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《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.

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  • [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]]
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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
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Received: 2010-03-04
Revised: 1900-01-01
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AdS/QCD and light front holography: A new approximation to QCD

    Corresponding author: Stanley J. Brodsky,

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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.

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