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arXiv:quant-ph/0605072 · Journal of Physics A Mathematical and Theoretical

Lower and upper bounds on CSL parameters from latent image formation and IGM heating

Stephen L. Adler

Published Mar 7, 2007• 221 citations
arXivHTMLPDF

Abstract

We study lower and upper bounds on the parameters for stochastic state vector reduction, focusing on the mass-proportional continuous spontaneous localization (CSL) model. We show that the assumption that the state vector is reduced whan a latent image is formed, in photography or etched track detection, requires a CSL rate parameter $λ$ that is larger than conventionally assumed by a factor of roughly $2 \times 10^{9\pm 2}$, for a correlation length $r_C$ of $10^{-5}{\rm cm}$. We reanalyze existing upper bounds on the reduction rate and conclude that all are compatible with such an increase in $λ$. The best bounds that we have obtained come from a consideration of heating of the intergalactic medium (IGM), which shows that $λ$ can be at most $\sim 10^{8\pm 1}$ times as large as the standard CSL value, again for $r_C=10^{-5} {\rm cm}$. (For both the lower and upper bounds, quoted errors are not purely statistical errors, but rather are estimates reflecting modeling uncertainties.) We discuss modifications in our analysis corresponding to a larger value of $r_C$. With a substantially enlarged rate parameter, CSL effects may be within range of experimental detection (or refutation) with current technologies. ADDED NOTE: A careful calculation of radiation from atomic systems in the CSL model (Adler and Ramazanoglu, arXiv:0707.3134) has reinstated the bound obtained by Fu as the best upper bound on lambda, with significant implications for CSL model phenomenology.

DOI
10.1088/1751-8113/40/12/s03

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Lower and upper bounds on CSL parameters from latent image formation and IGM~heating

Stephen L. Adler

A careful calculation of radiation from atomic systems in the CSL model (Adler S L and Ramazanoglu F M 2007 J. Phys. A: Math. Theor. at press ( preprint 0707.3134)) has reinstated the bound obtained by Fu as the best upper bound on λ, with significant implications for CSL model phenomenology.

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An Upper Bound on Atomic-Structure Corrections to the Germanium X-Ray Bound on CSL

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The strongest experimental bound on white, mass-proportional continuous spontaneous localization (CSL) at the canonical correlation length rC = 10-7 m is the Majorana Demonstrator's 2022 search for collapse-induced X-ray emission from germanium (Phys Rev Lett 129, 080401). That bound was derived assuming the emission rate scales as 1/E with the coherent-nucleus-plus-electron amplitude S = Np2 + Ne. In 2024, Piscicchia and colleagues showed the true atomic-system emission spectrum departs from 1/E in exactly the band the Majorana search used, and called for the Majorana analysis to be reconsidered. This paper bounds that departure two ways. First, an assumption-free bound: the two k-dependent terms of the emission strength are bounded separately by the true extrema of sinc(x) (minimum -0.2172, not -1), giving 0 ≤ S(k) ≤ Np2+Ne2+2|sincmin|NpNe for every photon momentum and every atomic configuration. For germanium (Np = Ne = 32) this caps any atomic-structure correction at a factor 2.361 (not the looser 3.879 obtained from the naive triangle inequality, which is not attainable): the tightest conceivable corrected ceiling is 2.09 × 10-15 s-1, and the GRW parameter point survives it by a further factor 20.9. Second, a Hartree-Fock argument, given hypotheses stated explicitly in the paper, that within that structure the correction can only weaken the bound, not tighten it. Under the best currently published spectrum (Manti, Bortolotti, Diósi, Piscicchia and Curceanu 2026, arXiv:2608.07205), GRW survives by 79-87 times, against a published margin of 49.4 times. All arithmetic is executed in VERIFY.py and reproduced in VERIFY-OUTPUT.txt. Combined with a scoped 34-source census of the field's other constraint classes, the result is that the white-CSL window at rC = 10-7 m remains open and is bounded against future spectrum corrections by a proved ceiling, strengthened by a hypothesis-bearing argument for its sign.

