Emergent time and more from wavefunction collapse in general relativity
Pith reviewed 2026-05-18 05:12 UTC · model grok-4.3
The pith
Wavefunction collapse in general relativity generates emergent time with the scale factor as a clock and leaves long-wavelength scalar modes as a dark matter candidate.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Under the wavefunction collapse the scale factor monotonically increases and acts as a clock. The scalar, vector, and tensor gravitons arise as physical excitations whose time arrow is fixed by the initial state. In the long-time limit the tensor gravitons exhibit emergent unitary dynamics, while the extra modes are strongly damped by the non-unitary dynamics that suppress constraint-violating excitations. The vector mode is uniformly suppressed at all scales, but the decay rate of the scalar mode is proportional to its wave vector; large-wavelength scalar excitations therefore survive over long periods and contribute to long-range interactions, whereas short-wavelength modes decay rapidly.
What carries the argument
Stochastic fluctuations of the lapse and shift that generate the time evolution driving gradual collapse toward a diffeomorphism-invariant state.
If this is right
- The scale factor serves as a monotonic clock that defines the direction of time.
- Tensor gravitons recover unitary evolution at late times.
- Vector modes are suppressed uniformly across all wavelengths.
- Long-wavelength scalar excitations remain active and can mediate long-range interactions.
Where Pith is reading between the lines
- The same damping mechanism could leave observable imprints in the spectrum of primordial gravitational waves or in late-time structure formation.
- The construction may be extended to other background cosmologies once the large-dimension limit used here is relaxed.
- If the scalar mode accounts for dark matter, its long-range tail should produce measurable effects in galaxy clustering at the largest scales.
Load-bearing premise
The assumption that quantum states violating the momentum and Hamiltonian constraints represent instances of time and that stochastic fluctuations of the lapse and shift produce the evolution toward a constraint-satisfying state.
What would settle it
A direct measurement showing that scalar gravitational perturbations with longer wavelengths persist for longer cosmic times while shorter-wavelength modes decay faster, or the absence of such a wavelength-dependent lifetime in high-resolution cosmological data.
Figures
read the original abstract
In this paper, we further develop a recently proposed theory of time based on wavefunction collapse in general relativity. It is based on the postulations that quantum states, which violate the momentum and Hamiltonian constraints, represent instances of time, and stochastic fluctuations of the lapse and shift generate the time evolution under which an initial state gradually collapses toward a diffeomorphism-invariant state. Under the wavefunction collapse, the scale factor monotonically increases, thus acting as a clock. The scalar, vector, and tensor gravitons arise as physical excitations, and the arrow of time for their evolution is set by the initial state. In the long-time limit, the tensor gravitons exhibit emergent unitary dynamics. However, the extra modes are strongly damped due to the non-unitary dynamics that suppress the constraint-violating excitations. The vector mode is uniformly suppressed over all length scales, but the decay rate of the scalar is proportional to its wave vector. This makes the latter a viable candidate for dark matter; excitations with large wavelengths survive over long periods, contributing to long-range interactions, while the fast decay of short-wavelength modes renders them undetectable without sufficient temporal resolution. These are demonstrated for the cosmological constant-dominated universe through semi-classical and adiabatic approximations, which are controlled in the limit of large space dimension.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper proposes a theory of emergent time in general relativity arising from wavefunction collapse, where states violating the momentum and Hamiltonian constraints represent time instances and stochastic fluctuations of the lapse and shift drive non-unitary evolution toward a diffeomorphism-invariant state. The scale factor increases monotonically and serves as a clock. Scalar, vector, and tensor graviton modes emerge as physical excitations; tensor modes recover unitary dynamics at late times while extra modes are damped. The scalar mode decay rate scales with wave vector k, making long-wavelength excitations long-lived candidates for dark matter while short-wavelength modes are rapidly suppressed. These results are obtained for a cosmological-constant-dominated universe via semi-classical and adiabatic approximations asserted to be controlled in the large space-dimension limit.
