Hadrons from a hard wall AdS/QCD model

Chul Kim; Youngman Kim

doi:10.1088/1674-1137/34/9/089

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《中国物理C》（英文）编辑部

2024年10月30日

Chinese Physics C> 2010, Vol. 34> Issue(9) : 1520-1522 DOI: 10.1088/1674-1137/34/9/089

Hadrons from a hard wall AdS/QCD model

Chul Kim ^, ,
Youngman Kim

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Abstract：
We review a recent work on masses of mesons and nucleons within a hard wall model of holographic QCD in a unified approach. In order to treat meson and nucleon properties on the same footing, we introduced the same infrared (IR) cut for both sectors. In framework of present approach, the best fit to the experimental data is achieved introducing the anomalous dimension for baryons.

References

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. Maldacena J M. Adv. Theor. Math. Phys., 1998, 2: 231-2522. Gubser S S, Klebanov I R, Polyakov A M. Phys. Lett. B,1998, 428: 105-1143. Witten E. Adv. Theor. Math. Phys., 1998, 2: 253-2914. Erdmenger J, Evans N, Kirsch I, Threlfall E. Eur. Phys. J.A, 2008, 35: 81-1335. Erlich J, Katz E, Son D T, Stephanov M A. Phys. Rev.Lett., 2005, 95: 261602(4)6. Rold D L, Pomarol A. Nucl. Phys. B, 2005, 721: 79-977. Hong D K, Inami T, Yee H U. Phys. Lett. B, 2007, 646:165-1718. Kim H Ch, Kim Y, Yakhshiev U T. JHEP, 2009, 0911:034(15)9. Kim H Ch, Kim Y. JHEP, 2009, 0901: 034(10)10. Hong D K, Kim H Ch, Siwach S, Yee H U. JHEP, 2007,0711: 036(19)11. Kim Y, Lee H C, Yee H U. Phys. Rev. D, 2008, 77:085030(8)

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Chul Kim and Youngman Kim. Hadrons from a hard wall AdS/QCD model[J]. Chinese Physics C, 2010, 34(9): 1520-1522. doi: 10.1088/1674-1137/34/9/089

Chul Kim and Youngman Kim. Hadrons from a hard wall AdS/QCD model[J]. Chinese Physics C, 2010, 34(9): 1520-1522. doi: 10.1088/1674-1137/34/9/089 shu

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Received: 2010-02-09
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

Hadrons from a hard wall AdS/QCD model

Chul Kim ^,
Youngman Kim

Corresponding author: Chul Kim,

Received Date: 2010-02-09
Accepted Date: 1900-01-01
Available Online: 2010-09-05

Abstract:

We review a recent work on masses of mesons and nucleons within a hard wall model of holographic QCD in a unified approach. In order to treat meson and nucleon properties on the same footing, we introduced the same infrared (IR) cut for both sectors. In framework of present approach, the best fit to the experimental data is achieved introducing the anomalous dimension for baryons.