[1] M. Bershadsky, C. Vafa and V. Sadov, “D-branes and topological field theories,” Nucl.
Phys. B 463, 420 (1996) doi:10.1016/0550-3213(96)00026-0 [hep-th/9511222].
[2] A. Strominger and C. Vafa, “Microscopic origin of the Bekenstein-Hawking entropy,”
Phys. Lett. B 379, 99 (1996) doi:10.1016/0370-2693(96)00345-0 [hep-th/9601029].
[3] J. C. Breckenridge, R. C. Myers, A. W. Peet and C. Vafa, “D-branes and spinning
black holes,” Phys. Lett. B 391, 93 (1997) doi:10.1016/S0370-2693(96)01460-8 [hepth/9602065].
[4] O. Lunin and S. D. Mathur, “AdS / CFT duality and the black hole information
paradox,” Nucl. Phys. B 623, 342 (2002) doi:10.1016/S0550-3213(01)00620-4 [hepth/0109154].
[5] O. Lunin, J. M. Maldacena and L. Maoz, “Gravity solutions for the D1-D5 system with
angular momentum,” hep-th/0212210.
[6] M. Taylor, “General 2 charge geometries,” JHEP 0603, 009 (2006) doi:10.1088/11266708/2006/03/009 [hep-th/0507223].
[7] I. Kanitscheider, K. Skenderis and M. Taylor, “Fuzzballs with internal excitations,”
JHEP 0706, 056 (2007) doi:10.1088/1126-6708/2007/06/056 [arXiv:0704.0690 [hep-th]].
[8] V. S. Rychkov, “D1-D5 black hole microstate counting from supergravity,” JHEP 0601,
063 (2006) doi:10.1088/1126-6708/2006/01/063 [hep-th/0512053].
[9] C. Krishnan and A. Raju, “A Note on D1-D5 Entropy and Geometric Quantization,”
JHEP 1506, 054 (2015) doi:10.1007/JHEP06(2015)054 [arXiv:1504.04330 [hep-th]].
[10] I. Bena, C. W. Wang and N. P. Warner, “Mergers and typical black hole microstates,”
JHEP 0611, 042 (2006) doi:10.1088/1126-6708/2006/11/042 [hep-th/0608217].
[11] I. Bena, N. Bobev, S. Giusto, C. Ruef and N. P. Warner, “An Infinite-Dimensional
Family of Black-Hole Microstate Geometries,” JHEP 1103, 022 (2011) Erratum:
[JHEP 1104, 059 (2011)] doi:10.1007/JHEP03(2011)022, 10.1007/JHEP04(2011)059
[arXiv:1006.3497 [hep-th]].
45
[12] P. Heidmann, “Four-center bubbled BPS solutions with a Gibbons-Hawking base,”
JHEP 1710, 009 (2017) doi:10.1007/JHEP10(2017)009 [arXiv:1703.10095 [hep-th]].
[13] I. Bena, P. Heidmann and P. F. Ramirez, “A systematic construction of microstate geometries with low angular momentum,” JHEP 1710, 217 (2017)
doi:10.1007/JHEP10(2017)217 [arXiv:1709.02812 [hep-th]].
[14] I. Bena and N. P. Warner, “Bubbling supertubes and foaming black holes,” Phys. Rev.
D 74, 066001 (2006) doi:10.1103/PhysRevD.74.066001 [hep-th/0505166].
[15] P. Berglund, E. G. Gimon and T. S. Levi, “Supergravity microstates for BPS black
holes and black rings,” JHEP 0606, 007 (2006) doi:10.1088/1126-6708/2006/06/007
[hep-th/0505167].
[16] S. D. Mathur, A. Saxena and Y. K. Srivastava, “Constructing ‘hair’ for the three
charge hole,” Nucl. Phys. B 680, 415 (2004) doi:10.1016/j.nuclphysb.2003.12.022 [hepth/0311092].
[17] O. Lunin, “Adding momentum to D-1 - D-5 system,” JHEP 0404, 054 (2004)
doi:10.1088/1126-6708/2004/04/054 [hep-th/0404006].
[18] S. Giusto, S. D. Mathur and A. Saxena, “Dual geometries for a set of 3-charge microstates,” Nucl. Phys. B 701, 357 (2004) doi:10.1016/j.nuclphysb.2004.09.001 [hepth/0405017].
