-
1
-
-
27844526209
-
-
NUPBBO 0550-3213 10.1016/0550-3213(88)90390-2
-
D.J. Gross and P.F. Mende, Nucl. Phys. NUPBBO 0550-3213 B303, 407 (1988). 10.1016/0550-3213(88)90390-2
-
(1988)
Nucl. Phys.
, vol.303
, pp. 407
-
-
Gross, D.J.1
Mende, P.F.2
-
2
-
-
0002793176
-
-
PYLBAJ 0370-2693 10.1016/0370-2693(93)91401-8
-
M. Maggiore, Phys. Lett. B 304, 65 (1993). PYLBAJ 0370-2693 10.1016/0370-2693(93)91401-8
-
(1993)
Phys. Lett. B
, vol.304
, pp. 65
-
-
Maggiore, M.1
-
3
-
-
0007020922
-
-
NUPBBO 0550-3213 10.1016/0550-3213(95)00150-Q
-
C. Rovelli and L. Smolin, Nucl. Phys. NUPBBO 0550-3213 B442, 593 (1995); 10.1016/0550-3213(95)00150-Q
-
(1995)
Nucl. Phys.
, vol.442
, pp. 593
-
-
Rovelli, C.1
Smolin, L.2
-
4
-
-
0000829738
-
-
NUPBBO 0550-3213 10.1016/0550-3213(95)00550-5
-
C. Rovelli L. Smolin Nucl. Phys. NUPBBO 0550-3213 B456, 753(E) (1995); 10.1016/0550-3213(95)00550-5
-
(1995)
Nucl. Phys.
, vol.456
-
-
Rovelli, C.1
Smolin, L.2
-
8
-
-
0035927457
-
-
PYLBAJ 0370-2693 10.1016/S0370-2693(01)00506-8
-
G. Amelino-Camelia, Phys. Lett. B 510, 255 (2001); PYLBAJ 0370-2693 10.1016/S0370-2693(01)00506-8
-
(2001)
Phys. Lett. B
, vol.510
, pp. 255
-
-
Amelino-Camelia, G.1
-
9
-
-
0036344664
-
-
IMPDEO 0218-2718 10.1142/S0218271802001330
-
G. Amelino-Camelia Int. J. Mod. Phys. D 11, 35 (2002); IMPDEO 0218-2718 10.1142/S0218271802001330
-
(2002)
Int. J. Mod. Phys. D
, vol.11
, pp. 35
-
-
Amelino-Camelia, G.1
-
10
-
-
26944464228
-
-
IMPAEF 0217-751X 10.1142/S0217751X05028569
-
G. Amelino-Camelia, J. Kowalski-Glikman, G. Mandanici, and A. Procaccini, Int. J. Mod. Phys. A 20, 6007 (2005); IMPAEF 0217-751X 10.1142/ S0217751X05028569
-
(2005)
Int. J. Mod. Phys. a
, vol.20
, pp. 6007
-
-
Amelino-Camelia, G.1
Kowalski-Glikman, J.2
Mandanici, G.3
Procaccini, A.4
-
13
-
-
0037071333
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.88.190403
-
J. Magueijo and L. Smolin, Phys. Rev. Lett. 88, 190403 (2002); PRLTAO 0031-9007 10.1103/PhysRevLett.88.190403
-
(2002)
Phys. Rev. Lett.
, vol.88
, pp. 190403
-
-
Magueijo, J.1
Smolin, L.2
-
14
-
-
0037441177
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.67.044017
-
J. Magueijo L. Smolin Phys. Rev. D 67, 044017 (2003). PRVDAQ 0556-2821 10.1103/PhysRevD.67.044017
-
(2003)
Phys. Rev. D
, vol.67
, pp. 044017
-
-
Magueijo, J.1
Smolin, L.2
-
15
-
-
17144374559
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.59.124021
-
R. Gambini and J. Pullin, Phys. Rev. D 59, 124021 (1999); PRVDAQ 0556-2821 10.1103/PhysRevD.59.124021
-
(1999)
Phys. Rev. D
, vol.59
, pp. 124021
-
-
Gambini, R.1
Pullin, J.2
-
17
-
-
33645566242
-
-
hep-th/0209079;
-
L. Smolin, hep-th/0209079;
-
-
-
Smolin, L.1
-
19
-
-
33645556998
-
-
hep-th/0501091.
