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Microscopic Cosmological Origin of CSL Collapse Noise via Higgs-Portal Scalar Misalignment

Ahmed Beniaiche

Published Dec 9, 2025• 0 citations
Publisher

Abstract

The Continuous Spontaneous Localization (CSL) model offers a dynamical solution to the quantum measurement problem by introducing a classical stochastic field that induces wavefunction collapse, yet the physical origin of this field remainselusive. A promising recent proposal identifies a light scalar field coupled via the Higgs portal as the source of this collapse-inducing noise, with its efficacy governed by a non-equilibrium enhancement factor Xϕ. In this work, we perform the first comprehensive, first-principles derivation of Xϕ from cosmological dynamics, establishing a concrete microphysical origin forCSL noise. We analyze two well-motivated cosmological production mechanisms: - vacuum misalignment—where the scalar acquires a coherent displacement during inflation—and freeze-in via ultra-weak Higgs interactions. For each mechanism, we derive explicit, predictive expressions for Xϕ in terms of fundamental parameters(λHS , ϕi, Hinf , mϕ), connecting inflationary initial conditions to laboratory-scale col lapse rates. Our analysis reveals a fundamental dichotomy: while the misalignment mechanism naturally yields Xϕ ∼ O(10−10e9) from realistic initial conditions (ϕi ∼ 10e13−10e15 GeV, Hinf ∼ 10e10 GeV), enabling observable CSL effects with λ ∼ 2×10e−12 s−1, the freeze-in mechanism produces Xϕ ≪ 1 for couplings allowed by astrophysics, rendering it phenomenologically irrelevant for collapse dynamics.We confront these predictions with the complete suite of current observational constraints, including stellar cooling bounds, fifth-force searches, Planck data on isocurvature perturbations and dark matter abundance, LHC Higgs measurements,and non-interferometric tests of CSL. Notably, we demonstrate that: 1. The viable parameter space for misalignment-produced CSL noise is robust, occupying approximately two orders of magnitude in ϕi and Hinf ;2. All existing constraints from particle physics, astrophysics, and cosmology are simultaneously satisfied without fine-tuning;3. Key predictions include a universal collapse rate λ ∼ 2 × 10e−12 s−1 for rC ∼ 200 nm, mass-dependent decoherence in matter-wave interferometry, and potential high-frequency spectral features from the oscillating condensate. This work provides three key advances: (i) it resolves the long-standing “no-go” obstruction for equilibrium scalar fields to generate Markovian collapse noise by identifying cosmological misalignment as a natural source of persistent non-equilibrium; (ii) it establishes a testable connection between early-universe physics (inflation, scalar condensates) and laboratory-scale quantum phenomena; and (iii) it transforms Higgs-portal collapse models from phenomenological frameworks into predictive cosmological scenarios with falsifiable predictions for next-generation experiments. By deriving Xϕ from cosmology rather than parameterizing it, we complete the microphysical foundation of scalar-field collapse models and open a new pathway toward unifying quantum foundations with cosmological history.

DOI
10.5281/zenodo.17873076

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Higgs-Portal Scalar-Field Collapse From Non-Markovian Dynamics to Viable CSL Limit