[19] S. Giusto, S. D. Mathur and A. Saxena, “3-charge geometries and their CFT duals,”
Nucl. Phys. B 710, 425 (2005) doi:10.1016/j.nuclphysb.2005.01.009 [hep-th/0406103].
[20] S. Giusto, S. D. Mathur and Y. K. Srivastava, “A Microstate for the 3-charge black ring,”
Nucl. Phys. B 763, 60 (2007) doi:10.1016/j.nuclphysb.2006.11.009 [hep-th/0601193].
[21] J. Ford, S. Giusto and A. Saxena, “A Class of BPS time-dependent 3-charge microstates
from spectral flow,” Nucl. Phys. B 790, 258 (2008) doi:10.1016/j.nuclphysb.2007.09.008
[hep-th/0612227].
[22] S. D. Mathur and D. Turton, “Microstates at the boundary of AdS,” JHEP 1205, 014
(2012) doi:10.1007/JHEP05(2012)014 [arXiv:1112.6413 [hep-th]].
[23] S. D. Mathur and D. Turton, “Momentum-carrying waves on D1-D5 microstate
geometries,” Nucl. Phys. B 862, 764 (2012) doi:10.1016/j.nuclphysb.2012.05.014
[arXiv:1202.6421 [hep-th]].
46
[24] O. Lunin, S. D. Mathur and D. Turton, “Adding momentum to supersymmetric geometries,” Nucl. Phys. B 868, 383 (2013) doi:10.1016/j.nuclphysb.2012.11.017
[arXiv:1208.1770 [hep-th]].
[25] S. Giusto and R. Russo, “Superdescendants of the D1D5 CFT and their dual 3-charge
geometries,” JHEP 1403, 007 (2014) doi:10.1007/JHEP03(2014)007 [arXiv:1311.5536
[hep-th]].
[26] S. Giusto, O. Lunin, S. D. Mathur and D. Turton, “D1-D5-P microstates at the cap,”
JHEP 1302, 050 (2013) doi:10.1007/JHEP02(2013)050 [arXiv:1211.0306 [hep-th]].
[27] I. Bena, S. El-Showk and B. Vercnocke, “Black Holes in String Theory,” Springer Proc.
Phys. 144, 59 (2013). doi:10.1007/978-3-319-00215-6 2
[28] N. P. Warner, “Lectures on Microstate Geometries,” arXiv:1912.13108 [hep-th].
[29] I. Bena, S. Giusto, R. Russo, M. Shigemori and N. P. Warner, “Habemus Superstratum! A constructive proof of the existence of superstrata,” JHEP 1505, 110 (2015)
doi:10.1007/JHEP05(2015)110 [arXiv:1503.01463 [hep-th]].
[30] I. Bena, J. de Boer, M. Shigemori and N. P. Warner, “Double, Double Supertube
Bubble,” JHEP 1110, 116 (2011) doi:10.1007/JHEP10(2011)116 [arXiv:1107.2650 [hepth]].
[31] D. Mateos and P. K. Townsend, “Supertubes,” Phys. Rev. Lett. 87, 011602 (2001)
doi:10.1103/PhysRevLett.87.011602 [hep-th/0103030].
[32] J. de Boer and M. Shigemori, “Exotic branes and non-geometric backgrounds,” Phys.
Rev. Lett. 104, 251603 (2010) doi:10.1103/PhysRevLett.104.251603 [arXiv:1004.2521
[hep-th]].
[33] J. de Boer and M. Shigemori, “Exotic Branes in String Theory,” Phys. Rept. 532, 65
(2013) doi:10.1016/j.physrep.2013.07.003 [arXiv:1209.6056 [hep-th]].
[34] J. B. Gutowski, D. Martelli and H. S. Reall, “All Supersymmetric solutions of minimal
supergravity in six- dimensions,” Class. Quant. Grav. 20, 5049 (2003) doi:10.1088/02649381/20/23/008 [hep-th/0306235].
[35] M. Cariglia and O. A. P. Mac Conamhna, “The General form of supersymmetric solutions of N=(1,0) U(1) and SU(2) gauged supergravities in six-dimensions,” Class.
Quant. Grav. 21, 3171 (2004) doi:10.1088/0264-9381/21/13/006 [hep-th/0402055].