-
L. Smolin, hep-th/0501091.
-
-
-
Smolin, L.1
-
20
-
-
23544457426
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.51.2827
-
W.G. Unruh, Phys. Rev. D 51, 2827 (1995). PRVDAQ 0556-2821 10.1103/PhysRevD.51.2827
-
(1995)
Phys. Rev. D
, vol.51
, pp. 2827
-
-
Unruh, W.G.1
-
21
-
-
0542397525
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.58.116002
-
D. Colladay and V.A. Kostelecky, Phys. Rev. D 58, 116002 (1998). PRVDAQ 0556-2821 10.1103/PhysRevD.58.116002
-
(1998)
Phys. Rev. D
, vol.58
, pp. 116002
-
-
Colladay, D.1
Kostelecky, V.A.2
-
22
-
-
85037889819
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.59.116008
-
S.R. Coleman and S.L. Glashow, Phys. Rev. D 59, 116008 (1999). PRVDAQ 0556-2821 10.1103/PhysRevD.59.116008
-
(1999)
Phys. Rev. D
, vol.59
, pp. 116008
-
-
Coleman, S.R.1
Glashow, S.L.2
-
23
-
-
0035423635
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.64.036005
-
G. Amelino-Camelia and T. Piran, Phys. Rev. D 64, 036005 (2001); PRVDAQ 0556-2821 10.1103/PhysRevD.64.036005
-
(2001)
Phys. Rev. D
, vol.64
, pp. 036005
-
-
Amelino-Camelia, G.1
Piran, T.2
-
24
-
-
0037777532
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.90.211601
-
R.C. Myers and M. Pospelov, Phys. Rev. Lett. 90, 211601 (2003); PRLTAO 0031-9007 10.1103/PhysRevLett.90.211601
-
(2003)
Phys. Rev. Lett.
, vol.90
, pp. 211601
-
-
Myers, R.C.1
Pospelov, M.2
-
25
-
-
4043122411
-
-
PRLTAO 0031-9007 10.1103/PhysRevLett.93.021101
-
T.A. Jacobson, S. Liberati, D. Mattingly, and F.W. Stecker, Phys. Rev. Lett. 93, 021101 (2004); PRLTAO 0031-9007 10.1103/PhysRevLett.93.021101
-
(2004)
Phys. Rev. Lett.
, vol.93
, pp. 021101
-
-
Jacobson, T.A.1
Liberati, S.2
Mattingly, D.3
Stecker, F.W.4
-
26
-
-
84989815178
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.59.124011
-
S. Corley and T. Jacobson, Phys. Rev. D 59, 124011 (1999); PRVDAQ 0556-2821 10.1103/PhysRevD.59.124011
-
(1999)
Phys. Rev. D
, vol.59
, pp. 124011
-
-
Corley, S.1
Jacobson, T.2
-
27
-
-
0242641588
-
-
PYLBAJ 0370-2693 10.1016/j.physletb.2003.09.040
-
S. Hossenfelder, Phys. Lett. B 575, 85 (2003); PYLBAJ 0370-2693 10.1016/j.physletb.2003.09.040
-
(2003)
Phys. Lett. B
, vol.575
, pp. 85
-
-
Hossenfelder, S.1
-
28
-
-
33244488556
-
-
CQGRDG 0264-9381 10.1088/0264-9381/23/5/N01
-
S. Hossenfelder, Classical Quantum Gravity CQGRDG 0264-9381 23, 1815 (2006). 10.1088/0264-9381/23/5/N01
-
(2006)
Classical Quantum Gravity
, vol.23
, pp. 1815
-
-
Hossenfelder, S.1
-
29
-
-
32644462766
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.73.024005
-
B.Z. Foster, Phys. Rev. D 73, 024005 (2006). PRVDAQ 0556-2821 10.1103/PhysRevD.73.024005
-
(2006)
Phys. Rev. D
, vol.73
, pp. 024005
-
-
Foster, B.Z.1
-
30
-
-
0001040167
-
-
IMPDEO 0218-2718 10.1142/S0218271893000246
-
J.W. Moffat, Int. J. Mod. Phys. D 2, 351 (1993); IMPDEO 0218-2718 10.1142/S0218271893000246
-
(1993)
Int. J. Mod. Phys. D
, vol.2
, pp. 351
-
-
Moffat, J.W.1
-
31
-
-
4243966138
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.59.043516
-
A. Albrecht and J. Magueijo, Phys. Rev. D 59, 043516 (1999). PRVDAQ 0556-2821 10.1103/PhysRevD.59.043516
