CFT Dual for Timelike Geodesic in Lorentzian dS
Pith reviewed 2026-06-30 08:58 UTC · model grok-4.3
The pith
Analytic continuation from Lorentzian de Sitter yields a PT defect whose state reproduces the Bunch-Davies Wightman function.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central claim is that analytic continuation produces a PT defect in the CFT dual that defines a PT-invariant state reproducing the Bunch-Davies Wightman function; the single-geodesic version, built from the timelike geodesic-integrated Wightman function, yields correlators between a bulk operator and a linear combination of an OPE block and its Casimir partner, while the associated conformal defect and anomaly follow from an integral identity of the dS/CFT symmetry group.
What carries the argument
The PT defect obtained by analytic continuation from Lorentzian dS to Euclidean CFT, which enforces PT invariance and supplies the state matching the Bunch-Davies Wightman function.
If this is right
- The dual state reproduces the full Bunch-Davies Wightman function.
- Correlators connect a bulk operator to a linear combination of an OPE block and its Casimir partner.
- The conformal defect and anomaly are derived from an integral identity of the dS/CFT symmetry group.
- Entanglement entropy from the construction captures only the real part of the central charge.
Where Pith is reading between the lines
- The PT-invariant state construction may extend to other choices of vacuum in de Sitter if the continuation preserves further symmetries.
- The linear combination of OPE block and Casimir partner may appear in other holographic calculations that integrate along timelike paths.
- The group-theoretic derivation of the anomaly suggests that similar integral identities could produce defects in related dualities.
Load-bearing premise
Analytic continuation from Lorentzian dS_{d+1} to Euclidean CFT_d preserves PT invariance and reproduces the full Bunch-Davies Wightman function without additional adjustments.
What would settle it
An explicit calculation for a specific scalar mass showing that the PT-defect correlator after continuation deviates from the known Bunch-Davies Wightman function.
Figures
read the original abstract
We construct the Euclidean CFT$_{d}$ dual of a generic massive scalar in Lorentzian dS$_{d+1}$ via analytic continuation. The resulting $PT$ defect defines a $PT$-invariant state that reproduces the Bunch-Davies Wightman function. However, the entanglement entropy captures only the real part of the central charge. This motivates a single-geodesic dual based on the timelike geodesic-integrated Wightman function, which yields the correlators between a bulk operator and a linear combination of an OPE block and its Casimir partner. We also derive the associated conformal defect and anomaly from an integral identity of the dS/CFT symmetry group.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript constructs the Euclidean CFT_d dual of a generic massive scalar in Lorentzian dS_{d+1} via analytic continuation. The resulting PT defect defines a PT-invariant state reproducing the Bunch-Davies Wightman function. Entanglement entropy is noted to capture only the real part of the central charge, motivating a single-geodesic dual based on the timelike geodesic-integrated Wightman function. This yields correlators between a bulk operator and a linear combination of an OPE block and its Casimir partner. The associated conformal defect and anomaly are derived from an integral identity of the dS/CFT symmetry group.
Significance. If the constructions hold, the work could advance the dS/CFT correspondence by linking timelike geodesics to CFT operators via analytic continuation and geodesic integration, while addressing limitations in entanglement entropy for the central charge. The symmetry-group derivation of the anomaly, if shown to be independent of auxiliary choices, would be a concrete technical contribution.
major comments (1)
- [Abstract] Abstract (and the central construction): the assertion that analytic continuation from Lorentzian dS_{d+1} to Euclidean CFT_d produces a PT defect whose state exactly reproduces the full complex Bunch-Davies Wightman function (including its imaginary part) is load-bearing for all subsequent claims. No explicit identity is supplied showing that the continuation commutes with the PT operator or preserves the iε prescription without extra real/imaginary terms; if such terms appear, the equality between the geodesic-integrated Wightman function and the OPE-block-plus-Casimir-partner combination fails, and the derived anomaly is incorrect.
minor comments (1)
- The abstract refers to 'an integral identity of the dS/CFT symmetry group' without naming the identity or the relevant group element; adding an equation number or reference in the main text would improve clarity.
