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General Relativity and Quantum Cosmology · arXiv:1211.3463 v3 · submitted 14 Nov 2012

CSL Wave Function Collapse Model as a Mechanism for the Emergence of Cosmological Asymmetries in Inflation

Pedro Cañate, Philip Pearle, Daniel Sudarsky

The paper says

“This leads to passage from a homogeneous and isotropic stage to another, where the quantum uncertainties in the initial state of inflation transmute into the primordial inhomogeneities and anisotropies.”

from the abstract · picked out as the main claim by a classifier

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The paper

Abstract

As previously discussed in (D. Sudarsky, Int.J.Mod.Phys.D20:509-552, (2011); [arXiv:0906.0315]), the inflationary account for the emergence of the seeds of cosmic structure falls short of actually explaining the generation of primordial anisotropies and inhomogeneities. This description starts from a symmetric background, and invokes symmetric dynamics, so it cannot explain asymmetries. To generate asymmetries, we present an application of the Continuous Spontaneous Localization (CSL) model of wave function collapse (P. Pearle, Phys. Rev. A 39, 2277, (1989); G. C. Ghirardi, P. Pearle and A. Rimini, Phys. Rev. A42, 78 (1990)) in the context of inflation. This modification of quantum dynamics introduces a stochastic non-unitary component to the evolution of the inflaton field perturbations. This leads to passage from a homogeneous and isotropic stage to another, where the quantum uncertainties in the initial state of inflation transmute into the primordial inhomogeneities and anisotropies. We examine requirements for, and show how to achieve, compatibility with the precise observations of the cosmic microwave background (CMB) radiation.

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abstract compiled · 2026-09-23 · no language-model review

How the main claim is stated: asserted 1.00

What the abstract itself states, as probabilities: claims first 0.05 · states limitation 0.20 · human participants 0.01 · controlled comparison 0.09 · randomized assignment 0.01 · states quantitative result 0.06 · compares with prior results 0.83 · mentions code or data availability 0.02

The abstract, sentence by sentence

This table labels the abstract only (arXiv listing abstract v3). The number is the probability the classifier gave the label.

SentenceRoleThe authors' own workStates the main conclusionStrength
As previously discussed in (D. background 0.98 0.05 0.01 unclear 0.99
Sudarsky, Int.J.Mod.Phys.D20:509-552, (2011); [arXiv:0906.0315]), the inflationary account for the emergence of the seeds of cosmic structure falls short of actually explaining the generation of primordial anisotropies and inhomogeneities. gap 0.58 0.07 0.06 asserted 1.00
This description starts from a symmetric background, and invokes symmetric dynamics, so it cannot explain asymmetries. gap 0.77 0.08 0.06 asserted 1.00
To generate asymmetries, we present an application of the Continuous Spontaneous Localization (CSL) model of wave function collapse (P. contribution 0.74 0.70 0.17 asserted 0.96
Pearle, Phys. Rev. A 39, 2277, (1989); G. C. Ghirardi, P. Pearle and A. background 0.53 0.04 0.03 unclear 0.89
Rimini, Phys. Rev. A42, 78 (1990)) in the context of inflation. background 0.46 0.12 0.03 unclear 0.72
This modification of quantum dynamics introduces a stochastic non-unitary component to the evolution of the inflaton field perturbations. method 0.92 0.32 0.09 asserted 1.00
This leads to passage from a homogeneous and isotropic stage to another, where the quantum uncertainties in the initial state of inflation transmute into the primordial inhomogeneities and anisotropies. result 0.52 0.65 0.64 asserted 1.00
We examine requirements for, and show how to achieve, compatibility with the precise observations of the cosmic microwave background (CMB) radiation. contribution 0.96 0.89 0.10 asserted 0.92

What kind of paper the classifier reports this is: theoretical result 0.98 · evidence from proof or derivation 0.57

What was examined, and what was not

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  • arXiv listing abstract v3

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  • figures and tables
  • references and citing sentences
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  • P abstract

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  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

How the labels were made

Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 6,991 input tokens, $0.0003 reported.

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. This record as JSON

Cited by 6 Pith papers
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20 arXiv papers cite this in 43 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers whose main result relates to this one's

Found among the papers closest to this one by title and main claim. Pith's classifier compared each pair's main results and a second model family confirmed the relation; checked against two further families, shown conflicts agreed 118 times in 120 and shown same results 218 times in 239. The quoted sentence is the other paper's main claim.

States the same result 1 paper
  • In particular, in addition to accounting for the quantum-to-classical transition, we use the CSL model to generate the primordial perturbations, that is, the dynamical evolution provided by the CSL model is responsible for the transition from a homogeneous and isotropic initial state to a final one lacking such symmetries.

    Emergence of inflationary perturbations in the CSL model · 0.88

Papers citing it · 26 sentences without a confident label

Builds on it 1 paper
Uses its method or tool 1 paper
Cites it as support 2 papers
Cites it as background 10 papers

What it cites · 7 sentences without a confident label

Compares with 1 paper
  • It seems therefore that the results can be understood as follows: The localizing effect of CSL is not enough to overcome the large increase in the uncertainty of the operator considered in [ref] , but on the other hand its enough to produce the desired localization in the operator whose uncertainty would have remained constant in the absence of the localization effects of CSL.

    Cosmological Inflation and the Quantum Measurement Problem · Discussion · 0.96

Cites as background 1 paper

Challenges and discussion

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