[1] Cumrun Vafa. The String landscape and the swampland. 9 2005.
[2] Nima Arkani-Hamed, Lubos Motl, Alberto Nicolis, and Cumrun Vafa.
The String landscape, black holes and gravity as the weakest force.
JHEP, 06:060, 2007.
[3] Tom Rudelius. Constraints on Axion Inflation from the Weak Gravity
Conjecture. JCAP, 09:020, 2015.
[4] Ben Heidenreich, Matthew Reece, and Tom Rudelius. Weak Gravity
Strongly Constrains Large-Field Axion Inflation. JHEP, 12:108, 2015.
[5] Makoto Natsuume. Higher order correction to the GHS string black
hole. Phys. Rev. D, 50:3949–3953, 1994.
[6] Yevgeny Kats, Lubos Motl, and Megha Padi. Higher-order corrections
to mass-charge relation of extremal black holes. JHEP, 12:068, 2007.
[7] Pablo A. Cano, Tom´as Ort´ın, and Pedro F. Ramirez. On the extremality
bound of stringy black holes. JHEP, 02:175, 2020.
[8] Pablo A. Cano, Samuele Chimento, Rom´an Linares, Tom´as Ort´ın, and
Pedro F. Ram´ırez. α′ corrections of Reissner-Nordstr¨om black holes.
JHEP, 02:031, 2020.
[9] Clifford Cheung, Junyu Liu, and Grant N. Remmen. Proof of the Weak
Gravity Conjecture from Black Hole Entropy. JHEP, 10:004, 2018.
[10] Yuta Hamada, Toshifumi Noumi, and Gary Shiu. Weak Gravity Conjecture from Unitarity and Causality. Phys. Rev. Lett., 123(5):051601,
2019.
[11] Brando Bellazzini, Matthew Lewandowski, and Javi Serra. Positivity
of Amplitudes, Weak Gravity Conjecture, and Modified Gravity. Phys.
Rev. Lett., 123(25):251103, 2019.
[12] Anthony M. Charles. The Weak Gravity Conjecture, RG Flows, and
Supersymmetry. 6 2019.
[13] Callum R. T. Jones and Brian McPeak. The Black Hole Weak Gravity
Conjecture with Multiple Charges. JHEP, 06:140, 2020.
58
[14] Gregory J. Loges, Toshifumi Noumi, and Gary Shiu. Thermodynamics
of 4D Dilatonic Black Holes and the Weak Gravity Conjecture. Phys.
Rev. D, 102(4):046010, 2020.
[15] Garrett Goon and Riccardo Penco. Universal Relation between Corrections to Entropy and Extremality. Phys. Rev. Lett., 124(10):101103,
2020.
[16] Sera Cremonini, Callum R. T. Jones, James T. Liu, and Brian McPeak.
Higher-Derivative Corrections to Entropy and the Weak Gravity Conjecture in Anti-de Sitter Space. JHEP, 09:003, 2020.
[17] Qiuhong Chen, Wei Hong, and Jun Tao.
Universal thermodynamic extremality relations for charged AdS black hole surrounded by
quintessence. 5 2020.
[18] Gregory J. Loges, Toshifumi Noumi, and Gary Shiu. Duality and Supersymmetry Constraints on the Weak Gravity Conjecture. JHEP, 11:008,
2020.
[19] Nikolay Bobev, Anthony M. Charles, Kiril Hristov, and Valentin
Reys. Higher-derivative supergravity, AdS4 holography, and black holes.
JHEP, 08:173, 2021.
[20] Nima Arkani-Hamed, Yu-tin Huang, Jin-Yu Liu, and Grant N. Remmen.
Causality, unitarity, and the weak gravity conjecture. JHEP, 03:083,
2022.
[21] Sera Cremonini, Callum R. T. Jones, James T. Liu, Brian McPeak, and
Yuezhang Tang. Repulsive black holes and higher-derivatives. JHEP,
03:013, 2022.
[22] Lars Aalsma. Corrections to extremal black holes from Iyer-Wald formalism. Phys. Rev. D, 105(6):066022, 2022.
[23] Mark J. Bowick, L. Smolin, and L. C. R. Wijewardhana. Role of String
Excitations in the Last Stages of Black Hole Evaporation. Phys. Rev.
Lett., 56:424, 1986.
[24] Leonard Susskind. Some speculations about black hole entropy in string
theory. pages 118–131, 10 1993.