Simulated Author's Rebuttal
We thank the referee for their careful reading and constructive comments on our manuscript. The major concern regarding the analytic continuation, PT defect, and explicit verification of the full complex Wightman function is addressed point-by-point below. We will incorporate additional explicit identities in the revision to substantiate the central construction.
read point-by-point responses
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Referee: [Abstract] Abstract (and the central construction): the assertion that analytic continuation from Lorentzian dS_{d+1} to Euclidean CFT_d produces a PT defect whose state exactly reproduces the full complex Bunch-Davies Wightman function (including its imaginary part) is load-bearing for all subsequent claims. No explicit identity is supplied showing that the continuation commutes with the PT operator or preserves the iε prescription without extra real/imaginary terms; if such terms appear, the equality between the geodesic-integrated Wightman function and the OPE-block-plus-Casimir-partner combination fails, and the derived anomaly is incorrect.
Authors: We agree that the manuscript would benefit from an explicit identity demonstrating commutation of analytic continuation with the PT operator and preservation of the iε prescription. In the revised version we will add a dedicated calculation (new subsection in Section 3) using the mode expansion of the massive scalar. This shows that the continued correlator matches the full complex Bunch-Davies Wightman function, with the imaginary part arising precisely from the standard iε contour without extraneous real or imaginary contributions. The PT invariance of the defect follows directly from the reality properties of the hypergeometric functions under the continuation map. With this addition the subsequent geodesic-integrated dual and anomaly derivations remain valid. revision: yes
Circularity Check
PT defect reproduction of BD Wightman function is by construction of the analytic continuation
specific steps
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self definitional
[Abstract]
"We construct the Euclidean CFT$_{d}$ dual of a generic massive scalar in Lorentzian dS$_{d+1}$ via analytic continuation. The resulting $PT$ defect defines a $PT$-invariant state that reproduces the Bunch-Davies Wightman function."
The PT defect is introduced precisely as the object obtained from the analytic continuation; the claim that its state reproduces the BD Wightman function is therefore built into the definition of the object rather than obtained as a separate result.
full rationale
The paper's central construction begins by defining the Euclidean CFT dual via analytic continuation from Lorentzian dS, resulting in a PT defect whose associated state is stated to reproduce the Bunch-Davies Wightman function. This reproduction is presented as a direct consequence of the definition rather than derived from an independent identity or verification. All downstream claims (single-geodesic dual, OPE block correlators, conformal anomaly) rest on this equality holding exactly. The provided abstract supplies the load-bearing statement but exhibits no separate check that would render the reproduction non-circular. No other patterns (fitted predictions, self-citation chains, or imported uniqueness theorems) are identifiable from the given text.
Axiom & Free-Parameter Ledger
Reference graph
Works this paper leans on
-
[1]
Dimensional Reduction in Quantum Gravity
G. ’t Hooft, “Dimensional reduction in quantum gravity,” Conf. Proc. C930308, 284-296 (1993) [arXiv:gr-qc/9310026 [gr-qc]]
work page internal anchor Pith review Pith/arXiv arXiv 1993
-
[2]
L. Susskind, “The World as a hologram,” J. Math. Phys.36, 6377-6396 (1995) doi:10.1063/1.531249 [arXiv:hep-th/9409089 [hep-th]]. 62
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1063/1.531249 1995
-
[3]
The Large N Limit of Superconformal Field Theories and Supergravity
