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pith:KU65E6ZS

pith:2025:KU65E6ZST2RQS2YDXPIY5YD2I7
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Numerical simulations of density perturbation and gravitational wave production from cosmological first-order phase transition

Jintao Zou, Ligong Bian, Zhiqing Zhu, Zizhuo Zhao

Lattice simulations show bubble wall motion dominates density perturbations for strong first-order phase transitions while vacuum decay delays dominate for weak ones.

arxiv:2502.20166 v4 · 2025-02-27 · hep-ph · astro-ph.CO · hep-th

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3 Author claim open · sign in to claim
4 Citations open
5 Replications open
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Claims

C1strongest claim

For phase transition strength α > 1, forward motion of bubble walls is the primary source of density perturbation, while for α < 1, the dominant contribution comes from the delay of vacuum decay; the density perturbation power spectrum has slope k^3 at small k and k^{-1.5} at large k; GW spectrum has k^3 and k^{-2}.

C2weakest assumption

The lattice simulations accurately capture the non-linear dynamics of bubble wall motion and vacuum decay without significant numerical artifacts or missing physical effects like friction or plasma interactions.

C3one line summary

3D simulations of cosmological first-order phase transitions find density perturbation spectra with k^3 and k^{-1.5} slopes and GW spectra with k^3 and k^{-2}, confirming slow transitions can produce PBHs.

References

111 extracted · 111 resolved · 43 Pith anchors

[1] As more and more bubbles form and collide, the initially uniform spatial structure is disrupted, resulting in an asymmetric energy distribution
[2] S. W. Hawking, I. G. Moss, and J. M. Stewart, Bubble Collisions in the Very Early Universe, Phys. Rev. D26, 2681 (1982) 1982
[3] M. Crawford and D. N. Schramm, Spontaneous Generation of Density Perturbations in the Early Universe, Nature298, 538 (1982) 1982
[4] H. Kodama, M. Sasaki, and K. Sato, Abundance of Primordial Holes Produced by Cosmological First Order Phase Transition, Prog. Theor. Phys.68, 1979 (1982) 1979
[5] Determining the outcome of cosmic bubble collisions in full General Relativity 2012 · arXiv:1112.4487

Cited by

2 papers in Pith

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First computed 2026-06-12T01:09:07.553637Z
Builder pith-number-builder-2026-05-17-v1
Signature Pith Ed25519 (pith-v1-2026-05) · public key
Schema pith-number/v1.0

Canonical hash

553dd27b329ea3096b03bbd18ee07a47eaa9651c15f737f33f0f5ea6b1a8f42c

Aliases

arxiv: 2502.20166 · arxiv_version: 2502.20166v4 · doi: 10.48550/arxiv.2502.20166 · pith_short_12: KU65E6ZST2RQ · pith_short_16: KU65E6ZST2RQS2YD · pith_short_8: KU65E6ZS
Agent API
Verify this Pith Number yourself
curl -sH 'Accept: application/ld+json' https://pith.science/pith/KU65E6ZST2RQS2YDXPIY5YD2I7 \
  | jq -c '.canonical_record' \
  | python3 -c "import sys,json,hashlib; b=json.dumps(json.loads(sys.stdin.read()), sort_keys=True, separators=(',',':'), ensure_ascii=False).encode(); print(hashlib.sha256(b).hexdigest())"
# expect: 553dd27b329ea3096b03bbd18ee07a47eaa9651c15f737f33f0f5ea6b1a8f42c
Canonical record JSON
{
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      "astro-ph.CO",
      "hep-th"
    ],
    "license": "http://arxiv.org/licenses/nonexclusive-distrib/1.0/",
    "primary_cat": "hep-ph",
    "submitted_at": "2025-02-27T15:04:55Z",
    "title_canon_sha256": "6fa7a1ceb25138038734feb40e71d40d4d0bea0c684d20a6eedf31e474d7bdcf"
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  "source": {
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}