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We calculate the photon emission rate from a general atomic system in the mass-proportional CSL model. For an isolated charged particle emitting kilovolt gamma rays, our results agree with those obtained by Fu. For a neutral atomic system, photon emission is strongly suppressed for photon wavelengths much larger than the atomic radius. However, for kilovolt gamma rays, Fu’s result is modified by a structure factor that is of order unity, giving no rate suppression. Our calculation is readily generalized to the case of non-white noise, noise couplings that are not mass-proportional, and general (non-Gaussian) spatial correlation functions, and corresponding results are given. We briefly discuss the implications of our calculation for upper bounds on the CSL model parameters. 1

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Photon-emission rate from atomic systems in the CSL model

Stephen L Adler, Fethi M. Ramazanoğlu

We calculate the photon emission rate from a general atomic system in the mass- proportional CSL model. For an isolated charged particle emitting kilovolt gamma rays, our results agree with those obtained by Fu. For a neutral atomic system, photon emission is strongly suppressed for photon wavelengths much larger than the atomic radius. However, for kilovolt gamma rays, Fu's result is modified by a structure factor that is of order unity, giving no rate suppression. Our calculation is readily generalized to the case of non-white noise, noise couplings that are not mass-proportional, and general (non-Gaussian) spatial correlation functions, and corresponding results are given. We briefly discuss the implications of our calculation for upper bounds on the CSL model parameters.