J. M. Maldacena, “The LargeNlimit of superconformal field the- ories and supergravity,” Adv. Theor. Math. Phys.2, 231-252 (1998) doi:10.4310/ATMP.1998.v2.n2.a1 [arXiv:hep-th/9711200 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.4310/atmp.1998.v2.n2.a1 1998
-
[4]
J. D. Brown and M. Henneaux, “Central Charges in the Canonical Realization of Asymptotic Symmetries: An Example from Three-Dimensional Gravity,” Com- mun. Math. Phys.104, 207-226 (1986) doi:10.1007/BF01211590
-
[5]
(2+1)-Dimensional Gravity as an Exactly Soluble System,
E. Witten, “(2+1)-Dimensional Gravity as an Exactly Soluble System,” Nucl. Phys. B311, 46 (1988) doi:10.1016/0550-3213(88)90143-5
-
[6]
Three-Dimensional Gravity Revisited
E. Witten, “Three-Dimensional Gravity Revisited,” [arXiv:0706.3359 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv
-
[7]
Gauge Theory Correlators from Non-Critical String Theory
S. S. Gubser, I. R. Klebanov and A. M. Polyakov, “Gauge theory correlators from noncritical string theory,” Phys. Lett. B428, 105-114 (1998) doi:10.1016/S0370- 2693(98)00377-3 [arXiv:hep-th/9802109 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/s0370- 1998
-
[8]
Anti De Sitter Space And Holography
E. Witten, “Anti de Sitter space and holography,” Adv. Theor. Math. Phys.2, 253-291 (1998) doi:10.4310/ATMP.1998.v2.n2.a2 [arXiv:hep-th/9802150 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.4310/atmp.1998.v2.n2.a2 1998
-
[9]
Bulk vs. Boundary Dynamics in Anti-de Sitter Spacetime
V. Balasubramanian, P. Kraus and A. E. Lawrence, “Bulk versus bound- ary dynamics in anti-de Sitter space-time,” Phys. Rev. D59, 046003 (1999) doi:10.1103/PhysRevD.59.046003 [arXiv:hep-th/9805171 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.59.046003 1999
-
[10]
Local bulk operators in AdS/CFT: a boundary view of horizons and locality
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. D73, 086003 (2006) doi:10.1103/PhysRevD.73.086003 [arXiv:hep-th/0506118 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.73.086003 2006
-
[11]
Holographic representation of local bulk operators
A. Hamilton, D. N. Kabat, G. Lifschytz and D. A. Lowe, “Holographic representation of local bulk operators,” Phys. Rev. D74, 066009 (2006) doi:10.1103/PhysRevD.74.066009 [arXiv:hep-th/0606141 [hep-th]]. 63
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.74.066009 2006
-
[12]
Integral Geometry and Holography
B. Czech, L. Lamprou, S. McCandlish and J. Sully, “Integral Geometry and Holog- raphy,” JHEP10, 175 (2015) doi:10.1007/JHEP10(2015)175 [arXiv:1505.05515 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep10(2015)175 2015
-
[13]
A Stereoscopic Look into the Bulk
B. Czech, L. Lamprou, S. McCandlish, B. Mosk and J. Sully, “A Stereo- scopic Look into the Bulk,” JHEP07, 129 (2016) doi:10.1007/JHEP07(2016)129 [arXiv:1604.03110 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep07(2016)129 2016
-
[14]
Entanglement, Holography and Causal Diamonds
J. de Boer, F. M. Haehl, M. P. Heller and R. C. Myers, “Entanglement, hologra- phy and causal diamonds,” JHEP08, 162 (2016) doi:10.1007/JHEP08(2016)162 [arXiv:1606.03307 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep08(2016)162 2016
-
[15]
The Probe of Curvature in the Lorentzian AdS2/CFT1 Correspondence,
X. Huang and C. T. Ma, “The Probe of Curvature in the Lorentzian AdS2/CFT1 Correspondence,” Phys. Lett. B798, 134936 (2019) doi:10.1016/j.physletb.2019.134936 [arXiv:1907.01422 [hep-th]]
-
[16]
Berry Curvature and Riemann Curvature in Kinematic Space with Spherical Entangling Surface,
X. Huang and C. T. Ma, “Berry Curvature and Riemann Curvature in Kinematic Space with Spherical Entangling Surface,” Fortsch. Phys.69, no.3, 2000048 (2021) doi:10.1002/prop.202000048 [arXiv:2003.12252 [hep-th]]
-
[17]
Witten Diagrams Revisited: The AdS Geometry of Conformal Blocks
E. Hijano, P. Kraus, E. Perlmutter and R. Snively, “Witten Diagrams Re- visited: The AdS Geometry of Conformal Blocks,” JHEP01, 146 (2016) doi:10.1007/JHEP01(2016)146 [arXiv:1508.00501 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep01(2016)146 2016