-
(1999)
Phys. Rev. D
, vol.59
, pp. 043516
-
-
Albrecht, A.1
Magueijo, J.2
-
33
-
-
10744220757
-
-
NPBSE7 0920-5632 10.1016/S0920-5632(03)02088-7
-
P. Chen and R.J. Adler, Nucl. Phys. B, Proc. Suppl. NPBSE7 0920-5632 124, 103 (2003). 10.1016/S0920-5632(03)02088-7
-
(2003)
Nucl. Phys. B, Proc. Suppl.
, vol.124
, pp. 103
-
-
Chen, P.1
Adler, R.J.2
-
34
-
-
0037824044
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.14.2474
-
R.J. Adler and T.K. Das, Phys. Rev. D 14, 2474 (1976); PRVDAQ 0556-2821 10.1103/PhysRevD.14.2474
-
(1976)
Phys. Rev. D
, vol.14
, pp. 2474
-
-
Adler, R.J.1
Das, T.K.2
-
35
-
-
0003768888
-
-
edited by C. DeWitt and B.S. DeWitt (Gordon Breach, New York
-
R.S. Hanni and R. Ruffini, in Black Holes, edited by, C. DeWitt, and, B.S. DeWitt, (Gordon Breach, New York, 1973).
-
(1973)
Black Holes
-
-
Hanni, R.S.1
Ruffini, R.2
-
36
-
-
33645577066
-
-
We assume that the modified dispersion relation will not change this relation which is consistent with the result in, where the impact of doubly special relativity on gravity is investigated. also see for recent work on the thermodynamics of modified black holes from gravity's rainbow.
-
We assume that the modified dispersion relation will not change this relation which is consistent with the result in, where the impact of doubly special relativity on gravity is investigated. also see for recent work on the thermodynamics of modified black holes from gravity's rainbow.
-
-
-
-
37
-
-
33645555373
-
-
We make this assumption based on the belief that the thermodynamical laws of black holes can still be captured even in the quantum theory of gravity. This belief has been supported by recent work in isolated horizon programs as well as the stretched horizon program, where the first law of black hole thermodynamics can still be established in a quasilocal fashion. In the context of DSR, which may be viewed as the semiclassical effect of quantum gravity, we assume the modification of dispersion relations of particle would not change this picture. However, before proceeding, we cautiously point out that this exact form of the first law may not be generally true but receives a small modification, or even fails for instance in the Einstein-Aether theory as investigated in.
-
We make this assumption based on the belief that the thermodynamical laws of black holes can still be captured even in the quantum theory of gravity. This belief has been supported by recent work in isolated horizon programs as well as the stretched horizon program, where the first law of black hole thermodynamics can still be established in a quasilocal fashion. In the context of DSR, which may be viewed as the semiclassical effect of quantum gravity, we assume the modification of dispersion relations of particle would not change this picture. However, before proceeding, we cautiously point out that this exact form of the first law may not be generally true but receives a small modification, or even fails for instance in the Einstein-Aether theory as investigated in.
