The DOI matches its Crossref record; 1 of the 1 references it cites were found in a registry or an index.
Why there is nothing rather than something: A theory of the cosmological constant
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Claims the paper makes
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Each is checked against this paper’s own text: does it say what the citing paper says it does?
The appearance of arbitrarily large universes causes the need for a cutoff.
“It is in particular the appearance of arbitrarily large universes that causes the need for a cutoff [5]”
From Dimensionality, topology, energy, the cosmological constant and signature change (1996) · cites this paper as [5]
In a model containing wormholes, a mismatch between probabilistic law and actual dynamics may be due to an effect induced by the existence of a wormhole scale.
“In a model containing wormholes, such a mismatch between propabilistic law and actual dynamics may also be due to an effect induced by the existence of a wormhole scale (whose magnitude is unknown, cf.Ref. [5]).”
From Dimensionality, topology, energy, the cosmological constant and signature change (1996) · cites this paper as [5]
In a model including wormholes, Λ should rapidly fall to zero once the size of the universe exceeds the wormhole scale.
“whereas in a model including wormholes it should rapidly fall to zero, once the size of the universe exceeds the wormhole scale [5]”
From Dimensionality, topology, energy, the cosmological constant and signature change (1996) · cites this paper as [5]
Citations
Cites
Loss of incoherence and determination of coupling constants in quantum gravity
Giddings, S. B., & Strominger, A. (1988) · Nuclear Physics B · doi:10.1016/0550-3213(88)90109-5 · Cited by 562
Flagged first, then by citations
Research works printed but not linked: 14
- Hawking, 1987, Phys. Lett., B195, 337, 10.1016/0370-2693(87)90028-1 · DOI
- Hawking, 1988, Phys. Rev., D37, 904
- Giddings, 1988, Nucl. Phys., B306, 890, 10.1016/0550-3213(88)90446-4 · DOI · Paper page
- Lavrelashvili, 1987, JETP Lett., 46, 167
- Hawking, 1980, Nucl. Phys., B170, 283, 10.1016/0550-3213(80)90151-0 · DOI
- Hawking, 1982, Comm. Math. Phys., 87, 395, 10.1007/BF01206031 · DOI
- Strominger, 1984, Phys. Rev. Lett., 52, 1733, 10.1103/PhysRevLett.52.1733 · DOI
- Gross, 1984, Nucl. Phys., B236, 349, 10.1016/0550-3213(84)90540-6 · DOI
- Coleman, 1988, Nucl. Phys., B307, 867, 10.1016/0550-3213(88)90110-1 · DOI · Paper page
- S.W. Hawking and R. Laflamme, Baby universes and the non-renormalizability of gravity, DAMTP preprint
- Hartle, 1983, Phys. Rev., D28, 2960
- Linde, 1988, Phys. Lett., B200, 272, 10.1016/0370-2693(88)90770-8 · DOI
- Hawking, 1984, Phys. Lett., B134, 403, 10.1016/0370-2693(84)91370-4 · DOI
- Banks, 1988, Nucl. Phys., B309, 493, 10.1016/0550-3213(88)90455-5 · DOI
Cited by
Sorted by citations
The cosmological constant problem
Weinberg, S. (1989) · Reviews of Modern Physics · doi:10.1103/revmodphys.61.1 · Cited by 7,341
QUANTUM GRAVITY AND MINIMUM LENGTH
GARAY, L. J. (1995) · International Journal of Modern Physics A · doi:10.1142/s0217751x95000085 · Cited by 1,371
Black holes as red herrings: Topological fluctuations and the loss of quantum coherence
Coleman, S. (1988) · Nuclear Physics B · doi:10.1016/0550-3213(88)90110-1 · Cited by 619
Self-citationMaldacena, J., & Maoz, L. (2004) · Journal of High Energy Physics · doi:10.1088/1126-6708/2004/02/053 · Cited by 426
Predictions from Quantum Cosmology
Vilenkin, A. (1995) · Physical Review Letters · doi:10.1103/physrevlett.74.846 · Cited by 368
Baby universe, third quantization and the cosmological constant
Giddings, S. B., & Strominger, A. (1989) · Nuclear Physics B · doi:10.1016/0550-3213(89)90353-2 · Cited by 295
Euclidean Wormholes, Baby Universes, and Their Impact on Particle Physics and Cosmology
Hebecker, A., Mikhail, T., & Soler, P. (2018) · Frontiers in Astronomy and Space Sciences · doi:10.3389/fspas.2018.00035 · Cited by 136
“Following [9, 18], one can give the action I a local form at the expense of introducing a set of auxiliary parameters αi.”
BackgroundMethodInfluentialWormholes in spacetime and the constants of nature
Preskill, J. (1989) · Nuclear Physics B · doi:10.1016/0550-3213(89)90592-0 · Cited by 87
Quantum cosmology and open universes
Coule, D. H., & Martin, J. (2000) · Physical Review D · doi:10.1103/physrevd.61.063501 · Cited by 60
Carlip, S. (2023) · Reports on Progress in Physics · doi:10.1088/1361-6633/acceb4 · Cited by 41
Lyons, A., & Hawking, S. W. (1991) · Physical Review D · doi:10.1103/physrevd.44.3802 · Cited by 25
Holographic principle and topology change in string theory
Rey, S.-J. (1999) · Classical and Quantum Gravity · doi:10.1088/0264-9381/16/7/102 · Cited by 23
Weak scale from the maximum entropy principle
Hamada, Y., Kawai, H., & Kawana, K. (2015) · Progress of Theoretical and Experimental Physics · doi:10.1093/ptep/ptv011 · Cited by 18
Dimensionality, topology, energy, the cosmological constant and signature change
Embacher, F. (1996) · Classical and Quantum Gravity · doi:10.1088/0264-9381/13/5/012 · Cited by 6
Metadata
- Authors
- Coleman, S.
- Venue
- Nuclear Physics B
- Publisher
- Elsevier BV
- Published
- 1988-12
- Volume
- 310
- Issue
- 3-4
- Pages
- 643-668
- ISSN
- 0550-3213
- Cited by
- 722
- References
- 1
- Language
- en
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Registry, retraction, Cites and statistics results are computed, not judged, with one exception: a printed reference that no index lists is read once by a model before it counts as a citation error. Claims are extracted by a model and kept only when their quote appears verbatim in the text; each cited source is then checked, with a model’s help, for whether it says what the claim relies on. Those verdicts can be wrong — read the claim’s quote and the cited source before relying on one.
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