[1]
|
D. A. Kirzhnits and A. D. Linde, “Macroscopic Consequence of the Weinberg Model,” Physics Letters B, Vol. 42, No. 4, 1972, pp. 471-474.
doi:10.1016/0370-2693(72)90109-8
|
[2]
|
S. Weinberg, “Gauge and Global Symmetry at High Temperature,” Physical Review D, Vol. 9, No. 12, 1974, pp. 3357-3378. doi:10.1103/PhysRevD.9.3357
|
[3]
|
L. Dolan and R. Jackiw, “Symmetry Behavior at Finite Temperature,” Physical Review D, Vol. 9, No. 12, 1974, pp. 3320-3341. doi:10.1103/PhysRevD.9.3320
|
[4]
|
S. W. Hawking, “Particle Creation by Black Holes,” Communications in Mathematical Physics, Vol. 43, No. 3, 1975, pp. 199-220. doi:10.1007/BF02345020
|
[5]
|
G. Denardo and E. Spallucci, “Symmetry Restoration in Conformally Flat Metric,” Nuovo Cimento A, Vol. 64, No, 1, 1981, pp. 15-26. doi:10.1007/BF02773363
|
[6]
|
W. G. Unruh, “Notes on Black Hole Evaporation,” Physical Review D, Vol. 14, No. 4, 1976, p. 870.
doi:10.1103/PhysRevD.14.870
|
[7]
|
W. G. Unruh and N. Weiss, “Acceleration Radiation in Interacting Field Theories,” Physical Review D, Vol. 29, No. 8, 1984, p. 1656. doi:10.1103/PhysRevD.29.1656
|
[8]
|
T. Ohsaku, “Dynamical Chiral Symmetry Breaking and its Restoration for an Accelerated Observer,” Physics Letters B, Vol. 599, No. 1-2, 2004, pp. 102-110.
doi:10.1016/j.physletb.2004.08.019
|
[9]
|
D. Ebert and V. Ch. Zhukovsky, “Restoration of Dynamically Broken Chiral and Color Symmetry for an Accelerated Observer,” Physics Letters B, Vol. 645, No. 2-3, 2007, pp. 267-274. doi:10.1016/j.physletb.2006.12.013
|
[10]
|
K. Peeters and M. Zamaklar, “Dissociation by Acceleration,” Journal of High Energy Physics, Vol. 801, 2008, p. 38. doi:10.1088/1126-6708/2008/01/038
|
[11]
|
J. M. Cornwall, R. Jackiw and E. Tomboulis, “Effective Action for Composite Operators,” Physical Review D, Vol. 10, No. 8, 1974, pp. 2428-2445.
doi:10.1103/PhysRevD.10.2428
|
[12]
|
L. C. B. Crispino, A. Higuchi and G. E. A. Matsas, “The Unruh Effect and its Applications,” Reviews of. Modern Physics, Vol. 80, No. 3, 2008, pp. 787-838.
doi:10.1103/RevModPhys.80.787
|
[13]
|
G. Amelino-Camelia and S.-Y. Pi, “Selfconsistent Improvement of the Finite Temperature Effective Potential,” Physical Review D, Vol. 47, No. 6, 1993, pp. 2356-2362.
doi:10.1103/PhysRevD.47.2356
|
[14]
|
P. Castorina, M. Consoli and D. Zappalà, “Finite Temperature Hartree-Fock Approximation to λφ4 Theory,” Physics Letters B, Vol. 201, No. 1, 1988, pp. 90-94.
doi:10.1016/0370-2693(88)90086-X
|
[15]
|
R. M. Cavalcanti, P. Giacconi, G. Pupillo and R. Soldati, “Bose-Einstein Condensation in the Presence of a Uniform Field and a Point-Like Impurity,” Physical Review A, Vol. 65, No. 5, 2002, pp. 53-60.
doi:10.1103/PhysRevA.65.053606
|
[16]
|
C. Barcelo, S. Liberati and M. Visser, “Analogue Gravity,” Living Reviews in Relativity, Vol. 4, No. 3, 2011, p. 12. http://www.livingreviews.org/lrr-2011-3
|
[17]
|
A. Iorio and G. Lambiase, “The Hawking-Unruh Phenomenon on Graphene,” Physics Letters B, Vol. 716, No. 2, 2012, pp. 334-337. doi:10.1016/j.physletb.2012.08.023
|
[18]
|
P. Castorina, D. Kharzeev and H. Satz, “Thermal Hadronization and Hawking-Unruh Radiation in QCD,” The European Physical Journal, Vol. 52, No. 1, 2007, pp. 187-201. doi:10.1140/epjc/s10052-007-0368-6
|
[19]
|
F. Becattini, P. Castorina, A. Milov and H. Satz, “Prediction of Hadron Abundances in pp Collision at LHC,” Journal of Physics G, Vol. 38, No. 2, p. 25.
doi:10.1088/0954-3899/38/2/025002
|
[20]
|
P. Castorina, R. V. Gavai and H. Satz, “The QCD Phase Structure at High Baryon Density,” The European Physical Journal, Vol. 69, No. 1-2, 2010, pp. 169-178.
doi:10.1140/epjc/s10052-011-1653-y
|