47
[36] I. Bena, S. Giusto, M. Shigemori and N. P. Warner, “Supersymmetric Solutions in Six Dimensions: A Linear Structure,” JHEP 1203, 084 (2012)
doi:10.1007/JHEP03(2012)084 [arXiv:1110.2781 [hep-th]].
[37] S. Giusto, S. Rawash and D. Turton, “Ads3 holography at dimension two,” JHEP 1907,
171 (2019) doi:10.1007/JHEP07(2019)171 [arXiv:1904.12880 [hep-th]].
[38] S. Giusto, R. Russo and D. Turton, “New D1-D5-P geometries from string amplitudes,”
JHEP 1111, 062 (2011) doi:10.1007/JHEP11(2011)062 [arXiv:1108.6331 [hep-th]].
[39] S. Giusto and R. Russo, “Perturbative superstrata,” Nucl. Phys. B 869, 164 (2013)
doi:10.1016/j.nuclphysb.2012.12.012 [arXiv:1211.1957 [hep-th]].
[40] S. Giusto, L. Martucci, M. Petrini and R. Russo, “6D microstate geometries from
10D structures,” Nucl. Phys. B 876, 509 (2013) doi:10.1016/j.nuclphysb.2013.08.018
[arXiv:1306.1745 [hep-th]].
[41] I. Bena, E. Martinec, D. Turton and N. P. Warner, “Momentum Fractionation on Superstrata,” JHEP 1605, 064 (2016) doi:10.1007/JHEP05(2016)064 [arXiv:1601.05805
[hep-th]].
[42] I. Bena, S. Giusto, E. J. Martinec, R. Russo, M. Shigemori, D. Turton and N. P. Warner,
“Smooth horizonless geometries deep inside the black-hole regime,” Phys. Rev. Lett.
117, no. 20, 201601 (2016) doi:10.1103/PhysRevLett.117.201601 [arXiv:1607.03908
[hep-th]].
[43] I. Bena, E. Martinec, D. Turton and N. P. Warner, “M-theory Superstrata and the MSW
String,” JHEP 1706, 137 (2017) doi:10.1007/JHEP06(2017)137 [arXiv:1703.10171 [hepth]].
[44] I. Bena, S. Giusto, E. J. Martinec, R. Russo, M. Shigemori, D. Turton and N. P. Warner,
“Asymptotically-flat supergravity solutions deep inside the black-hole regime,” JHEP
1802, 014 (2018) doi:10.1007/JHEP02(2018)014 [arXiv:1711.10474 [hep-th]].
[45] E. Bakhshaei and A. Bombini, “Three-charge superstrata with internal excitations,” Class. Quant. Grav. 36, no. 5, 055001 (2019) doi:10.1088/1361-6382/ab01bc
[arXiv:1811.00067 [hep-th]].
[46] N. Ceplak, R. Russo and M. Shigemori, “Supercharging Superstrata,” JHEP 1903, 095
(2019) doi:10.1007/JHEP03(2019)095 [arXiv:1812.08761 [hep-th]].
[47] P. Heidmann and N. P. Warner, “Superstratum Symbiosis,” JHEP 1909, 059 (2019)
doi:10.1007/JHEP09(2019)059 [arXiv:1903.07631 [hep-th]].
48
[48] S. Giusto, E. Moscato and R. Russo, “AdS3 holography for 1/4 and 1/8 BPS geometries,” JHEP 1511, 004 (2015) doi:10.1007/JHEP11(2015)004 [arXiv:1507.00945 [hepth]].
[49] J. R. David, G. Mandal and S. R. Wadia, “Microscopic formulation of black holes in
string theory,” Phys. Rept. 369, 549 (2002) doi:10.1016/S0370-1573(02)00271-5 [hepth/0203048].
[50] S. G. Avery, “Using the D1D5 CFT to Understand Black Holes,” arXiv:1012.0072 [hepth].
[51] C. Vafa, “Instantons on D-branes,” Nucl. Phys. B 463, 435 (1996) doi:10.1016/05503213(96)00075-2 [hep-th/9512078].
[52] E. Witten, “On the conformal field theory of the Higgs branch,” JHEP 9707, 003 (1997)
doi:10.1088/1126-6708/1997/07/003 [hep-th/9707093].
[53] J. M. Maldacena, G. W. Moore and A. Strominger, “Counting BPS black holes in
toroidal Type II string theory,” hep-th/9903163.
