Cited by 722

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

Coleman, Sidney·1988·Nuclear Physics B

Overview

Integrity signals

Registry

Crossref · 10.1016/0550-3213(88)90097-1

Cites

1 of 1 references verified0 citation errors · 0 not checkable

Statistics

Recomputing p-values needs the paper’s full text.

Verification

Claims the paper makes

We couldn’t retrieve this paper’s full text, so its claims and self-check weren’t run. The registry and citation checks still apply.

Claims other papers make about this one

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]”
  • 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]).”
  • 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]”

Citations

Cites

Flagged first, then by citations

Research works printed but not linked: 14

  1. Hawking, 1987, Phys. Lett., B195, 337, 10.1016/0370-2693(87)90028-1 · DOI
  2. Hawking, 1988, Phys. Rev., D37, 904
  3. Giddings, 1988, Nucl. Phys., B306, 890, 10.1016/0550-3213(88)90446-4 · DOI · Paper page
  4. Lavrelashvili, 1987, JETP Lett., 46, 167
  5. Hawking, 1980, Nucl. Phys., B170, 283, 10.1016/0550-3213(80)90151-0 · DOI
  6. Hawking, 1982, Comm. Math. Phys., 87, 395, 10.1007/BF01206031 · DOI
  7. Strominger, 1984, Phys. Rev. Lett., 52, 1733, 10.1103/PhysRevLett.52.1733 · DOI
  8. Gross, 1984, Nucl. Phys., B236, 349, 10.1016/0550-3213(84)90540-6 · DOI
  9. Coleman, 1988, Nucl. Phys., B307, 867, 10.1016/0550-3213(88)90110-1 · DOI · Paper page
  10. S.W. Hawking and R. Laflamme, Baby universes and the non-renormalizability of gravity, DAMTP preprint
  11. Hartle, 1983, Phys. Rev., D28, 2960
  12. Linde, 1988, Phys. Lett., B200, 272, 10.1016/0370-2693(88)90770-8 · DOI
  13. Hawking, 1984, Phys. Lett., B134, 403, 10.1016/0370-2693(84)91370-4 · DOI
  14. Banks, 1988, Nucl. Phys., B309, 493, 10.1016/0550-3213(88)90455-5 · DOI

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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

About these checks

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.

Statistics and arithmetic are recomputed, not judged.

Confidence bands are shown only for fields calibrated on our annotated test set. None is calibrated yet, so no band is shown.

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