-
-
-
-
38
-
-
84856127429
-
-
The factor -1/2 in the logarithmic term happens to be the same as the one appearing in where this factor is rigorously fixed in the context of loop quantum gravity. However, we stress that, at the semiclassical level as discussed in our paper, this factor cannot be fixed uniquely, but depends on the value of η which has been set as a unit in our paper. A straightforward calculation shows that in general the factor would be -η/2. If we insist that the minimum area in our paper is the same as that in loop quantum gravity as we suggested in above reference, then the factor turns out to be -3πγ/4, rather than -1/2. Reversely, if we insist on setting the factor exactly to be -1/2, namely η=1, then from this approach we have an Immirzi parameter γ 0.37, different from the result in. This discrepancy can be understood as this specific MDR we proposed is only a coarse grained model at the semiclassical limit of quantum gravity.
-
The factor -1/2 in the logarithmic term happens to be the same as the one appearing in where this factor is rigorously fixed in the context of loop quantum gravity. However, we stress that, at the semiclassical level as discussed in our paper, this factor cannot be fixed uniquely, but depends on the value of η which has been set as a unit in our paper. A straightforward calculation shows that in general the factor would be -η/2. If we insist that the minimum area in our paper is the same as that in loop quantum gravity as we suggested in above reference, then the factor turns out to be -3πγ/4, rather than -1/2. Reversely, if we insist on setting the factor exactly to be -1/2, namely η=1, then from this approach we have an Immirzi parameter γ 0.37, different from the result in. This discrepancy can be understood as this specific MDR we proposed is only a coarse grained model at the semiclassical limit of quantum gravity.
-
-
-
-
40
-
-
33645073005
-
-
CQGRDG 0264-9381 10.1088/0264-9381/23/7/022
-
G. Amelino-Camelia, M. Arzano, Y. Ling, and G. Mandanici, Classical Quantum Gravity CQGRDG 0264-9381 23, 2585 (2006); 10.1088/0264-9381/23/7/022
-
(2006)
Classical Quantum Gravity
, vol.23
, pp. 2585
-
-
Amelino-Camelia, G.1
Arzano, M.2
Ling, Y.3
Mandanici, G.4
-
41
-
-
42749102097
-
-
PRVDAQ 0556-2821 10.1103/PhysRevD.70.124021
-
A.J.M. Medved and E.C. Vagenas, Phys. Rev. D 70, 124021 (2004). PRVDAQ 0556-2821 10.1103/PhysRevD.70.124021
-
(2004)
Phys. Rev. D
, vol.70
, pp. 124021
-
-
Medved, A.J.M.1
Vagenas, E.C.2
-
42
-
-
0001735887
-
-
NATUAS 0028-0836 10.1038/329308a0
-
J.H. MacGibbon, Nature (London) NATUAS 0028-0836 329, 308 (1987); 10.1038/329308a0
-
(1987)
Nature (London)
, vol.329
, pp. 308
-
-
MacGibbon, J.H.1
-
45
-
-
2142770186
-
-
CQGRDG 0264-9381 10.1088/0264-9381/21/7/001
-
J. Magueijo and L. Smolin, Classical Quantum Gravity CQGRDG 0264-9381 21, 1725 (2004). 10.1088/0264-9381/21/7/001
-
(2004)
Classical Quantum Gravity
, vol.21
, pp. 1725
-
-
Magueijo, J.1
Smolin, L.2
-
47
-
-
10044267716
-
-
CQGRDG 0264-9381 10.1088/0264-9381/21/22/015
-
K.A. Meissner, Classical Quantum Gravity CQGRDG 0264-9381 21, 5245 (2004). 10.1088/0264-9381/21/22/015
-
(2004)
Classical Quantum Gravity
, vol.21
, pp. 5245
-
-
Meissner, K.A.1
|