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1.
A method for obtaining the small current quark mass effect on the dressed quark propagator within the Dyson-Schwinger approach is developed. From this the small current quark mass dependence of the bag constant is evaluated. It is found that the bag constant decreases with the increasing current quark mass and the contribution of the current quark mass cannot be dropped.  相似文献   

2.
A method for obtaining the small current quark mass effect on the dressed quark propagator within the Dyson Schwinger approach is developed. From this the small current quark mass dependence of the bag constant is evaluated. It is found that the bag constant decreases with the increasing current quark mass and the contribution of the current quark mass cannot be dropped.  相似文献   

3.
Based on the global color symmetry mode/ (GCM), a method for obtaining the quark loop effects on the dressed gluon propagator in GCM is developed. In the chiral limit, it is found that the dressed gluon propagator containing the quark loop effects in the Nambu-Goldstone and Wigner phases are quite different. In solving the quark self-energy functions in the two different phases and subsequent study of bag constant one shouM use the above dressed gluon propagator as input. The above approach for obtaining the current quark mass effects on the dressed gluon propagator is quite general and can also be used to calculate the chemical potential dependence of the dressed gluon propagator.  相似文献   

4.
Based on the global color symmetry model (GCM), a method for obtaining the quark loop effects on the dressed gluon propagator in GCM is developed. In the chiral limit, it is found that the dressed gluon propagator containing the quark loop effects in the Nambu-Goldstone and Wigner phases are quite different. In solving the quark self-energy functions in the two different phases and subsequent study of bag constant one should use the above dressed gluon propagator as input. The above approach for obtaining the current quark mass effects on the dressed gluon propagator is quite general and can also be used to calculate the chemical potential dependence of the dressed gluon propagator.  相似文献   