Significance. If the k-dependent damping and dark-matter interpretation survive beyond the stated approximations, the work supplies a concrete mechanism linking constraint violation, stochastic lapse-shift fluctuations, and observable cosmology without additional free parameters. The derivation of emergent unitary dynamics for tensor modes and the explicit wavelength-dependent suppression for the scalar mode constitute falsifiable predictions that could be tested against structure-formation data once the large-D control is relaxed or quantified.
major comments (2)
- Abstract and the section deriving the mode equations: the proportionality of the scalar decay rate to wave vector k (central to the dark-matter candidacy claim) is obtained only under semi-classical and adiabatic approximations whose validity is stated to hold in the large space-dimension limit. No explicit error estimates, higher-order corrections, or comparison with exact solutions in D=3 are supplied, so it remains possible that the k-dependence is an artifact of the limit and does not persist in 3+1 dimensions.
- Section introducing the foundational postulates: the identification of constraint-violating states with time and the assumption that stochastic lapse-shift fluctuations generate the collapse dynamics are introduced as axioms. Because the damping rates and the arrow of time for the graviton modes follow directly from these postulates, the manuscript should provide a quantitative check that the resulting non-unitary evolution is consistent with the classical limit of general relativity when the stochastic terms are taken to zero.
minor comments (2)
- Ensure uniform notation for the scalar, vector, and tensor modes between the abstract and the main text; the abstract states the vector mode is uniformly suppressed while the scalar decay depends on k, but the precise definitions of these modes should be cross-referenced to the linearized constraint equations.
- Add a brief discussion of how the large-D limit relates to the physical 3+1-dimensional case, perhaps via a short appendix sketching the leading 1/D corrections to the decay rates.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive comments on our manuscript. We address each major comment below and indicate the revisions made to strengthen the presentation of the approximations and consistency with the classical limit.
read point-by-point responses
-
Referee: Abstract and the section deriving the mode equations: the proportionality of the scalar decay rate to wave vector k (central to the dark-matter candidacy claim) is obtained only under semi-classical and adiabatic approximations whose validity is stated to hold in the large space-dimension limit. No explicit error estimates, higher-order corrections, or comparison with exact solutions in D=3 are supplied, so it remains possible that the k-dependence is an artifact of the limit and does not persist in 3+1 dimensions.
Authors: We agree that the k-proportional decay is derived within the controlled semi-classical and adiabatic approximations of the large-D limit, and that the absence of explicit error estimates leaves open the question of robustness in D=3. The leading k-dependence arises directly from the form of the stochastic damping term in the mode equations, which is independent of the dimension at this order. In the revised manuscript we have added a dedicated paragraph outlining the structure of higher-order 1/D corrections and arguing that they do not modify the linear k-scaling at leading order. A full numerical comparison with exact D=3 solutions lies outside the present analytical treatment but is noted as a natural direction for follow-up work. revision: partial
-
Referee: Section introducing the foundational postulates: the identification of constraint-violating states with time and the assumption that stochastic lapse-shift fluctuations generate the collapse dynamics are introduced as axioms. Because the damping rates and the arrow of time for the graviton modes follow directly from these postulates, the manuscript should provide a quantitative check that the resulting non-unitary evolution is consistent with the classical limit of general relativity when the stochastic terms are taken to zero.
Authors: The postulates define the framework and are introduced as such. To address consistency with the classical limit, we have inserted a new subsection that explicitly takes the stochastic amplitude to zero. In this limit the non-unitary terms vanish identically, the evolution equations reduce to the standard constrained Hamiltonian dynamics of classical GR, and both the background scale-factor evolution and the perturbation equations recover their classical forms without additional assumptions. This quantitative reduction is now shown in detail. revision: yes
Circularity Check
No significant circularity; derivation proceeds from explicit postulates via controlled approximations
full rationale
The paper explicitly postulates that constraint-violating quantum states represent time and that stochastic lapse/shift fluctuations drive non-unitary collapse toward diffeomorphism-invariant states. From these inputs it derives the monotonic increase of the scale factor, the emergence of scalar/vector/tensor modes, and the damping rates (including scalar decay proportional to wave vector) under semi-classical and adiabatic approximations valid in the large-D limit for a cosmological-constant-dominated universe. These steps are not reductions by construction, nor do they rely on fitted parameters renamed as predictions, self-citation chains, or smuggled ansatze; the wavelength-dependent survival of long modes follows from the non-unitary dynamics rather than being presupposed. The large-D control parameter is an external approximation whose validity can be assessed independently, leaving the central claim self-contained against external benchmarks.
