,1976 ,97:16 04. Collins J C .Renormalization.,NewYork :Cambridge University Press,1984 .316

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[17]	WU Hua-Chuan . THE QUADRUPOLE OPERATOR IN s-d-g MODEL AND THE SPECTRUM OF DEFORMED NUCLEI. Chinese Physics C, 1986, 10(6): 715-719.
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[20]	LI ZI-PING . APPROXIMATE SEQUENCE FOR U（t,t₀）-OPERATOR. Chinese Physics C, 1979, 3(4): 511-517.

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DUAN HuaiYu and LIU JuePing. Calculation of Anomalous Dimension of Three-Gluon Tensor Operators[J]. Chinese Physics C, 2000, 24(7): 642-648.

DUAN HuaiYu and LIU JuePing. Calculation of Anomalous Dimension of Three-Gluon Tensor Operators[J]. Chinese Physics C, 2000, 24(7): 642-648. shu

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Received: 1999-06-24
Revised: 1900-01-01

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沈阳化工大学材料科学与工程学院沈阳 110142

Calculation of Anomalous Dimension of Three-Gluon Tensor Operators

DUAN HuaiYu ^,
LIU JuePing

Corresponding author: DUAN HuaiYu,

Department of Physics,Wuhan University,Wuhan 430072,China

Received Date: 1999-06-24
Accepted Date: 1900-01-01
Available Online: 2000-07-05

Abstract: The renormalization coefficient matrix and anomalous dimension matrix of two three gluon tensor operator Ωαβ1=Gαa,μ Gμb,ν Gνβc f_abc and Ωαβ2=gαβ Gσa,μ Gμb,v Gνc,σ f_abc,which are closely related to the glueball current operator with quantum number J^PC=1^－+, were calculated. The divergent terms of amputated three point Green function of Ωαβi (nonzero momentum transfer) in Lorentz gauge were calculated explicitly up to g2s order,and no other gauge invaraiant operators were found to mix with them. Defining αβ1=Ωαβ 1-14Ωαβ2, the physical part of renormalization coefficient matrix of αβ1 in minimum subtraction scheme with space dimension D=4+2 is Z1=1+g 2s C A(4 π)276+O(g4s). The Physical part of anomalous dimension matrix of αβ1 is gauge invariant, and γ1=g2 sCA(4π)273