-
[18]
Locality, bulk equations of motion and the conformal bootstrap
D. Kabat and G. Lifschytz, “Locality, bulk equations of motion and the conformal bootstrap,” JHEP10, 091 (2016) doi:10.1007/JHEP10(2016)091 [arXiv:1603.06800 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep10(2016)091 2016
-
[19]
A theory of reparameterizations for AdS$_3$ gravity
J. Cotler and K. Jensen, “A theory of reparameterizations for AdS3 gravity,” JHEP 02, 079 (2019) doi:10.1007/JHEP02(2019)079 [arXiv:1808.03263 [hep-th]]. 64
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep02(2019)079 2019
-
[20]
One-loop Partition Functions of 3D Gravity
S. Giombi, A. Maloney and X. Yin, “One-loop Partition Functions of 3D Gravity,” JHEP08, 007 (2008) doi:10.1088/1126-6708/2008/08/007 [arXiv:0804.1773 [hep- th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/1126-6708/2008/08/007 2008
-
[21]
X. Huang, C. T. Ma and H. Shu, “Quantum correction of the Wilson line and entanglement entropy in the pure AdS3 Einstein gravity theory,” Phys. Lett. B806, 135515 (2020) doi:10.1016/j.physletb.2020.135515 [arXiv:1911.03841 [hep-th]]
-
[22]
U(1) CS theory vs SL(2) CS for- mulation: Boundary theory and Wilson line,
X. Huang, C. T. Ma, H. Shu and C. H. Wu, “U(1) CS theory vs SL(2) CS for- mulation: Boundary theory and Wilson line,” Nucl. Phys. B984, 115971 (2022) doi:10.1016/j.nuclphysb.2022.115971 [arXiv:2011.03953 [hep-th]]
-
[23]
A. Strominger, “The dS / CFT correspondence,” JHEP10, 034 (2001) doi:10.1088/1126-6708/2001/10/034 [arXiv:hep-th/0106113 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/1126-6708/2001/10/034 2001
-
[24]
Higher Spin Realization of the dS/CFT Correspondence
D. Anninos, T. Hartman and A. Strominger, “Higher Spin Realization of the dS/CFT Correspondence,” Class. Quant. Grav.34, no.1, 015009 (2017) doi:10.1088/1361-6382/34/1/015009 [arXiv:1108.5735 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/1361-6382/34/1/015009 2017
-
[25]
Probing de Sitter space using CFT states,
K. Doi, N. Ogawa, K. Shinmyo, Y. k. Suzuki and T. Takayanagi, “Probing de Sitter space using CFT states,” JHEP02, 093 (2025) doi:10.1007/JHEP02(2025)093 [arXiv:2405.14237 [hep-th]]
-
[26]
dS/CFT Correspondence from a Defect Operator
X. Huang and C. T. Ma, “dS/CFT Correspondence from a Defect Operator,” [arXiv:2512.11759 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv
-
[27]
Real Spectra in Non-Hermitian Hamiltonians Having PT Symmetry
C. M. Bender and S. Boettcher, “Real spectra in nonHermitian Hamil- tonians having PT symmetry,” Phys. Rev. Lett.80, 5243-5246 (1998) doi:10.1103/PhysRevLett.80.5243 [arXiv:physics/9712001 [math-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevlett.80.5243 1998
-
[28]
Complex Extension of Quantum Mechanics
C. M. Bender, D. C. Brody and H. F. Jones, “Complex extension of quantum me- chanics,” Phys. Rev. Lett.89, 270401 (2002) [erratum: Phys. Rev. Lett.92, 119902 (2004)] doi:10.1103/PhysRevLett.89.270401 [arXiv:quant-ph/0208076 [quant-ph]]. 65
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevlett.89.270401 2002
-
[29]
A. Mostafazadeh, “PseudoHermiticity versus PT symmetry. The necessary con- dition for the reality of the spectrum,” J. Math. Phys.43, 205-214 (2002) doi:10.1063/1.1418246 [arXiv:math-ph/0107001 [math-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1063/1.1418246 2002
-
[30]
A. Mostafazadeh, “PseudoHermiticity versus PT symmetry 2. A Complete char- acterization of nonHermitian Hamiltonians with a real spectrum,” J. Math. Phys. 43, 2814-2816 (2002) doi:10.1063/1.1461427 [arXiv:math-ph/0110016 [math-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1063/1.1461427 2002
-
[31]
A. Mostafazadeh, “PseudoHermiticity versus PT symmetry 3: Equivalence of pseu- doHermiticity and the presence of antilinear symmetries,” J. Math. Phys.43, 3944- 3951 (2002) doi:10.1063/1.1489072 [arXiv:math-ph/0203005 [math-ph]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1063/1.1489072 2002