arXiv:0707.3134•Journal of Physics A Mathematical and Theoretical•Oct 16, 2007•72 citations
We study lower and upper bounds on the parameters for stochastic state vector reduction, focusing on the mass-proportional continuous spontaneous localization (CSL) model. We show that the assumption that the state vector is reduced whan a latent image is formed, in photography or etched track detection, requires a CSL rate parameter λλλ that is larger than conventionally assumed by a factor of roughly 2×109±22 \times 10^{9\pm 2}2×109±2, for a correlation length rCr_CrC​ of 10−5cm10^{-5}{\rm cm}10−5cm. We reanalyze existing upper bounds on the reduction rate and conclude that all are compatible with such an increase in λλλ. The best bounds that we have obtained come from a consideration of heating of the intergalactic medium (IGM), which shows that λλλ can be at most ∼108±1\sim 10^{8\pm 1}∼108±1 times as large as the standard CSL value, again for rC=10−5cmr_C=10^{-5} {\rm cm}rC​=10−5cm. (For both the lower and upper bounds, quoted errors are not purely statistical errors, but rather are estimates reflecting modeling uncertainties.) We discuss modifications in our analysis corresponding to a larger value of rCr_CrC​. With a substantially enlarged rate parameter, CSL effects may be within range of experimental detection (or refutation) with current technologies. ADDED NOTE: A careful calculation of radiation from atomic systems in the CSL model (Adler and Ramazanoglu, arXiv:0707.3134) has reinstated the bound obtained by Fu as the best upper bound on lambda, with significant implications for CSL model phenomenology.
The strongest experimental bound on white, mass-proportional continuous spontaneous localization (CSL) at the canonical correlation length rC = 10-7 m is the Majorana Demonstrator's 2022 search for collapse-induced X-ray emission from germanium (Phys Rev Lett 129, 080401). That bound was derived assuming the emission rate scales as 1/E with the coherent-nucleus-plus-electron amplitude S = Np2 + Ne. In 2024, Piscicchia and colleagues showed the true atomic-system emission spectrum departs from 1/E in exactly the band the Majorana search used, and called for the Majorana analysis to be reconsidered. This paper bounds that departure two ways. First, an assumption-free bound: the two k-dependent terms of the emission strength are bounded separately by the true extrema of sinc(x) (minimum -0.2172, not -1), giving 0 ≤ S(k) ≤ Np2+Ne2+2|sincmin|NpNe for every photon momentum and every atomic configuration. For germanium (Np = Ne = 32) this caps any atomic-structure correction at a factor 2.361 (not the looser 3.879 obtained from the naive triangle inequality, which is not attainable): the tightest conceivable corrected ceiling is 2.09 × 10-15 s-1, and the GRW parameter point survives it by a further factor 20.9. Second, a Hartree-Fock argument, given hypotheses stated explicitly in the paper, that within that structure the correction can only weaken the bound, not tighten it. Under the best currently published spectrum (Manti, Bortolotti, Diósi, Piscicchia and Curceanu 2026, arXiv:2608.07205), GRW survives by 79-87 times, against a published margin of 49.4 times. All arithmetic is executed in VERIFY.py and reproduced in VERIFY-OUTPUT.txt. Combined with a scoped 34-source census of the field's other constraint classes, the result is that the white-CSL window at rC = 10-7 m remains open and is bounded against future spectrum corrections by a proved ceiling, strengthened by a hypothesis-bearing argument for its sign.
We calculate the photon emission rate from a general atomic system in the mass-proportional CSL model. For an isolated charged particle emitting kilovolt gamma rays, our results agree with those obtained by Fu. For a neutral atomic system, photon emission is strongly suppressed for photon wavelengths much larger than the atomic radius. However, for kilovolt gamma rays, Fu’s result is modified by a structure factor that is of order unity, giving no rate suppression. Our calculation is readily generalized to the case of non-white noise, noise couplings that are not mass-proportional, and general (non-Gaussian) spatial correlation functions, and corresponding results are given. We briefly discuss the implications of our calculation for upper bounds on the CSL model parameters. 1
Abstract Among the open problems in fundamental physics, few are as conceptually significant as the “measurement problem” in Quantum Mechanics. One of the proposed solutions to this problem is the Continuous Spontaneous Localization (CSL) model, which introduces a non-linear and stochastic modification of the Schrödinger equation. This model incorporates two parameters that can be subjected to experimental constraints. One of the most notable consequences of this theory is the spontaneous heating of massive objects; this anomalous heating is dependent on the CSL parameters. In this work, we will revisit some astrophysical bounds previously found, and introduce new methods for testing the spontaneous heating in a variety of compact objects. Finally, we will compare our different bounds and discuss the benefits and shortcomings of each one.
This Zenodo record contains the main preprint and supplementary information for a shared-parameter closure analysis of Continuous Spontaneous Localization (CSL) using public upper-bound evidence and direct astrophysical inequalities. Over the reporting domain x = log10(r_C / m) in [-10, 0] and y = log10(λ / s^-1) in [-20, -5], the study reconstructs admissible upper envelopes for XENONnT, a GW/LISA composite constraint, radiation-channel searches, cold-atom and bulk-heating constraints, cantilever-related bounds, and direct astrophysical heating inequalities. The principal result is a quantified compression of the shared admissible CSL region under the current public evidence stack, together with an evidence-class limit: when each channel is represented only by one-sided admissible upper envelopes or direct inequalities, the shared-envelope admissible set is exactly the intersection of the individual admissible sets. Under this evidence class alone, positive-measure closure-failure regions cannot be established. Accordingly, the record supports a bounded claim: current public single-channel summaries overstate the shared admissible CSL volume, whereas decisive inconsistency testing requires richer, likelihood-aware evidence. Files included in this record:1. Main preprint PDF.2. Supplementary PDF containing source/provenance notes, formulas, exact reported metrics, and reproducibility notes.
We calculate the photon emission rate from a general atomic system in the mass- proportional CSL model. For an isolated charged particle emitting kilovolt gamma rays, our results agree with those obtained by Fu. For a neutral atomic system, photon emission is strongly suppressed for photon wavelengths much larger than the atomic radius. However, for kilovolt gamma rays, Fu's result is modified by a structure factor that is of order unity, giving no rate suppression. Our calculation is readily generalized to the case of non-white noise, noise couplings that are not mass-proportional, and general (non-Gaussian) spatial correlation functions, and corresponding results are given. We briefly discuss the implications of our calculation for upper bounds on the CSL model parameters.