[1] S. Aoki and J. Balog, HKLL bulk reconstruction for small ∆, JHEP 02 (2022) 015
[arXiv:2112.04326] [INSPIRE].
[2] J.M. Maldacena, The Large N limit of superconformal field theories and supergravity, Adv.
Theor. Math. Phys. 2 (1998) 231 [hep-th/9711200] [INSPIRE].
[3] E. Witten, Anti-de Sitter space and holography, Adv. Theor. Math. Phys. 2 (1998) 253
[hep-th/9802150] [INSPIRE].
[4] A. Hamilton, D.N. Kabat, G. Lifschytz and D.A. Lowe, Local bulk operators in AdS/CFT: A
Boundary view of horizons and locality, Phys. Rev. D 73 (2006) 086003 [hep-th/0506118]
[INSPIRE].
[5] A. Hamilton, D.N. Kabat, G. Lifschytz and D.A. Lowe, Holographic representation of local
bulk operators, Phys. Rev. D 74 (2006) 066009 [hep-th/0606141] [INSPIRE].
[6] D. Kabat, G. Lifschytz, S. Roy and D. Sarkar, Holographic representation of bulk fields with
spin in AdS/CFT, Phys. Rev. D 86 (2012) 026004 [arXiv:1204.0126] [INSPIRE].
[7] T. De Jonckheere, Modave lectures on bulk reconstruction in AdS/CFT, PoS Modave2017
(2018) 005 [arXiv:1711.07787] [INSPIRE].
[8] D. Harlow, TASI Lectures on the Emergence of Bulk Physics in AdS/CFT, PoS TASI2017
(2018) 002 [arXiv:1802.01040] [INSPIRE].
[9] N. Kajuri, Lectures on Bulk Reconstruction, SciPost Phys. Lect. Notes 22 (2021) 1
[arXiv:2003.00587] [INSPIRE].
[10] S. Bhowmick, K. Ray and S. Sen, Holography in de Sitter and anti-de Sitter Spaces and
Gel’fand Graev Radon transform, Phys. Lett. B 798 (2019) 134977 [arXiv:1903.07336]
[INSPIRE].
– 35 –
JHEP05(2023)034
• From the recursion (G.24) and (G.25), we can calculate the value of the coefficients
− 1)(−1)a π
Γ(∆)(−1)a π
−d Γ(∆
−d
f0 = 2
πc = 2
(I.7)
2π d/2 Γ(D/2)Γ(ν + 1)
Γ d−1
Γ(ν + 2)π d/2
[11] D. Kabat and G. Lifschytz, CFT representation of interacting bulk gauge fields in AdS, Phys.
Rev. D 87 (2013) 086004 [arXiv:1212.3788] [INSPIRE].
[12] I. Heemskerk, Construction of Bulk Fields with Gauge Redundancy, JHEP 09 (2012) 106
[arXiv:1201.3666] [INSPIRE].
[13] D. Kabat and G. Lifschytz, Decoding the hologram: Scalar fields interacting with gravity,
Phys. Rev. D 89 (2014) 066010 [arXiv:1311.3020] [INSPIRE].
[14] D. Sarkar and X. Xiao, Holographic Representation of Higher Spin Gauge Fields, Phys. Rev.
D 91 (2015) 086004 [arXiv:1411.4657] [INSPIRE].
[16] D. Kabat, G. Lifschytz and D.A. Lowe, Constructing local bulk observables in interacting
AdS/CFT, Phys. Rev. D 83 (2011) 106009 [arXiv:1102.2910] [INSPIRE].
[17] I. Heemskerk, D. Marolf, J. Polchinski and J. Sully, Bulk and Transhorizon Measurements in
AdS/CFT, JHEP 10 (2012) 165 [arXiv:1201.3664] [INSPIRE].
[18] I.R. Klebanov and E. Witten, AdS / CFT correspondence and symmetry breaking, Nucl.
Phys. B 556 (1999) 89 [hep-th/9905104] [INSPIRE].
[19] I.R. Klebanov and A.M. Polyakov, AdS dual of the critical O(N) vector model, Phys. Lett. B
550 (2002) 213 [hep-th/0210114] [INSPIRE].
[20] E. Sezgin and P. Sundell, Massless higher spins and holography, Nucl. Phys. B 644 (2002)
303 [hep-th/0205131] [INSPIRE].
[21] N. Del Grosso, A. Garbarz, G. Palau and G. Pérez-Nadal, Boundary-to-bulk maps for AdS
causal wedges and RG flow, JHEP 10 (2019) 135 [arXiv:1908.05738] [INSPIRE].
[22] T. Banks, M.R. Douglas, G.T. Horowitz and E.J. Martinec, AdS dynamics from conformal
field theory, hep-th/9808016 [INSPIRE].
[23] E. D’Hoker and D.Z. Freedman, Supersymmetric gauge theories and the AdS / CFT
correspondence, in the proceedings of the Theoretical Advanced Study Institute in Elementary
Particle Physics (TASI 2001), Strings, Branes and EXTRA Dimensions (2002), pp. 3–158
[hep-th/0201253] [INSPIRE].
[24] S. Aoki, J. Balog, T. Onogi and S. Yokoyama, Special flow equation and the GKP–Witten
relation, PTEP 2023 (2023) 013B03 [arXiv:2204.06855] [INSPIRE].
[25] B. Bhattacharjee, C. Krishnan and D. Sarkar, HKLL for the non-normalizable mode, JHEP
12 (2022) 075 [arXiv:2209.01130] [INSPIRE].
– 36 –
JHEP05(2023)034
[15] V.F. Foit, D. Kabat and G. Lifschytz, Bulk reconstruction for spinor fields in AdS/CFT,
JHEP 02 (2020) 129 [arXiv:1912.00952] [INSPIRE].
...