[54] J. M. Maldacena and A. Strominger, “AdS(3) black holes and a stringy exclusion principle,” JHEP 9812, 005 (1998) doi:10.1088/1126-6708/1998/12/005 [hep-th/9804085].
[55] C. Vafa and E. Witten, “A Strong coupling test of S duality,” Nucl. Phys. B 431, 3
(1994) doi:10.1016/0550-3213(94)90097-3 [hep-th/9408074].
[56] S. Deger, A. Kaya, E. Sezgin and P. Sundell, “Spectrum of D = 6, N=4b supergravity
on AdS in three-dimensions x S**3,” Nucl. Phys. B 536, 110 (1998) doi:10.1016/S05503213(98)00555-0 [hep-th/9804166].
[57] F. Larsen, “The Perturbation spectrum of black holes in N=8 supergravity,” Nucl. Phys.
B 536, 258 (1998) doi:10.1016/S0550-3213(98)00564-1 [hep-th/9805208].
[58] J. de Boer, “Six-dimensional supergravity on S**3 x AdS(3) and 2-D conformal
field theory,” Nucl. Phys. B 548, 139 (1999) doi:10.1016/S0550-3213(99)00160-1 [hepth/9806104].
[59] J. de Boer, K. Papadodimas and E. Verlinde, “Black Hole Berry Phase,” Phys. Rev.
Lett. 103, 131301 (2009) doi:10.1103/PhysRevLett.103.131301 [arXiv:0809.5062 [hepth]].
[60] 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) doi:10.1016/S03701573(99)00083-6 [hep-th/9905111].
49
[61] K. Skenderis and M. Taylor, “Fuzzball solutions and D1-D5 microstates,” Phys. Rev.
Lett. 98, 071601 (2007) doi:10.1103/PhysRevLett.98.071601 [hep-th/0609154].
[62] I. Kanitscheider, K. Skenderis and M. Taylor, “Holographic anatomy of fuzzballs,”
JHEP 0704, 023 (2007) doi:10.1088/1126-6708/2007/04/023 [hep-th/0611171].
[63] M.
Shigemori,
“Counting
Superstrata,”
JHEP
1910,
017
(2019)
doi:10.1007/JHEP10(2019)017 [arXiv:1907.03878 [hep-th]].
[64] M. A. Walton, “The Heterotic String on the Simplest Calabi-yau Manifold and Its
Orbifold Limits,” Phys. Rev. D 37, 377 (1988). doi:10.1103/PhysRevD.37.377
[65] I. Bena, M. Shigemori and N. P. Warner, “Black-Hole Entropy from Supergravity Superstrata States,” JHEP 1410, 140 (2014) doi:10.1007/JHEP10(2014)140 [arXiv:1406.4506
[hep-th]].
[66] R. Dijkgraaf, G. W. Moore, E. P. Verlinde and H. L. Verlinde, “Elliptic genera of
symmetric products and second quantized strings,” Commun. Math. Phys. 185, 197
(1997) doi:10.1007/s002200050087 [hep-th/9608096].
[67] J. de Boer, “Large N elliptic genus and AdS / CFT correspondence,” JHEP 9905, 017
(1999) doi:10.1088/1126-6708/1999/05/017 [hep-th/9812240].
[68] S. Hampton, S. D. Mathur and I. G. Zadeh, “Lifting of D1-D5-P states,” JHEP 1901,
075 (2019) doi:10.1007/JHEP01(2019)075 [arXiv:1804.10097 [hep-th]].
[69] B. Guo and S. D. Mathur, “Lifting of level-1 states in the D1D5 CFT,” arXiv:1912.05567
[hep-th].
[70] G. Bossard and S. L¨
ust, “Microstate geometries at a generic point in moduli space,”
Gen. Rel. Grav. 51, no. 9, 112 (2019) doi:10.1007/s10714-019-2584-4 [arXiv:1905.12012
[hep-th]].
[71] A. Tyukov, R. Walker and N. P. Warner, “The Structure of BPS Equations for
Ambi-polar Microstate Geometries,” Class. Quant. Grav. 36, no. 1, 015021 (2019)
doi:10.1088/1361-6382/aaf133 [arXiv:1807.06596 [hep-th]].
