# Acceleration and Energy Loss in N=4 SYM

- Published: 02 Mar 2009

[1] M. Chernicoff and A. Guijosa, “Acceleration, Energy Loss and Screening in Strongly-Coupled Gauge Theories,” JHEP 0806, 005 (2008) [arXiv:0803.3070 [hep-th]]. [OpenAIRE]

[2] W. A. Zajc, “The Fluid Nature of Quark-Gluon Plasma,” arXiv:0802.3552 [nuclex]; B. Muller, “From Quark-Gluon Plasma to the Perfect Liquid,” Acta Phys. Polon. B 38, 3705 (2007) [arXiv:0710.3366 [nucl-th]]; E. Shuryak, “Emerging theory of strongly coupled quark-gluon plasma,” arXiv:hep-ph/0703208. [OpenAIRE]

[3] J. Casalderrey-Solana and C. A. Salgado, “Introductory lectures on jet quenching in heavy ion collisions,” arXiv:0712.3443 [hep-ph]; R. Rapp and H. van Hees, “Heavy Quark Diffusion as a Probe of the QuarkGluon Plasma,” arXiv:0803.0901 [hep-ph].

[4] J. M. Maldacena, “The large N limit of superconformal field theories and supergravity,” Adv. Theor. Math. Phys. 2, 231 (1998) [Int. J. Theor. Phys. 38, 1113 (1999)] [arXiv:hep-th/9711200].

[5] S. S. Gubser, I. R. Klebanov and A. M. Polyakov, “Gauge theory correlators from non-critical string theory,” Phys. Lett. B 428, 105 (1998) [arXiv:hep-th/9802109]; E. Witten, “Anti-de Sitter space and holography,” Adv. Theor. Math. Phys. 2, 253 (1998) [arXiv:hep-th/9802150].

[6] O. Aharony, S. S. Gubser, J. M. Maldacena, H. Ooguri and Y. Oz, “Large N field theories, string theory and gravity,” Phys. Rept. 323, 183 (2000) [arXiv:hep-th/9905111].

[7] C. P. Herzog, A. Karch, P. Kovtun, C. Kozcaz and L. G. Yaffe, “Energy loss of a heavy quark moving through N = 4 supersymmetric Yang-Mills plasma,” JHEP 0607 (2006) 013 [arXiv:hep-th/0605158].

[8] S. S. Gubser, “Drag force in AdS/CFT,” Phys. Rev. D 74 (2006) 126005 [arXiv:hep-th/0605182].

[9] J. Casalderrey-Solana and D. Teaney, “Heavy quark diffusion in strongly coupled N = 4 Yang Mills,” Phys. Rev. D 74 (2006) 085012 [arXiv:hep-ph/0605199]. [OpenAIRE]

[10] H. Liu, K. Rajagopal and U. A. Wiedemann, “Calculating the jet quenching parameter from AdS/CFT,” Phys. Rev. Lett. 97 (2006) 182301 [arXiv:hep-ph/0605178].

[11] K. Peeters, J. Sonnenschein and M. Zamaklar, “Holographic melting and related properties of mesons in a quark gluon plasma,” Phys. Rev. D 74 (2006) 106008 [arXiv:hep-th/0606195]. [OpenAIRE]

[12] H. Liu, K. Rajagopal and U. A. Wiedemann, “An AdS/CFT calculation of screening in a hot wind,” Phys. Rev. Lett. 98 (2007) 182301 [arXiv:hep-ph/0607062].

[13] M. Chernicoff, J. A. Garc´ıa and A. Gu¨ijosa, “The energy of a moving quark-antiquark pair in an N = 4 SYM plasma,” JHEP 0609 (2006) 068 [arXiv:hep-th/0607089]. [OpenAIRE]

[14] K. Dusling, J. Erdmenger, M. Kaminski, F. Rust, D. Teaney and C. Young, “Quarkonium transport in thermal AdS/CFT,” JHEP 0810 (2008) 098 [arXiv:0808.0957 [hep-th]].

[15] M. Chernicoff and A. Gu¨ijosa, “Energy loss of gluons, baryons and k-quarks in an N = 4 SYM plasma,” JHEP 0702 (2007) 084 [arXiv:hep-th/0611155].

