×
近期发现有不法分子冒充我刊与作者联系,借此进行欺诈等不法行为,请广大作者加以鉴别,如遇诈骗行为,请第一时间与我刊编辑部联系确认(《中国物理C》(英文)编辑部电话:010-88235947,010-88236950),并作报警处理。
本刊再次郑重声明:
(1)本刊官方网址为cpc.ihep.ac.cn和https://iopscience.iop.org/journal/1674-1137
(2)本刊采编系统作者中心是投稿的唯一路径,该系统为ScholarOne远程稿件采编系统,仅在本刊投稿网网址(https://mc03.manuscriptcentral.com/cpc)设有登录入口。本刊不接受其他方式的投稿,如打印稿投稿、E-mail信箱投稿等,若以此种方式接收投稿均为假冒。
(3)所有投稿均需经过严格的同行评议、编辑加工后方可发表,本刊不存在所谓的“编辑部内部征稿”。如果有人以“编辑部内部人员”名义帮助作者发稿,并收取发表费用,均为假冒。
                  
《中国物理C》(英文)编辑部
2024年10月30日

AdS/QCD and light front holography: A new approximation to QCD

  • The combination of Anti-de Sitter space (AdS) methods with light-front holography leads to a semi-classical first approximation to the spectrum and wavefunctions of meson and baryon light-quark bound states. Starting from the bound-state Hamiltonian equation of motion in QCD, we derive relativistic light-front wave equations in terms of an invariant impact variable ζ which measures the separation of the quark and gluonic constituents within the hadron at equal light-front time. These equations of motion in physical space-time are equivalent to the equations of motion which describe the propagation of spin-J modes in anti—de Sitter (AdS) space. Its eigenvalues give the hadronic spectrum, and its eigenmodes represent the probability distributions of the hadronic constituents at a given scale. Applications to the light meson and baryon spectra are presented. The predicted meson spectrum has a string-theory Regge form M2 = 4κ2(n+L+S/2 ); i.e., the square of the eigenmass is linear in both L and n, where n counts the number of nodes of the wavefunction in the radial variable ζ. The space-like pion and nucleon form factors are also well reproduced. One thus obtains a remarkable connection between the description of hadronic modes in AdS space and the Hamiltonian formulation of QCD in physical space-time quantized on the light-front at fixed light-front time τ. The model can be systematically improved by using its complete orthonormal solutions to diagonalize the full QCD light-front Hamiltonian or by applying the Lippmann-Schwinger method in order to systematically include the QCD interaction terms.