[72] R. Walker, “D1-D5-P superstrata in 5 and 6 dimensions: separable wave equations and prepotentials,” JHEP 1909, 117 (2019) doi:10.1007/JHEP09(2019)117
[arXiv:1906.04200 [hep-th]].
[73] S. Giusto and R. Russo, “Adding new hair to the 3-charge black ring,” Class. Quant.
Grav. 29, 085006 (2012) doi:10.1088/0264-9381/29/8/085006 [arXiv:1201.2585 [hepth]].
50
[74] H. Nishino and E. Sezgin, “Matter and Gauge Couplings of N=2 Supergravity in SixDimensions,” Phys. Lett. 144B, 187 (1984). doi:10.1016/0370-2693(84)91800-8
[75] H. Nishino and E. Sezgin, “The Complete N = 2, d = 6 Supergravity With Matter and Yang-Mills Couplings,” Nucl. Phys. B 278, 353 (1986). doi:10.1016/05503213(86)90218-X
[76] H. Het Lam and S. Vandoren, “BPS solutions of six-dimensional (1, 0) supergravity
coupled to tensor multiplets,” JHEP 1806, 021 (2018) doi:10.1007/JHEP06(2018)021
[arXiv:1804.04681 [hep-th]].
[77] P. A. Cano and T. Ortin, “The structure of all the supersymmetric solutions of ungauged N = (1, 0), d = 6 supergravity,” Class. Quant. Grav. 36, no. 12, 125007 (2019)
doi:10.1088/1361-6382/ab1f1e [arXiv:1804.04945 [hep-th]].
[78] M. Shigemori, “Perturbative 3-charge microstate geometries in six dimensions,” JHEP
1310, 169 (2013) doi:10.1007/JHEP10(2013)169 [arXiv:1307.3115 [hep-th]].
[79] I. Bena, D. Turton, R. Walker and N. P. Warner, “Integrability and BlackHole Microstate Geometries,” JHEP 1711, 021 (2017) doi:10.1007/JHEP11(2017)021
[arXiv:1709.01107 [hep-th]].
[80] B. E. Niehoff and N. P. Warner, “Doubly-Fluctuating BPS Solutions in Six Dimensions,”
JHEP 1310, 137 (2013) doi:10.1007/JHEP10(2013)137 [arXiv:1303.5449 [hep-th]].
[81] J. de Boer, S. El-Showk, I. Messamah and D. Van den Bleeken, “A Bound on
the entropy of supergravity?,” JHEP 1002, 062 (2010) doi:10.1007/JHEP02(2010)062
[arXiv:0906.0011 [hep-th]].
[82] A. Tyukov, R. Walker and N. P. Warner, “Tidal Stresses and Energy Gaps in Microstate
Geometries,” JHEP 1802, 122 (2018) doi:10.1007/JHEP02(2018)122 [arXiv:1710.09006
[hep-th]].
[83] S. Raju and P. Shrivastava, “Critique of the fuzzball program,” Phys. Rev. D 99, no.
6, 066009 (2019) doi:10.1103/PhysRevD.99.066009 [arXiv:1804.10616 [hep-th]].
[84] I. Bena, P. Heidmann and D. Turton, “AdS2 holography: mind the cap,” JHEP 1812,
028 (2018) doi:10.1007/JHEP12(2018)028 [arXiv:1806.02834 [hep-th]].
[85] M. Bianchi, D. Consoli, A. Grillo and J. F. Morales, “The dark side of fuzzball geometries,” JHEP 1905, 126 (2019) doi:10.1007/JHEP05(2019)126 [arXiv:1811.02397
[hep-th]].
51
[86] I. Bena, E. J. Martinec, R. Walker and N. P. Warner, “Early Scrambling and
Capped BTZ Geometries,” JHEP 1904, 126 (2019) doi:10.1007/JHEP04(2019)126
[arXiv:1812.05110 [hep-th]].
[87] A. Bombini and A. Galliani, “AdS3 four-point functions from 18 -BPS states,” JHEP
1906, 044 (2019) doi:10.1007/JHEP06(2019)044 [arXiv:1904.02656 [hep-th]].
[88] J. Tian, J. Hou and B. Chen, “Holographic Correlators on Integrable Superstrata,” Nucl.
Phys. B 948, 114766 (2019) doi:10.1016/j.nuclphysb.2019.114766 [arXiv:1904.04532
[hep-th]].