[25] Gary T. Horowitz and Joseph Polchinski. A Correspondence principle
for black holes and strings. Phys. Rev. D, 55:6189–6197, 1997.
59
[26] Ben Heidenreich, Matthew Reece, and Tom Rudelius. Evidence for a
sublattice weak gravity conjecture. JHEP, 08:025, 2017.
[27] Miguel Montero, Gary Shiu, and Pablo Soler. The Weak Gravity Conjecture in three dimensions. JHEP, 10:159, 2016.
[28] Seung-Joo Lee, Wolfgang Lerche, and Timo Weigand. Tensionless
Strings and the Weak Gravity Conjecture. JHEP, 10:164, 2018.
[29] Seung-Joo Lee, Wolfgang Lerche, and Timo Weigand. Modular Fluxes,
Elliptic Genera, and Weak Gravity Conjectures in Four Dimensions.
JHEP, 08:104, 2019.
[30] Lars Aalsma, Alex Cole, and Gary Shiu. Weak Gravity Conjecture,
Black Hole Entropy, and Modular Invariance. JHEP, 08:022, 2019.
[31] Clifford Cheung and Grant N. Remmen. Infrared Consistency and the
Weak Gravity Conjecture. JHEP, 12:087, 2014.
[32] Stefano Andriolo, Daniel Junghans, Toshifumi Noumi, and Gary Shiu.
A Tower Weak Gravity Conjecture from Infrared Consistency. Fortsch.
Phys., 66(5):1800020, 2018.
[33] Wei-Ming Chen, Yu-Tin Huang, Toshifumi Noumi, and Congkao Wen.
Unitarity bounds on charged/neutral state mass ratios. Phys. Rev. D,
100(2):025016, 2019.
[34] Lasma Alberte, Claudia de Rham, Sumer Jaitly, and Andrew J. Tolley.
QED positivity bounds. Phys. Rev. D, 103(12):125020, 2021.
[35] Katsuki Aoki, Tran Quang Loc, Toshifumi Noumi, and Junsei Tokuda.
Is the Standard Model in the Swampland? Consistency Requirements
from Gravitational Scattering. Phys. Rev. Lett., 127(9):091602, 2021.
[36] Toshifumi Noumi and Junsei Tokuda. Gravitational positivity bounds
on scalar potentials. Phys. Rev. D, 104(6):066022, 2021.
[37] Ben Heidenreich, Matthew Reece, and Tom Rudelius. Sharpening the
Weak Gravity Conjecture with Dimensional Reduction. JHEP, 02:140,
2016.
[38] Allan Adams, Nima Arkani-Hamed, Sergei Dubovsky, Alberto Nicolis,
and Riccardo Rattazzi. Causality, analyticity and an IR obstruction to
UV completion. JHEP, 10:014, 2006.
60
[39] Toshifumi Noumi and Hibiki Satake. Higher derivative corrections to
black brane thermodynamics and the weak gravity conjecture. JHEP,
12:130, 2022.
[40] Hirosi Ooguri and Cumrun Vafa. On the Geometry of the String Landscape and the Swampland. Nucl. Phys. B, 766:21–33, 2007.
[41] S. W. Hawking. Particle Creation by Black Holes. Commun. Math.
Phys., 43:199–220, 1975. [Erratum: Commun.Math.Phys. 46, 206
(1976)].
[42] Fritz Sauter. Uber das Verhalten eines Elektrons im homogenen elektrischen Feld nach der relativistischen Theorie Diracs. Z. Phys., 69:742–
764, 1931.
[43] W. Heisenberg and H. Euler. Consequences of Dirac’s theory of
positrons. Z. Phys., 98(11-12):714–732, 1936.
[44] Julian Schwinger. On gauge invariance and vacuum polarization. Phys.
Rev., 82:664–679, Jun 1951.
[45] A. I. Nikishov. Pair production by a constant external field. Zh. Eksp.
Teor. Fiz., 57:1210–1216, 1969.
[46] J. D. Bekenstein. Black holes and the second law. Lett. Nuovo Cim.,
4:737–740, 1972.
[47] Leonard Susskind. Trouble for remnants. 1 1995.
[48] S. Deser and B. Zumino. A complete action for the spinning string.
Physics Letters B, 65(4):369–373, 1976.