  • 加载中
  • [1] . Dirac P A M. Rev. Mod. Phys. , 1949, 21: 3922. de Teramond G F, Brodsky S J. Phys. Rev. Lett., 2009,102: 081601 [arXiv:0809.4899 [hep-ph]]3. Amsler C et al (Particle Data Group). Phys. Lett. B, 2008,667: 14. Baldini R, Dubnicka S, Gauzzi P, Pacetti S, Pasqualucci E,Srivastava Y. Eur. Phys. J. C, 1999, 11: 7095. Tadevosyan V et al (Je erson Lab F(pi) collaboration).Phys. Rev. C, 2007, 75: 055205 [arXiv:nucl-ex/0607007]6. Horn T et al (Fpi2 collaboration). Phys. Rev. Lett., 2006,97: 192001 [arXiv:nucl-ex/0607005]7. Maldacena J M. Adv. Theor. Math. Phys., 1998, 2:231; Int. J. Theor. Phys., 1999, 38: 1113 [arXiv:hep-th/9711200]8. Deur A, Burkert V, CHEN J P, Korsch W. Phys. Lett. B,2008, 665: 349 [arXiv:0803.4119 [hep-ph]]9. Brodsky S J, Shrock R. Phys. Lett. B, 2008, 666: 95[arXiv:0806.1535 [hep-th]]10. Polchinski J, Strassler M J. Phys. Rev. Lett. , 2002, 88:031601. [arXiv:hep-th/0109174]11. Karch A, Katz E, Son D T, Stephanov M A. Phys. Rev. D,2006, 74: 015005 [arXiv:hep-ph/0602229]12. de Teramond G F, Brodsky S J arXiv:0909.3900 [hep-ph]13. Andreev O, Zakharov V I. Phys. Rev. D, 2006, 74: 025023[arXiv:hep-ph/0604204]14. ZUO F. arXiv:0909.4240 [hep-ph]15. Glazek S D, Schaden M. Phys. Lett. B, 1987, 198: 4216. Hoyer P. arXiv:0909.3045 [hep-ph]17. Craig N J, Green D. JHEP, 2009, 0909: 113[arXiv:0905.4088 [hep-ph]]18. Polchinski J, Strassler M J. JHEP, 2003, 0305: 012[arXiv:hep-th/0209211]19. Brodsky S J, de Teramond G F. Phys. Rev. Lett., 2006,96: 201601 [arXiv:hep-ph/0602252]20. Brodsky S J, de Teramond G F. Phys. Rev. D, 2008, 77:056007. [arXiv:0707.3859 [hep-ph]]21. Brodsky S J, de Teramond G F. Phys. Rev. D, 2008, 78:025032. [arXiv:0804.0452 [hep-ph]]22. Abidin Z, Carlson C E. Phys. Rev. D, 2008, 77:095007. [arXiv:0801.3839 [hep-ph]]23. Brodsky S J, de Teramond G F. Phys. Lett. B, 2004, 582:211. [arXiv:hep-th/0310227]24. Erlich J, Katz E, Son D T, Stephanov M A. Phys. Rev.Lett., 2005, 95: 261602 [arXiv:hep-ph/0501128]25. Da Rold L, Pomarol A. Nucl. Phys. B, 2005, 721: 79[arXiv:hep-ph/0501218]26. Klempt E, Zaitsev A. Phys. Rept., 2007, 454: 1[arXiv:0708.4016 [hep-ph]]27. Boschi-Filho H, Braga N R F. JHEP, 2003, 0305: 009[arXiv:hep-th/0212207]28. Boschi-Filho H, Braga N R F, Carrion H L. Phys. Rev. D,2006, 73: 047901 [arXiv:hep-th/0507063]29. Evans N, Tedder A. Phys. Lett. B, 2006, 642: 546[arXiv:hep-ph/0609112]30. HONG D K, Inami T, Yee H U. Phys. Lett. B, 2007, 646:165. [arXiv:hep-ph/0609270]31. Colangelo P, de Fazio F, Jugeau F, Nicotri S. Phys. Lett.B, 2007, 652: 73 [arXiv:hep-ph/0703316]32. Forkel H. Phys. Rev. D, 2008, 78: 025001 [arXiv:0711.1179[hep-ph]]33. Vega A, Schmidt I. Phys. Rev. D, 2008, 78: 017703[arXiv:0806.2267 [hep-ph]]34. Nawa K, Suganuma H, Kojo T. Mod. Phys. Lett. A, 2008,23: 2364 [arXiv:0806.3040 [hep-th]]35. de Paula W, Frederico T, Forkel H, Beyer M. Phys. Rev.D, 2009, 79: 075019 [arXiv:0806.3830 [hep-ph]]36. Colangelo P, de Fazio F, Giannuzzi F, Jugeau F, Nicotri S.Phys. Rev. D, 2008, 78: 055009 [arXiv:0807.1054 [hep-ph]]37. Forkel H, Klempt E. Phys. Lett. B, 2009, 679: 77[arXiv:0810.2959 [hep-ph]]38. Ahn H C, HONG D K, Park C, Siwach S. Phys. Rev. D,2009, 80: 054001 [arXiv:0904.3731 [hep-ph]]39. SUI Y Q, WU Y L, XIE Z F, YANG Y B. arXiv:0909.3887[hep-ph]40. Kwee H J, Lebed R F. JHEP, 2008, 0801: 027 [arXiv:0708.4054 [hep-ph]]; Phys. Rev. D, 2008, 77: 11500[arXiv:0712.1811 [hep-ph]]41. Grigoryan H R, Radyushkin A V. Phys. Rev. D, 2007, 76:115007. [arXiv:0709.0500 [hep-ph]]; Phys. Rev. D, 2009, 78:115008. [arXiv:0808.1243 [hep-ph]]42. The SU(6) 70-plet of light baryons is not well described inthis simple model, and further investigation is necessary.See: [37]43. de Teramond G F, Brodsky S J. Phys. Rev. Lett., 2005,94, 201601 [arXiv:hep-th/0501022]44. Brodsky S J, de Teramond G F. arXiv:0802.0514 [hep-ph]45. Grigoryan H R, Radyushkin A V. Phys. Rev. D, 2007, 76:095007. [arXiv:0706.1543 [hep-ph]]46. Diehl M. Nucl. Phys. Proc. Suppl., 2006, 161: 49[arXiv:hep-ph/0510221]47. Vary J P et al. arXiv:0905.1411 [nucl-th]48. Brodsky S J, de Teramond G F, Shrock R. AIP Conf. Proc.,2008, 1056: 3 [arXiv:0807.2484 [hep-ph]]49. Brodsky S J, Deur A, de Teramond G F, to be published50. Brodsky S J, Hwang D S, Schmidt I. Phys. Lett. B, 2002,530: 99 [arXiv:hep-ph/0201296]51. Collins J C. Phys. Lett. B, 2002, 536: 43 [arXiv:hep-ph/0204004]52. Boer D, Brodsky S J, Hwang D S. Phys. Rev. D, 2003, 67:054003. [arXiv:hep-ph/0211110]53. Brodsky S J, Hoang A H, Kuhn J H, Teubner T. Phys.Lett. B, 1995, 359: 355 [arXiv:hep-ph/9508274]54. Collins J, QIU J W. Phys. Rev. D, 2007, 75: 114014[arXiv:0705.2141 [hep-ph]]55. Brodsky S J, Shrock R. arXiv:0803.2541 [hep-th]56. Brodsky S J, Shrock R. arXiv:0803.2554 [hep-th]57. Casher A, Susskind L. Phys. Rev. D, 1974, 9: 43658. Maris P, Roberts C D, Tandy P C. Phys. Lett. B, 1998,420: 267 [arXiv:nucl-th/9707003]59. Maris P, Roberts C D. Phys. Rev. C, 1997, 56: 3369[arXiv:nucl-th/9708029]60. Io e B L, Zyablyuk K N. Eur. Phys. J. C, 2003, 27: 229[arXiv:hep-ph/0207183]61. Davier M, Hocker A, ZHANG Z. Nucl. Phys. Proc. Suppl.,2007, 169: 22 [arXiv:hep-ph/0701170]62. Davier M, Descotes-Genon S, Hocker A, Malaescu B,ZHANG Z. Eur. Phys. J. C, 2008, 56: 305 [arXiv:0803.0979[hep-ph]]
  • 加载中