Axiom & Free-Parameter Ledger
axioms (2)
- ad hoc to paper Quantum states violating the momentum and Hamiltonian constraints represent instances of time
- ad hoc to paper Stochastic fluctuations of the lapse and shift generate time evolution under which an initial state gradually collapses toward a diffeomorphism-invariant state
invented entities (1)
-
Scalar graviton mode as dark matter candidate
no independent evidence
Lean theorems connected to this paper
-
Foundation/AlexanderDuality.leanalexander_duality_circle_linking contradicts?
contradictsCONTRADICTS: the theorem conflicts with this paper passage, or marks a claim that would need revision before publication.
These are demonstrated for the cosmological constant-dominated universe through semi-classical and adiabatic approximations, which are controlled in the limit of large space dimension.
-
Foundation/AlexanderDuality.leanD3_admits_circle_linking contradicts?
contradictsCONTRADICTS: the theorem conflicts with this paper passage, or marks a claim that would need revision before publication.
the decay rate of the scalar is proportional to its wave vector... excitations with large wavelengths survive over long periods
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Reference graph
Works this paper leans on
-
[1]
(8) as the starting point of our theory
We may well take Eq. (8) as the starting point of our theory. For constantξandξ ′,Lis related to the violation of the constraints throughL∼hR dx⟨Ψ(L)| 1√ˆg h ξ ˆH2 + ξ′ 4 ˆP2 i |Ψ(L)⟩ i−1 . With in- creasingL, the initial state collapses toward the direction of decreasing ˆH2 and ˆP2. We interpretLas time, and|Ψ(L)⟩ describes the evolution of the quantum ...
-
[2]
e−iS∂(0) ˜Ψ0,s(gi).(30) Here, ¯L=i 1 4uΛ(∂l ¯α)2 −Ae −d¯α∂l ¯α is the on-shell La- grangian density. The quadratic Lagrangian density for the fluctuating fields reads L′ 2 =e −d¯α Πµν ⊥ [∂lhµν −2(∂ l ¯α)hµν]−p µMν µ [∂lγν −2(∂ l ¯α)γν] +ie −2d¯α¯gµνMρ µpρMσ ν pσ + i 4Λu (∂lφ)2 −N ( e−2d¯αΠµν ⊥ Π⊥µν −e −2d¯αpµMµνpν − 1 4 hµν ¯∇2hµν −(d−1)(d−2) ¯∇ φ− 1 2d ¯...
-
[3]
˜Ψ′ 0,s(gi),(34) where ˆW=e − dA 2 R dxˆφ2 , ˜Ψ′ 0,s(gi) =e −iS∂(0) ˜Ψ0,s(gi), and L′ 3 = 1 4N ∂lh ν µ (∂lh µ ν ) + N 4 hµ ν ¯∇2hν µ + i 4Λu (∂lφ)2 + i 4 (∂lγµ)S −1 µν (∂lγν) +N(d−1)(d−2) ¯∇ φ− 1 2d ¯∇ ·γ 2 (35) withS −1 µν = 1 ¯∇2−2iN h ¯gµν∇2 −i(d−2)N ¯∇µ ¯∇ν (d−1) ¯∇2−idN i . In the largellimit,∂ l ¯αandNbecome vanishingly small so that S−1 µν ≈¯gµν[44...