[49] L. Brink, P. Di Vecchia, and P. Howe. A locally supersymmetric and
reparametrization invariant action for the spinning string. Physics Letters B, 65(5):471–474, 1976.
[50] A.M. Polyakov. Quantum geometry of bosonic strings. Physics Letters
B, 103(3):207–210, 1981.
[51] Daniel Harlow and Hirosi Ooguri. Constraints on Symmetries from
Holography. Phys. Rev. Lett., 122(19):191601, 2019.
[52] Juan Martin Maldacena. The Large N limit of superconformal field
theories and supergravity. Adv. Theor. Math. Phys., 2:231–252, 1998.
61
[53] Daniel Harlow, Ben Heidenreich, Matthew Reece, and Tom Rudelius.
The Weak Gravity Conjecture: A Review. 1 2022.
[54] R. Penrose. Gravitational collapse: The role of general relativity. Riv.
Nuovo Cim., 1:252–276, 1969.
[55] Gary T. Horowitz and Andrew Strominger. Black strings and P-branes.
Nucl. Phys. B, 360:197–209, 1991.
[56] James M. Bardeen, B. Carter, and S. W. Hawking. The Four laws of
black hole mechanics. Commun. Math. Phys., 31:161–170, 1973.
[57] Friedrich Kottler. Uber
die physikalischen grundlagen der einsteinschen
gravitationstheorie. Annalen der Physik, 361(14):401–462, 1918.
[58] Roger Penrose. Gravitational Collapse: the Role of General Relativity.
Nuovo Cimento Rivista Serie, 1:252, January 1969.
[59] J. M. Bardeen, B. Carter, and S. W. Hawking. The four laws of black
hole mechanics. Communications in Mathematical Physics, 31(2):161–
170, June 1973.
[60] Robert M. Wald. Black hole entropy is the Noether charge. Phys. Rev.
D, 48(8):R3427–R3431, 1993.
[61] J. G. Valatin. Comments on the theory of superconductivity. Nuovo
Cim., 7:843–857, 1958.
[62] N. N. Bogolyubov. On a New method in the theory of superconductivity.
Nuovo Cim., 7:794–805, 1958.
[63] S. W. Hawking. Black hole explosions. Nature, 248:30–31, 1974.
[64] Larry Smarr. Mass formula for kerr black holes. Phys. Rev. Lett., 30:521–
521, Mar 1973.
[65] James W. York. Role of conformal three-geometry in the dynamics of
gravitation. Phys. Rev. Lett., 28:1082–1085, Apr 1972.
[66] G. W. Gibbons and S. W. Hawking. Action integrals and partition
functions in quantum gravity. Phys. Rev. D, 15:2752–2756, May 1977.
[67] R. Arnowitt, S. Deser, and C. W. Misner. Dynamical structure and
definition of energy in general relativity. Phys. Rev., 116:1322–1330,
Dec 1959.
62
[68] Paul K. Townsend and Marija Zamaklar. The First law of black brane
mechanics. Class. Quant. Grav., 18:5269–5286, 2001.
[69] J. X. Lu. ADM masses for black strings and p-branes. Phys. Lett. B,
313:29–34, 1993.
[70] Arthur Komar. Covariant conservation laws in general relativity. Phys.
Rev., 113:934–936, 1959.
[71] Harvey S. Reall and Jorge E. Santos. Higher derivative corrections to
Kerr black hole thermodynamics. JHEP, 04:021, 2019.
[72] Lasma Alberte, Claudia de Rham, Sumer Jaitly, and Andrew J. Tolley. Positivity Bounds and the Massless Spin-2 Pole. Phys. Rev. D,
102(12):125023, 2020.
[73] Junsei Tokuda, Katsuki Aoki, and Shin’ichi Hirano. Gravitational positivity bounds. JHEP, 11:054, 2020.
[74] Mario Herrero-Valea, Raquel Santos-Garcia, and Anna Tokareva. Massless positivity in graviton exchange. Phys. Rev. D, 104(8):085022, 2021.
[75] Nima Arkani-Hamed, Tzu-Chen Huang, and Yu-Tin Huang. The EFTHedron. JHEP, 05:259, 2021.
[76] Simon Caron-Huot, Dalimil Mazac, Leonardo Rastelli, and David
Simmons-Duffin. Sharp boundaries for the swampland. JHEP, 07:110,
2021.
63
...
論文の公開元へ