[89] I. Bena, P. Heidmann, R. Monten and N. P. Warner, “Thermal Decay without Information Loss in Horizonless Microstate Geometries,” SciPost Phys. 7, no. 5, 063 (2019)
doi:10.21468/SciPostPhys.7.5.063 [arXiv:1905.05194 [hep-th]].
[90] I. Bena and A. Tyukov, “BTZ Trailing Strings,” arXiv:1911.12821 [hep-th].
[91] P. Heidmann, D. R. Mayerson, R. Walker and N. P. Warner, “Holomorphic Waves of
Black Hole Microstructure,” arXiv:1910.10714 [hep-th].
[92] J. M. Maldacena, A. Strominger and E. Witten, “Black hole entropy in M theory,”
JHEP 9712, 002 (1997) doi:10.1088/1126-6708/1997/12/002 [hep-th/9711053].
[93] F. Denef, D. Gaiotto, A. Strominger, D. Van den Bleeken and X. Yin, “Black
Hole Deconstruction,” JHEP 1203, 071 (2012) doi:10.1007/JHEP03(2012)071 [hepth/0703252].
[94] J. de Boer, S. El-Showk, I. Messamah and D. Van den Bleeken, “Quantizing N=2
Multicenter Solutions,” JHEP 0905, 002 (2009) doi:10.1088/1126-6708/2009/05/002
[arXiv:0807.4556 [hep-th]].
[95] E. G. Gimon and T. S. Levi, “Black Ring Deconstruction,” JHEP 0804, 098 (2008)
doi:10.1088/1126-6708/2008/04/098 [arXiv:0706.3394 [hep-th]].
[96] E. J. Martinec and B. E. Niehoff, “Hair-brane Ideas on the Horizon,” JHEP 1511, 195
(2015) doi:10.1007/JHEP11(2015)195 [arXiv:1509.00044 [hep-th]].
[97] A. Tyukov and N. P. Warner, “Supersymmetry and Wrapped Branes in Microstate
Geometries,” JHEP 1710, 011 (2017) doi:10.1007/JHEP10(2017)011 [arXiv:1608.04023
[hep-th]].
[98] P. Roy, Y. K. Srivastava and A. Virmani, “Hair on non-extremal D1-D5 bound states,”
JHEP 1609, 145 (2016) doi:10.1007/JHEP09(2016)145 [arXiv:1607.05405 [hep-th]].
52
[99] A. Bombini and S. Giusto, “Non-extremal superdescendants of the D1D5 CFT,” JHEP
1710, 023 (2017) doi:10.1007/JHEP10(2017)023 [arXiv:1706.09761 [hep-th]].
[100] I. Bena, S. Giusto, C. Ruef and N. P. Warner, “Supergravity Solutions from Floating
Branes,” JHEP 1003, 047 (2010) doi:10.1007/JHEP03(2010)047 [arXiv:0910.1860 [hepth]].
[101] E. J. Martinec and S. Massai, “String Theory of Supertubes,” JHEP 1807, 163 (2018)
doi:10.1007/JHEP07(2018)163 [arXiv:1705.10844 [hep-th]].
[102] E. J. Martinec, S. Massai and D. Turton, “String dynamics in NS5-F1-P geometries,”
arXiv:1803.08505 [hep-th].
[103] E. J. Martinec, S. Massai and D. Turton, “Little Strings, Long Strings, and Fuzzballs,”
JHEP 1911, 019 (2019) doi:10.1007/JHEP11(2019)019 [arXiv:1906.11473 [hep-th]].
[104] K. Skenderis and M. Taylor, “The fuzzball proposal for black holes,” Phys. Rept. 467,
117 (2008) doi:10.1016/j.physrep.2008.08.001 [arXiv:0804.0552 [hep-th]].
[105] M. Baggio, J. de Boer and K. Papadodimas, “A non-renormalization theorem for chiral primary 3-point functions,” JHEP 1207, 137 (2012) doi:10.1007/JHEP07(2012)137
[arXiv:1203.1036 [hep-th]].
[106] A. Galliani, S. Giusto and R. Russo, “Holographic 4-point correlators with heavy
states,” JHEP 1710, 040 (2017) doi:10.1007/JHEP10(2017)040 [arXiv:1705.09250 [hepth]].