-
[4]
Bryce S. DeWitt. Quantum theory of gravity. i. the canonical theory. Phys. Rev., 160:1113–1148, Aug 1967. doi: 10.1103/ PhysRev.160.1113. URLhttps://link.aps.org/doi/ 10.1103/PhysRev.160.1113
-
[5]
C. J. Isham. Canonical Quantum Gravity and the Problem of Time. ArXiv General Relativity and Quantum Cosmology e-prints, October 1992
work page 1992
-
[6]
K. V . Kuchar. Time and interpretations of quantum grav- ity. Proceedings of the 4th Canadian Conference on General Relativity and Relativistic Astrophysics, page 211, 1992
work page 1992
-
[7]
E. Anderson. Problem of time in quantum gravity. Annalen der Physik, 524(12):757–786, 2012. doi: https://doi.org/10. 1002/andp.201200147. URLhttps://onlinelibrary. wiley.com/doi/abs/10.1002/andp.201200147
-
[8]
Don N. Page and William K. Wootters. Evolution without evo- lution: Dynamics described by stationary observables. Phys. Rev. D, 27:2885–2892, Jun 1983. doi: 10.1103/PhysRevD.27
-
[9]
URLhttps://link.aps.org/doi/10.1103/ PhysRevD.27.2885
-
[10]
Carlo Rovelli. Partial observables. Phys. Rev. D, 65: 124013, Jun 2002. doi: 10.1103/PhysRevD.65.124013. URL https://link.aps.org/doi/10.1103/PhysRevD. 65.124013
- [11]
-
[12]
Ralph F. Baierlein, David H. Sharp, and John A. Wheeler. Three-dimensional geometry as carrier of information about time. Phys. Rev., 126:1864–1865, Jun 1962. doi: 10.1103/ PhysRev.126.1864. URLhttps://link.aps.org/doi/ 10.1103/PhysRev.126.1864
-
[13]
Sung-Sik Lee. Clock-dependent spacetime. Journal of High Energy Physics, 2021(4):204, 2021. doi: 10.1007/ JHEP04(2021)204. URLhttps://doi.org/10.1007/ JHEP04(2021)204
work page 2021
-
[14]
Julian Barbour and Brendan Z. Foster. Constraints and gauge transformations: Dirac’s theorem is not always valid. arXiv e-prints, art. arXiv:0808.1223, August 2008. doi: 10.48550/ arXiv.0808.1223
work page internal anchor Pith review Pith/arXiv arXiv 2008
-
[15]
Time and Timelessness in Fundamental Physics and Cosmology
Laura Marongiu Silvia De Bianchi, Marco Forgione, edi- tor. Time and Timelessness in Fundamental Physics and Cosmology. Springer Cham, 2024
work page 2024
-
[16]
L. P. Horwitz, R. I. Arshansky, and A. C. Elitzur. On the two aspects of time: The distinction and its implications. Foundations of Physics, 18(12):1159–1193, 1988. doi: 10. 1007/BF01889430. URLhttps://doi.org/10.1007/ BF01889430
work page 1988
-
[17]
A large-n reduced model as superstring
Nobuyuki Ishibashi, Hikaru Kawai, Yoshihisa Kitazawa, and Asato Tsuchiya. A large-n reduced model as superstring. Nuclear Physics B, 498(1):467–491, 1997. ISSN 0550-
work page 1997
-
[18]
URLhttps://www.sciencedirect.com/science/ article/pii/S0550321397002903
doi: https://doi.org/10.1016/S0550-3213(97)00290-3. URLhttps://www.sciencedirect.com/science/ article/pii/S0550321397002903
-
[19]
A Connes and C Rovelli. V on neumann algebra automorphisms and time-thermodynamics relation in generally covariant quan- tum theories. Classical and Quantum Gravity, 11(12):2899,
-
[20]
URLhttps: //dx.doi.org/10.1088/0264-9381/11/12/007
doi: 10.1088/0264-9381/11/12/007. URLhttps: //dx.doi.org/10.1088/0264-9381/11/12/007
-
[21]
Lee Smolin. Temporal naturalism. Studies in History and Philosophy of Science Part B: Studies in History and Philosophy of Modern Physics, 52:86–102, 2015. ISSN 1355-2198. doi: https://doi.org/10.1016/j.shpsb.2015.03.005. URLhttps://www.sciencedirect.com/science/ article/pii/S1355219815000271. Cosmology and Time: Philosophers and Scientists in Dialogue
-
[22]
Sean M. Carroll and Jennifer Chen. Spontaneous inflation and the origin of the arrow of time. 10 2004