5.
[1]C.D. Roberts and A.G. Williams, Prog. Part. Nucl. Phys.33 (1994) 477, and references therein. [2]P.C. Tandy, Prog. Part. Nucl. Phys. 39 (1997) 117; R.T.Cahill and S.M. Gunner, Fiz. B7 (1998) 17, and references therein. [3]R. Alkofer and L. von Smekal, Phys. Rep. 353 (2001)281; C.S. Fischer and R. Alkofer, Phys. Rev. D67 (2003)094020, and references therein. [4]C.D. Roberts and S.M. Schmidt, Prog. Part. Nucl. Phys.45S1 (2000) 1, and references therein. [5]P. Maris and C.D. Roberts, Int. J. Mod Phys. E12 (2003)297. [6]R.T. Cahill and C.D. Roberts, Phys. Rev. D32 (1985)2419; C.D. Roberts, R.T. Cahill, and J. Praschiflca, Ann.Phys. (N. Y.) 188 (1988) 20. [7]M.R. Frank and T. Meissner, Phys. Rev C57 (1998) 345. [8]P. Maris, C.D. Roberts, and P.C. Tandy, Phys. Lett.B420 (1998) 267. [9]M.R. Frank and T. Meissner, Phys. Rev C53 (1996) 2410. [10]R.T. Cahill and S. Gunner, Phys. Lett. B359 (1995) 281;Mod. Phys. Lett. A10 (1995) 3051. [11]P. Maris and C.D. Roberts, Phys. Rev C56 (1997) 3369. [12]C. Burden, C.D. Roberts, and M. Thomson, Phys. Lett.B371 (1996) 163. [13]C. Burden and D. Liu, Phys. Rev. D55 (1997) 367; M.A.Ivanov, Yu. L. Kalinovskii, P. Maris, and C.D. Roberts,Phys. Lett. B416 (1998) 29; Phys. Rev. C57 (1998) 1991. [14]A. Bender, D. Blaschke, Y. Kalinovskii, and C.D.Roberts, Phys. Rev. Lett. 77 (1996) 3724. [15]M.R. Frank, P.C. Tandy, and G. Fai, Phys. Rev. C43(1991) 2808; M.R. Frank and P.C. Tandy, Phys. Rev. C46(1992) 338; C.W. Johnson, G. Fai, and M.R. Frank, Phys.Lett. B386 (1996) 75. [16]Xiao-Fu L, Yu-Xin Liu, Hong-Shi Zong, and En-Guang Zhao, Phys. Rev. C58 (1998) 1195; Yu-Xin Liu, DongFeng Gao, and Hua Guo, Nucl. Phys. A695 (2001) 353;Yu-Xin Liu, Dong-Feng Gao, and Hua Guo, Phys. Rev.C68 (2003) 035204. [17]C.D. Roberts and R.T. Cahill, Aust. J. Phys. 40 (1987)499. [18]M.R. Frank, Phys. Rev. C51 (1995) 987. [19]T. Meissner and L.S. Kisslinger, Phys. Rev. C59 (1999)986. [20]Hong-Shi Zong, Xiao-Fu Lu, Jian-Zhong Gu, Chao-Hsi Chang, and En-Guang Zhao, Phys. Rev. C60 (1999)055208; Hong-Shi Zong, Xiao-Fu Lui, Fan Wang, Chao-Hsi Chang, and En-Guang Zhao, Commun. Theor. Phys. (Beijing, China) 34 (2000) 563; Hong-Shi Zong, Yu-Xin Liu,Xiao-Fu Lu, Fan Wang, and En-Guang Zhao, Commun.Theor. Phys. (Beijing, China) 36 (2001) 187; Hong-Shi Zong, Xiang-Song Chen, Fan Wang, Chao-Hsi Chang, and En-Guang Zhao, Phys. Rev. C66 (2002) 015201; HongTing Yang, Hong-Shi Zong, Jia-Lun Ping, and Fan Wang,Phys. Lett. B557 (2003) 33; Hong-Shi Zong, Jia-Lun Ping, Hong-Ting Yang, Xiao-Fu Lu, and Fan Wang, Phys.Rev. D67 (2003) 074004; Hong-Shi Zong, Shi Qi, Wei Chen, Wei-Min Sun, and En-Guang, Zhao, Phys. Lett.B576 (2003) 289; Wei-Min Sun, Hong-Shi Zong, XiangSong Chen, and Fan Wang, Phys. Lett. B569 (2003) 211;Hong-Shi Zong, Xiao-Hua Wu, Feng-Yao Hou, and EnGuang Zhao, Chin. Phys. Lett. 21 (2004) 43; Wei-Min Sun, Hong-Shi Zong, Xiang-Song Chen, and Fan Wang,Int. J. Mod. Phys. A19 (2004 261; Hong-Shi Zong, FengYao Hou, Wei-Min Sun, and Xiao-Hua WU, Commun.Theor. Physics. (Beijng, China) 42 (2004) 581. [21]P. Maris and P.C. Tandy, Phys. Rev. C60 (1999) 055214.  相似文献   

6.
A method for obtaining the smallcurrent quark mass dependence of the dressed quark propagator froman effective quark-quark interaction model is developed. Within this approach the small current quark mass effects ondressed-quark propagator have been studied. A comparison with previous results is given.  相似文献   

7.
Based on the rainbow approximation of Dyson-Schwinger equation and the assumption that the full inverse quark propagator at finite chemical potential is analytic in the neighborhood of μ = 1, it is proved that the dressed quark propagator at finite chemical potential μ can be written as G0^-1 [μ] =iγ·p↑-A(p↑-^2) +B(p↑-^2) with p↑-μ= (p↑-p4 +iμ). From the dressed quark propagator at finite chemical potential in Munczek model the bag constant of a baryon and the scalar quark condensate are evaluated. A comparison with previous results is given.  相似文献   

8.
9.
In quantum chromodynamics (QCD), the scalar susceptibility represents the modification of the quark condensate, to a small perturbation of the parameter responsible for the explicit breaking of the symmetry, i.e., the current quark mass. By studying the linear response of the dressed quark propagator to the presence of a nonzero quark mass, we derive a model-independent formula for the scalar susceptibility, which contains the dressed quark propagator G(p) and the dressed scalar vertex F(p, 0). The numerical values of the scalar susceptibility Xs are calculated within the framework of the rainbow-ladder approximation of the Dyson-Schwinger approach by employing two typical forms of model gluon propagator.  相似文献   