##### Similar Outcomes

[1] M. Chernicoff and A. Guijosa, “Acceleration, Energy Loss and Screening in Strongly-Coupled Gauge Theories,” JHEP 0806, 005 (2008) [arXiv:0803.3070 [hep-th]]. [OpenAIRE]

[2] W. A. Zajc, “The Fluid Nature of Quark-Gluon Plasma,” arXiv:0802.3552 [nuclex]; B. Muller, “From Quark-Gluon Plasma to the Perfect Liquid,” Acta Phys. Polon. B 38, 3705 (2007) [arXiv:0710.3366 [nucl-th]]; E. Shuryak, “Emerging theory of strongly coupled quark-gluon plasma,” arXiv:hep-ph/0703208. [OpenAIRE]

[3] J. Casalderrey-Solana and C. A. Salgado, “Introductory lectures on jet quenching in heavy ion collisions,” arXiv:0712.3443 [hep-ph]; R. Rapp and H. van Hees, “Heavy Quark Diffusion as a Probe of the QuarkGluon Plasma,” arXiv:0803.0901 [hep-ph].

[4] J. M. Maldacena, “The large N limit of superconformal field theories and supergravity,” Adv. Theor. Math. Phys. 2, 231 (1998) [Int. J. Theor. Phys. 38, 1113 (1999)] [arXiv:hep-th/9711200].

[5] S. S. Gubser, I. R. Klebanov and A. M. Polyakov, “Gauge theory correlators from non-critical string theory,” Phys. Lett. B 428, 105 (1998) [arXiv:hep-th/9802109]; E. Witten, “Anti-de Sitter space and holography,” Adv. Theor. Math. Phys. 2, 253 (1998) [arXiv:hep-th/9802150].

[6] O. Aharony, S. S. Gubser, J. M. Maldacena, H. Ooguri and Y. Oz, “Large N field theories, string theory and gravity,” Phys. Rept. 323, 183 (2000) [arXiv:hep-th/9905111].

[7] C. P. Herzog, A. Karch, P. Kovtun, C. Kozcaz and L. G. Yaffe, “Energy loss of a heavy quark moving through N = 4 supersymmetric Yang-Mills plasma,” JHEP 0607 (2006) 013 [arXiv:hep-th/0605158].

[8] S. S. Gubser, “Drag force in AdS/CFT,” Phys. Rev. D 74 (2006) 126005 [arXiv:hep-th/0605182].

[9] J. Casalderrey-Solana and D. Teaney, “Heavy quark diffusion in strongly coupled N = 4 Yang Mills,” Phys. Rev. D 74 (2006) 085012 [arXiv:hep-ph/0605199]. [OpenAIRE]

[10] H. Liu, K. Rajagopal and U. A. Wiedemann, “Calculating the jet quenching parameter from AdS/CFT,” Phys. Rev. Lett. 97 (2006) 182301 [arXiv:hep-ph/0605178].

[11] K. Peeters, J. Sonnenschein and M. Zamaklar, “Holographic melting and related properties of mesons in a quark gluon plasma,” Phys. Rev. D 74 (2006) 106008 [arXiv:hep-th/0606195]. [OpenAIRE]

[12] H. Liu, K. Rajagopal and U. A. Wiedemann, “An AdS/CFT calculation of screening in a hot wind,” Phys. Rev. Lett. 98 (2007) 182301 [arXiv:hep-ph/0607062].

[13] M. Chernicoff, J. A. Garc´ıa and A. Gu¨ijosa, “The energy of a moving quark-antiquark pair in an N = 4 SYM plasma,” JHEP 0609 (2006) 068 [arXiv:hep-th/0607089]. [OpenAIRE]

[14] K. Dusling, J. Erdmenger, M. Kaminski, F. Rust, D. Teaney and C. Young, “Quarkonium transport in thermal AdS/CFT,” JHEP 0810 (2008) 098 [arXiv:0808.0957 [hep-th]].

[15] M. Chernicoff and A. Gu¨ijosa, “Energy loss of gluons, baryons and k-quarks in an N = 4 SYM plasma,” JHEP 0702 (2007) 084 [arXiv:hep-th/0611155].