Ahmed Beniaiche

We propose and analyze a model of objective wave-function collapse induced by alightreal scalar field ϕ coupled to the mass density of matter viaa Higgs-portal interaction. Themodel aims to provide a microscopic origin for continuous spontaneous localization (CSL)–type dynamics while remaining compatible with particle physics, astrophysical, and non-interferometric collapse constraints. Starting from a concrete Higgs-portal Lagrangian, we derive the non-Markovian master equation for the reduced density matrix of matter obtained by integrating out ϕ in a general Gaussian state. We show that for a massive scalar field in thermal equilibrium (including the vacuum) the Markovian limit required to recover a CSL-like Lindblad term vanishes identically : the time-integrated field correlator defining the would-be Markovian kernel is zero for m_ϕ= ̸=0. This provides a simple“no-go” result: a standard equilibrium quantum field cannot generate a white-noise collapse term of CSL type. We then introduce a phenomenological non-equilibrium scalar noise parameterized by a dimensionless amplification factor X_ϕ and derive the mapping between the scalar–nucleon coupling gs and the CSL collapse rate λ as a function of the correlation length r_C. Using theHiggs-portal structure, we relate gs to the mixing angle θ and portal coupling λHS and confront the model with (i) astrophysical bounds on fifth-forces and stellar cooling, (ii) collider limits on invisible Higgs decays and Higgs–scalar mixing, and (iii) non-interferometric CSL constraints from X-ray emission, bulk heating, cold atoms, LISA Pathfinder and planetary heating. We show that the reexists aviable region of parameter space with mϕ∼eV, r_C∼200nm, gs≲10e-13, λ_HS∼10e−11 and λ∼10e12s−1 which satisfies simultaneously all current constraints while providing a potentially observable collapse rate for mesoscopic systems. Our analysis clarifies both the promise and limitations of Higgs-portal scalar field collapse models : they offer a concrete, testable UV completion for CSL, but require the scalar sector to be in a non-equilibrium, effectively classical state whose microscopic origin remains to be explained. NB: "This is personal/unfunded research."

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According to cosmological inflation, the inhomogeneities in our Universe are of quantum-mechanical origin. This scenario is phenomenologically very appealing as it solves the puzzles of the standard hot big bang model and naturally explains why the spectrum of cosmological perturbations is almost scale invariant. It is also an ideal playground to discuss deep questions among which is the quantum measurement problem in a cosmological context. Although the large squeezing of the quantum state of the perturbations and the phenomenon of decoherence explain many aspects of the quantum-to-classical transition, it remains to understand how a specific outcome can be produced in the early Universe, in the absence of any observer. The continuous spontaneous localization (CSL) approach to quantum mechanics attempts to solve the quantum measurement question in a general context. In this framework, the wave function collapse is caused by adding new nonlinear and stochastic terms to the Schr\"odinger equation. In this paper, we apply this theory to inflation, which amounts to solving the CSL parametric oscillator case. We choose the wave function collapse to occur on an eigenstate of the Mukhanov-Sasaki variable and discuss the corresponding modified Schr\"odinger equation. Then, we compute the power spectrum of the perturbations and show that it acquires a universal shape with two branches, one which remains scale invariant and one with ${n}_{\mathrm{S}}=4$, a spectral index in obvious contradiction with the cosmic microwave background anisotropy observations. The requirement that the non-scale-invariant part be outside the observational window puts stringent constraints on the parameter controlling the deviations from ordinary quantum mechanics. Due to the absence of a CSL amplification mechanism in field theory, this also has the consequence that the collapse mechanism of the inflationary fluctuations is not efficient. Then, we determine the collapse time. On small scales the collapse is almost instantaneous, and we recover exactly the behavior of the CSL harmonic oscillator (a case for which we present new results), whereas, on large scales, we find that the collapse is delayed and can take several e-folds to happen. We conclude that recovering the observational successes of inflation and, at the same time, reaching a satisfactory resolution of the inflationary ``macro-objectification'' issue seems problematic in the framework considered here. This work also provides a complete solution to the CSL parametric oscillator system, a topic we suggest could play a very important role to further constrain the CSL parameters. Our results illustrate the remarkable power of inflation and cosmology to constrain new physics.