[107] A. Bombini, A. Galliani, S. Giusto, E. Moscato and R. Russo, “Unitary 4point correlators from classical geometries,” Eur. Phys. J. C 78, no. 1, 8 (2018)
doi:10.1140/epjc/s10052-017-5492-3 [arXiv:1710.06820 [hep-th]].
[108] S. Giusto, R. Russo and C. Wen, “Holographic correlators in AdS3 ,” JHEP 1903, 096
(2019) doi:10.1007/JHEP03(2019)096 [arXiv:1812.06479 [hep-th]].
[109] J. Garcia i Tormo and M. Taylor, “One point functions for black hole microstates,”
Gen. Rel. Grav. 51, no. 7, 89 (2019) doi:10.1007/s10714-019-2566-6 [arXiv:1904.10200
[hep-th]].
[110] F. C. Eperon, H. S. Reall and J. E. Santos, “Instability of supersymmetric microstate
geometries,” JHEP 1610, 031 (2016) doi:10.1007/JHEP10(2016)031 [arXiv:1607.06828
[hep-th]].
[111] J. Keir, “Wave propagation on microstate geometries,” arXiv:1609.01733 [gr-qc].
53
[112] F. C. Eperon, “Geodesics in supersymmetric micro state geometries,” Class. Quant.
Grav. 34, no. 16, 165003 (2017) doi:10.1088/1361-6382/aa7bfe [arXiv:1702.03975 [grqc]].
[113] D. Marolf, B. Michel and A. Puhm, “A rough end for smooth microstate geometries,”
JHEP 1705, 021 (2017) doi:10.1007/JHEP05(2017)021 [arXiv:1612.05235 [hep-th]].
[114] A. Dabholkar, J. Gomes, S. Murthy and A. Sen, “Supersymmetric Index from Black
Hole Entropy,” JHEP 1104, 034 (2011) doi:10.1007/JHEP04(2011)034 [arXiv:1009.3226
[hep-th]].
[115] A. Chowdhury, R. S. Garavuso, S. Mondal and A. Sen, “Do All BPS Black
Hole Microstates Carry Zero Angular Momentum?,” JHEP 1604, 082 (2016)
doi:10.1007/JHEP04(2016)082 [arXiv:1511.06978 [hep-th]].
[116] S. Sachdev and J. Ye, “Gapless spin fluid ground state in a random, quantum Heisenberg
magnet,” Phys. Rev. Lett. 70, 3339 (1993) doi:10.1103/PhysRevLett.70.3339 [condmat/9212030].
[117] A. Kitaev, “A simple model of quantum holography,” KITP strings seminar
and Entanglement 2015 program (Feb. 12, April 7, and May 27, 2015) .
http://online.kitp.ucsb.edu/online/entangled15/.
[118] G. S´arosi, “AdS2 holography and the SYK model,” PoS Modave 2017, 001 (2018)
doi:10.22323/1.323.0001 [arXiv:1711.08482 [hep-th]].
[119] J. M. Maldacena, J. Michelson and A. Strominger, “Anti-de Sitter fragmentation,”
JHEP 9902, 011 (1999) doi:10.1088/1126-6708/1999/02/011 [hep-th/9812073].
[120] A. Almheiri and J. Polchinski, “Models of AdS2 backreaction and holography,” JHEP
1511, 014 (2015) doi:10.1007/JHEP11(2015)014 [arXiv:1402.6334 [hep-th]].
[121] I. Bena, M. Berkooz, J. de Boer, S. El-Showk and D. Van den Bleeken, “Scaling BPS Solutions and pure-Higgs States,” JHEP 1211, 171 (2012) doi:10.1007/JHEP11(2012)171
[arXiv:1205.5023 [hep-th]].
[122] P. Heidmann and S. Mondal, “The full space of BPS multicenter states with
pure D-brane charges,” JHEP 1906, 011 (2019) doi:10.1007/JHEP06(2019)011
[arXiv:1810.10019 [hep-th]].
[123] M. Bianchi, D. Consoli and J. F. Morales, “Probing Fuzzballs with Particles, Waves
and Strings,” JHEP 1806, 157 (2018) doi:10.1007/JHEP06(2018)157 [arXiv:1711.10287
[hep-th]].
54
[124] S. S. Gubser, “Drag force in AdS/CFT,” Phys. Rev. D 74, 126005 (2006)
doi:10.1103/PhysRevD.74.126005 [hep-th/0605182].
55
...