-
[32]
On a Factorization of Symmetric Matrices and Antilinear Symmetries
A. Mostafazadeh, “On a Factorization of Symmetric Matrices and Antilinear Sym- metries,” [arXiv:math-ph/0203023 [math-ph]]
work page internal anchor Pith review Pith/arXiv arXiv
-
[33]
Conformal Vacua and Entropy in de Sitter Space
R. Bousso, A. Maloney and A. Strominger, “Conformal vacua and entropy in de Sitter space,” Phys. Rev. D65, 104039 (2002) doi:10.1103/PhysRevD.65.104039 [arXiv:hep-th/0112218 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.65.104039 2002
-
[34]
The Boundary and Crosscap States in Conformal Field Theories,
N. Ishibashi, “The Boundary and Crosscap States in Conformal Field Theories,” Mod. Phys. Lett. A4, 251 (1989) doi:10.1142/S0217732389000320
-
[35]
Bulk Locality and Boundary Creating Operators
Y. Nakayama and H. Ooguri, “Bulk Locality and Boundary Creating Operators,” JHEP10, 114 (2015) doi:10.1007/JHEP10(2015)114 [arXiv:1507.04130 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep10(2015)114 2015
-
[36]
Holographic Representation of Local Operators In De Sitter Space
X. Xiao, “Holographic representation of local operators in de sitter space,” Phys. Rev. D90, no.2, 024061 (2014) doi:10.1103/PhysRevD.90.024061 [arXiv:1402.7080 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevd.90.024061 2014
-
[37]
Defects in conformal field theory
M. Bill` o, V. Gon¸ calves, E. Lauria and M. Meineri, “Defects in conformal field theory,” JHEP04, 091 (2016) doi:10.1007/JHEP04(2016)091 [arXiv:1601.02883 [hep-th]]. 66
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep04(2016)091 2016
-
[38]
There and back again: bulk-to-defect via Ward identities,
J. Belton and Z. Kong, “There and back again: bulk-to-defect via Ward identities,” JHEP05, 103 (2026) doi:10.1007/JHEP05(2026)103 [arXiv:2510.08519 [hep-th]]
-
[39]
Nonlinearly Realised Defect Symmetries and Anomalies,
N. Drukker, Z. Kong and P. Kravchuk, “Nonlinearly Realised Defect Symmetries and Anomalies,” [arXiv:2512.15913 [hep-th]]
-
[40]
Geometric and Renormalized Entropy in Conformal Field Theory
C. Holzhey, F. Larsen and F. Wilczek, “Geometric and renormalized entropy in conformal field theory,” Nucl. Phys. B424, 443-467 (1994) doi:10.1016/0550- 3213(94)90402-2 [arXiv:hep-th/9403108 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1016/0550- 1994
-
[41]
Holographic Derivation of Entanglement Entropy from AdS/CFT
S. Ryu and T. Takayanagi, “Holographic derivation of entangle- ment entropy from AdS/CFT,” Phys. Rev. Lett.96, 181602 (2006) doi:10.1103/PhysRevLett.96.181602 [arXiv:hep-th/0603001 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1103/physrevlett.96.181602 2006
-
[42]
Aspects of Holographic Entanglement Entropy
S. Ryu and T. Takayanagi, “Aspects of Holographic Entanglement Entropy,” JHEP 08, 045 (2006) doi:10.1088/1126-6708/2006/08/045 [arXiv:hep-th/0605073 [hep- th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1088/1126-6708/2006/08/045 2006
-
[43]
Generalized gravitational entropy
A. Lewkowycz and J. Maldacena, “Generalized gravitational entropy,” JHEP08, 090 (2013) doi:10.1007/JHEP08(2013)090 [arXiv:1304.4926 [hep-th]]
work page internal anchor Pith review Pith/arXiv arXiv doi:10.1007/jhep08(2013)090 2013
-
[44]
New holographic generalization of entanglement entropy,
Y. Nakata, T. Takayanagi, Y. Taki, K. Tamaoka and Z. Wei, “New holographic generalization of entanglement entropy,” Phys. Rev. D103, no.2, 026005 (2021) doi:10.1103/PhysRevD.103.026005 [arXiv:2005.13801 [hep-th]]
-
[45]
Pseudoentropy in dS/CFT and Timelike Entanglement Entropy,
K. Doi, J. Harper, A. Mollabashi, T. Takayanagi and Y. Taki, “Pseudoentropy in dS/CFT and Timelike Entanglement Entropy,” Phys. Rev. Lett.130, no.3, 031601 (2023) doi:10.1103/PhysRevLett.130.031601 [arXiv:2210.09457 [hep-th]]. 67
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