10.
We study the quark loop effects on the dressed gluon propagator and also on the quark propagator itself. We find that the gluon propagators are different in two phases. The quark mass effects on the gluon propagator are small but not negligible. We also study the current quark mass dependence on the bag constant.  相似文献   

11.
We study the quark loop effects on the dressed gluon propagator and also on the quark propagator itself. We find that the gluon propagators are different in two phases. The quark mass effects on the gluon propagator are small but not negligible. We also study the current quark mass dependence on the bag constant.  相似文献   

12.
Based on an extensive study of the Dyson-Schwinger equations for a fully dressed quark propagator in the “rainbow” approximation, a parametrized form of the quark propagator is suggested. The corresponding quark self-energy Σf and the structure of non-local quark vacuum condensate <0|:\bar{q}(x)q(0):|0> are investigated. The algebraic form of the quark propagator proposed in this work describes a confining quark propagation, and is quite convenient to be used in any numerical calculations.  相似文献   

13.
According to extensive study of the Dyson-Schwinger equations for a fully dressed quark propagator in the "rainbow" approximation with an effective gluon propagator, a parametrized fully dressed confining quark propagator is suggested in this paper. The parametrized quark propagator describes a confined quark propagation in hadron, and is analytic everywhere in complex p2-plane and has no Lehmann representation. The vector and scalar self-energy functions [1 - Af(p2)] and [Bf(p2) - mf], dynamically running effective mass of quark Mf(p2) and the structure of non-local quark vacuum condensates as well as local quark vacuum condensates are predicted by use of the parametrized quark propagator. The results are compatible with other theoretical calculations.  相似文献   

14.
在彩虹近似下用Dyson Schwinger 方程研究了禁闭夸克的传播子, 得到了夸克动力学质量随动量变化的关系, 即得到了从流夸克质量到组分夸克质量的动力学过渡.  相似文献   

15.
We exhibit a method for obtaining the low chemical potential dependence of the dressed quark propagator from the dressed-quark propagator,which provides a means of determining the behavior of the chiral and deconfinement order parameters.A comparison with the results of previous researches is given.  相似文献   

16.
We exhibit a method for obtaining the low chemical potential dependence of the dressed quark propagatorfrom an effective quark-quark interaction model. Within this approach we explore the chemical potential dependenceof the dressed-quark propagator, which provides a means of determining the behavior of the chiral and deconfinementorder parameters. A comparison with the results of previous researches is given.  相似文献   

17.
In this paper, the gluon propagator in Landau gauge has been studied on a lattice, including the quenched and the unquenched one. The small geometry size of lattice we use is 163×32, and the big one is 203×64. For the quenched approximation, we fit the numerical results and give a little different fitting values. We also obtain unquenched effects by comparing the gluon propagator resulting from the quenched and unquenched configurations, for both the two-flavor and three-flavor cases. For the unquenched configurations, an obvious quark mass dependence has not been found in the small quark mass case, but is found in the three-flavor case when the quark mass is big.  相似文献   

18.
In this paper, the gluon propagator in Landau gauge has been studied on a lattice, including the quenched and the unquenched one. The small geometry size of lattice we use is 16^3 × 32, and the big one is 20^3 × 64. For the quenched approximation, we fit the numerical results and give a little different fitting values. We also obtain unquenched effects by comparing the gluon propagator resulting from the quenched and unquenched configurations, for both the two-flavor and three-flavor cases. For the unquenched configurations, an obvious quark mass dependence has not been found in the small quark mass case, but is found in the three-flavor case when the quark mass is big.  相似文献   

19.
In three-dimensional quantum electrodynamics (QED3) with a massive gauge boson, we investigate the coupled Dyson-Schwinger equations for the fermion and photon propagators in the rainbow approximation, and obtain the critical gauge boson mass for various numbers of the fermion flavors. A comparison with the previous results is presented.  相似文献   

20.
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