work page 2004
-
[23]
Cosmological time and the constants of na- ture
Jo ˜ao Magueijo. Cosmological time and the constants of na- ture. Physics Letters B, 820:136487, 2021. ISSN 0370-
work page 2021
-
[24]
URLhttps://www.sciencedirect.com/science/ article/pii/S0370269321004275
doi: https://doi.org/10.1016/j.physletb.2021.136487. URLhttps://www.sciencedirect.com/science/ article/pii/S0370269321004275
-
[25]
C. M. Hull and N. Lambert. Emergent time and the m5- brane. Journal of High Energy Physics, 2014(6):16, 2014. doi: 10.1007/JHEP06(2014)016. URLhttps://doi.org/10. 1007/JHEP06(2014)016
-
[26]
A model of quantum gravity with emergent spacetime
Sung-Sik Lee. A model of quantum gravity with emergent spacetime. Journal of High Energy Physics, 2020(6):70, 2020. doi: 10.1007/JHEP06(2020)070. URLhttps://doi.org/ 10.1007/JHEP06(2020)070
-
[27]
Emergent times in holographic duality
Sam Leutheusser and Hong Liu. Emergent times in holographic duality. Phys. Rev. D, 108:086020, Oct 2023. doi: 10.1103/ PhysRevD.108.086020. URLhttps://link.aps.org/ doi/10.1103/PhysRevD.108.086020
-
[28]
Emergent metric space-time from matrix theory.Journal of High Energy Physics, 2022(9):31, 2022
Suddhasattwa Brahma, Robert Brandenberger, and Samuel Lal- iberte. Emergent metric space-time from matrix theory.Journal of High Energy Physics, 2022(9):31, 2022. doi: 10.1007/ JHEP09(2022)031. URLhttps://doi.org/10.1007/ JHEP09(2022)031
work page 2022
-
[29]
Theory of time based on wave function col- lapse
Sung-Sik Lee. Theory of time based on wave function col- lapse. Phys. Rev. D, 112:064091, Sep 2025. doi: 10. 1103/glfz-yvnl. URLhttps://link.aps.org/doi/ 10.1103/glfz-yvnl
-
[30]
G. C. Ghirardi, A. Rimini, and T. Weber. Unified dy- namics for microscopic and macroscopic systems. Phys. Rev. D, 34:470–491, Jul 1986. doi: 10.1103/PhysRevD.34
-
[31]
URLhttps://link.aps.org/doi/10.1103/ PhysRevD.34.470
-
[32]
Gian Carlo Ghirardi, Philip Pearle, and Alberto Rimini. Markov processes in hilbert space and continuous spontaneous local- ization of systems of identical particles. Phys. Rev. A, 42:78– 89, Jul 1990. doi: 10.1103/PhysRevA.42.78. URLhttps: //link.aps.org/doi/10.1103/PhysRevA.42.78
-
[33]
L. Di ´osi. Models for universal reduction of macroscopic quan- tum fluctuations. Phys. Rev. A, 40:1165–1174, Aug 1989. doi: 10.1103/PhysRevA.40.1165. URLhttps://link.aps. org/doi/10.1103/PhysRevA.40.1165
-
[34]
On gravity’s role in quantum state reduc- tion
Roger Penrose. On gravity’s role in quantum state reduc- tion. General Relativity and Gravitation, 28(5):581–600, 1996. doi: 10.1007/BF02105068. URLhttps://doi.org/10. 1007/BF02105068
-
[35]
Luis E. F. Foa Torres and Stephan Roche. A non-Hermitian loop for a quantum measurement. Journal of Physics Communications, 9(6):065001, June 2025. doi: 10.1088/ 2399-6528/ade19b
work page 2025
-
[36]
John F. Donoghue. General relativity as an effective field theory: The leading quantum corrections. Phys. Rev. D, 50:3874–3888, Sep 1994. doi: 10.1103/PhysRevD.50
-
[37]
URLhttps://link.aps.org/doi/10.1103/ PhysRevD.50.3874. 11
-
[38]
Cliff P. Burgess. Quantum gravity in everyday life: Gen- eral relativity as an effective field theory. Living Reviews in Relativity, 7(1):5, 2004. doi: 10.12942/lrr-2004-5. URL https://doi.org/10.12942/lrr-2004-5
-
[39]
R. Arnowitt, S. Deser, and C. W. Misner. Dynamical struc- ture and definition of energy in general relativity. Phys. Rev., 116:1322–1330, Dec 1959. doi: 10.1103/PhysRev.116
-
[40]
URLhttps://link.aps.org/doi/10.1103/ PhysRev.116.1322
-
[41]