Get Citation
Stanley J. Brodsky and Guy F. de Teramond. AdS/QCD and light front holography: A new approximation to QCD[J]. Chinese Physics C, 2010, 34(9): 1229-1235. doi: 10.1088/1674-1137/34/9/015
Stanley J. Brodsky and Guy F. de Teramond. AdS/QCD and light front holography: A new approximation to QCD[J]. Chinese Physics C, 2010, 34(9): 1229-1235.  doi: 10.1088/1674-1137/34/9/015 shu
Milestone
Received: 2010-03-04
Revised: 1900-01-01
Article Metric

Article Views(2612)
PDF Downloads(500)
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, [email protected]
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Email This Article

Title:
Email:

AdS/QCD and light front holography: A new approximation to QCD

    Corresponding author: Stanley J. Brodsky,

Abstract: 

The combination of Anti-de Sitter space (AdS) methods with light-front holography leads to a semi-classical first approximation to the spectrum and wavefunctions of meson and baryon light-quark bound states. Starting from the bound-state Hamiltonian equation of motion in QCD, we derive relativistic light-front wave equations in terms of an invariant impact variable ζ which measures the separation of the quark and gluonic constituents within the hadron at equal light-front time. These equations of motion in physical space-time are equivalent to the equations of motion which describe the propagation of spin-J modes in anti—de Sitter (AdS) space. Its eigenvalues give the hadronic spectrum, and its eigenmodes represent the probability distributions of the hadronic constituents at a given scale. Applications to the light meson and baryon spectra are presented. The predicted meson spectrum has a string-theory Regge form M2 = 4κ2(n+L+S/2 ); i.e., the square of the eigenmass is linear in both L and n, where n counts the number of nodes of the wavefunction in the radial variable ζ. The space-like pion and nucleon form factors are also well reproduced. One thus obtains a remarkable connection between the description of hadronic modes in AdS space and the Hamiltonian formulation of QCD in physical space-time quantized on the light-front at fixed light-front time τ. The model can be systematically improved by using its complete orthonormal solutions to diagonalize the full QCD light-front Hamiltonian or by applying the Lippmann-Schwinger method in order to systematically include the QCD interaction terms.

    HTML

Reference (1)

目录

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return