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•Jul 12, 2021•0 citations
The Continuous Spontaneous Localization (CSL) model offers a dynamical solution to the quantum measurement problem by introducing a classical stochastic field that induces wavefunction collapse, yet the physical origin of this field remainselusive. A promising recent proposal identifies a light scalar field coupled via the Higgs portal as the source of this collapse-inducing noise, with its efficacy governed by a non-equilibrium enhancement factor Xϕ. In this work, we perform the first comprehensive, first-principles derivation of Xϕ from cosmological dynamics, establishing a concrete microphysical origin forCSL noise. We analyze two well-motivated cosmological production mechanisms: - vacuum misalignment—where the scalar acquires a coherent displacement during inflation—and freeze-in via ultra-weak Higgs interactions. For each mechanism, we derive explicit, predictive expressions for Xϕ in terms of fundamental parameters(λHS , ϕi, Hinf , mϕ), connecting inflationary initial conditions to laboratory-scale col lapse rates. Our analysis reveals a fundamental dichotomy: while the misalignment mechanism naturally yields Xϕ ∼ O(10−10e9) from realistic initial conditions (ϕi ∼ 10e13−10e15 GeV, Hinf ∼ 10e10 GeV), enabling observable CSL effects with λ ∼ 2×10e−12 s−1, the freeze-in mechanism produces Xϕ ≪ 1 for couplings allowed by astrophysics, rendering it phenomenologically irrelevant for collapse dynamics.We confront these predictions with the complete suite of current observational constraints, including stellar cooling bounds, fifth-force searches, Planck data on isocurvature perturbations and dark matter abundance, LHC Higgs measurements,and non-interferometric tests of CSL. Notably, we demonstrate that: 1. The viable parameter space for misalignment-produced CSL noise is robust, occupying approximately two orders of magnitude in ϕi and Hinf ;2. All existing constraints from particle physics, astrophysics, and cosmology are simultaneously satisfied without fine-tuning;3. Key predictions include a universal collapse rate λ ∼ 2 × 10e−12 s−1 for rC ∼ 200 nm, mass-dependent decoherence in matter-wave interferometry, and potential high-frequency spectral features from the oscillating condensate. This work provides three key advances: (i) it resolves the long-standing “no-go” obstruction for equilibrium scalar fields to generate Markovian collapse noise by identifying cosmological misalignment as a natural source of persistent non-equilibrium; (ii) it establishes a testable connection between early-universe physics (inflation, scalar condensates) and laboratory-scale quantum phenomena; and (iii) it transforms Higgs-portal collapse models from phenomenological frameworks into predictive cosmological scenarios with falsifiable predictions for next-generation experiments. By deriving Xϕ from cosmology rather than parameterizing it, we complete the microphysical foundation of scalar-field collapse models and open a new pathway toward unifying quantum foundations with cosmological history.
We propose and analyze a model of objective wave-function collapse induced by alightreal scalar field ϕ coupled to the mass density of matter viaa Higgs-portal interaction. Themodel aims to provide a microscopic origin for continuous spontaneous localization (CSL)–type dynamics while remaining compatible with particle physics, astrophysical, and non-interferometric collapse constraints. Starting from a concrete Higgs-portal Lagrangian, we derive the non-Markovian master equation for the reduced density matrix of matter obtained by integrating out ϕ in a general Gaussian state. We show that for a massive scalar field in thermal equilibrium (including the vacuum) the Markovian limit required to recover a CSL-like Lindblad term vanishes identically : the time-integrated field correlator defining the would-be Markovian kernel is zero for m_ϕ= ̸=0. This provides a simple“no-go” result: a standard equilibrium quantum field cannot generate a white-noise collapse term of CSL type. We then introduce a phenomenological non-equilibrium scalar noise parameterized by a dimensionless amplification factor X_ϕ and derive the mapping between the scalar–nucleon coupling gs and the CSL collapse rate λ as a function of the correlation length r_C. Using theHiggs-portal structure, we relate gs to the mixing angle θ and portal coupling λHS and confront the model with (i) astrophysical bounds on fifth-forces and stellar cooling, (ii) collider limits on invisible Higgs decays and Higgs–scalar mixing, and (iii) non-interferometric CSL constraints from X-ray emission, bulk heating, cold atoms, LISA Pathfinder and planetary heating. We show that the reexists aviable region of parameter space with mϕ∼eV, r_C∼200nm, gs≲10e-13, λ_HS∼10e−11 and λ∼10e12s−1 which satisfies simultaneously all current constraints while providing a potentially observable collapse rate for mesoscopic systems. Our analysis clarifies both the promise and limitations of Higgs-portal scalar field collapse models : they offer a concrete, testable UV completion for CSL, but require the scalar sector to be in a non-equilibrium, effectively classical state whose microscopic origin remains to be explained. NB: "This is personal/unfunded research."