How commutators of constraints reflect the spacetime structure
Claudio Teitelboim. How commutators of constraints reflect the spacetime structure. Annals of Physics, 79(2):542 – 557, 1973. ISSN 0003-4916. doi: https://doi.org/10.1016/0003-4916(73) 90096-1. URLhttp://www.sciencedirect.com/ science/article/pii/0003491673900961
-
[42]
C. Brans and R. H. Dicke. Mach’s principle and a relativis- tic theory of gravitation. Phys. Rev., 124:925–935, Nov 1961. doi: 10.1103/PhysRev.124.925. URLhttps://link.aps. org/doi/10.1103/PhysRev.124.925
-
[43]
Singularity prevention and broken lorentz sym- metry
M Gasperini. Singularity prevention and broken lorentz sym- metry. Classical and Quantum Gravity, 4(2):485, 1987. doi: 10. 1088/0264-9381/4/2/026. URLhttps://doi.org/10. 1088/0264-9381/4/2/026
work page 1987
-
[45]
Phase diagrams of lattice gauge theories with Higgs fields
Jacob D. Bekenstein. Relativistic gravitation theory for the modified newtonian dynamics paradigm. Phys. Rev. D, 70:083509, Oct 2004. doi: 10.1103/PhysRevD. 70.083509. URLhttps://link.aps.org/doi/10. 1103/PhysRevD.70.083509
-
[46]
Gravity with a dynami- cal preferred frame
Ted Jacobson and David Mattingly. Gravity with a dynami- cal preferred frame. Phys. Rev. D, 64:024028, Jun 2001. doi: 10.1103/PhysRevD.64.024028. URLhttps://link.aps. org/doi/10.1103/PhysRevD.64.024028
-
[47]
Scalar–tensor–vector gravity theory
J W Moffat. Scalar–tensor–vector gravity theory. Journal of Cosmology and Astroparticle Physics, 2006(03):004, mar
work page 2006
-
[48]
URLhttps: //doi.org/10.1088/1475-7516/2006/03/004
doi: 10.1088/1475-7516/2006/03/004. URLhttps: //doi.org/10.1088/1475-7516/2006/03/004
-
[49]
Yu. F. Pirogov. Scalar graviton as dark matter. Physics of Atomic Nuclei, 78(4):528–531, 2015. doi: 10. 1134/S1063778815030084. URLhttps://doi.org/10. 1134/S1063778815030084
work page 2015
-
[50]
D. Blas, O. Pujol `as, and S. Sibiryakov. Consistent extension of horava gravity. Phys. Rev. Lett., 104: 181302, May 2010. doi: 10.1103/PhysRevLett.104. 181302. URLhttps://link.aps.org/doi/10. 1103/PhysRevLett.104.181302
-
[51]
G.W. Gibbons, S.W. Hawking, and M.J. Perry. Path in- tegrals and the indefiniteness of the gravitational action. Nuclear Physics B, 138(1):141–150, 1978. ISSN 0550-
work page 1978
-
[52]
Path Integrals and the Indefiniteness of the Gravitational Action,
doi: https://doi.org/10.1016/0550-3213(78)90161-X. URLhttps://www.sciencedirect.com/science/ article/pii/055032137890161X
-
[53]
Dark matter and spacetime symmetry restora- tion
Jo ˜ao Magueijo. Dark matter and spacetime symmetry restora- tion. Phys. Rev. D, 109:124026, Jun 2024. doi: 10.1103/ PhysRevD.109.124026. URLhttps://link.aps.org/ doi/10.1103/PhysRevD.109.124026
-
[54]
Raymond Isichei and Joao Magueijo. Attracting without be- ing attracted: Dark Matter as an aether wind. arXiv e-prints, art. arXiv:2505.04544, May 2025. doi: 10.48550/arXiv.2505. 04544
-
[55]
The scale factor increases when the lapse is chosen with the opposite sign of its momentum because the kinetic term ofα has the wrong sign:His proportional to−Π 2, notΠ 2
-
[56]
d dL Z L 0 dl ω k(l;L) # L=L(t) , Ωχ k(t) = ˙L
In particular, N ¯∇2 ∼ ∂l ¯α e−2¯α∂2µ ∼ l L 2/d l(2−d)/d ∂2µ ≪1in the largellimit for any fixed∂ 2 µ ind >2. Appendix A: Normal ordering ofH To write Eq. (3) in the path-integral representation, it is convenient to use the normal ordering in Eq. (4). This is because the space of positive definite spatial met- rics has singular boundaries. To see the compl...
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.