This deposit collects Papers I–XIII of an ongoing research programme developing a “Transactional Unimodular CSL” (TUCSL) framework: a non-perturbative approach to quantum gravity and cosmology that combines (i) a version of relativistic direct–action / transactional interpretation (RTI/QDAT) of quantum fields, (ii) Continuous Spontaneous Localization (CSL) collapse dynamics, and (iii) unimodular gravity with an emergent, fluctuating cosmological constant. We differ from standard RTI or transactional approach because we do not see classic, lorentzian spacetime as just an emerging property. The central idea is a dual ontology. We consider psi-ontic description valid in the unitary quantum regime and the classic spacetime as equally valid in the lorentzian regime. As we will see, there is a bandage region connecting the two regimes: this is where the CSL "noise" comes from. At the fundamental level there is a prespacetime Hilbert space of offer and confirmation waves; actualized transactions pick out events, which, after coarse-graining, appear as an effective Lorentzian spacetime with metric and causal structure. A single covariant noise kernel C(x,y) (or its q-metric version C_q) links the two levels: it drives CSL-type decoherence, encodes the statistics of failed transactions, and generates an intrinsic arrow of time and entropy production. The early papers construct such kernels in flat and curved spacetimes, relate their strength to standard CSL parameters, and show how Diósi–Penrose–like gravitational decoherence, unimodular Λ-fluctuations and an effective dark-energy component arise from the same noise sector. The q-metric / zero-point-length geometry of Padmanabhan and Kothawala is used to implement a minimal area and a discrete four-volume structure, tying TUCSL to causal-set ideas and generalized quantum mechanics. Later papers apply this framework to black holes and cosmology. For black holes, the noise-modified field equations and a stochastic Raychaudhuri equation yield de Sitter–like regular cores, horizon thermodynamics and an obstruction to Penrose-type singularities compatible with QFC/QNEC-style bounds. For cosmology, a transactional “bandage region” between prespacetime and minisuperspace selects a most probable inflaton potential via two effective parameters: β, a geometric–entropic count of unimodular four-volume cells (naturally modelled by Tsallis-type entropy), and α_eff, the integrated CSL noise power constrained by information-theoretic bounds. Their competition produces a sharply peaked inflationary scale V^(1/4) ~ 10¹⁵–10¹⁶ GeV, in line with CMB data, without ad hoc tuning. Overall, Papers I–XIII offer a coherent scenario in which the arrow of time, black-hole thermodynamics, Λ-fluctuations and the inflationary scale are different faces of a single transactional CSL noise sector implemented in a unimodular setting.
This memo addresses a question: In the “substrate field–soliton” model (v2 paper), canthe intuition “observation collapse = irreversible physical process” be realized as a concretedynamical collapse model? The answer is yes, but with a decisive number attached. Weprove that: (i) The master equation driven by the noise naturally derived from the masscoupling m(ϕ) is structurally isomorphic to the CSL (Continuous Spontaneous Localization) model, and the two ad hoc assumptions of CSL—mass-weighted coupling and positionbasis—are no longer assumptions in this model, but corollaries of the equivalence principleand the mass density operator; (ii) The collapse rate is proportional to Newton’s constant,Γ ∝ Gm2, realizing the motivation of the Di´osi–Penrose program that “collapse strengthis given by gravity,” though the mechanism is different (substrate noise rather than spacetime superposition instability); (iii) Decisive verdict: If the noise is taken as the quantumvacuum fluctuation of ϕ, the single-nucleon collapse rate is ∼ 10−28 s−1, which is 12 orders of magnitude smaller than the value required by GRW—the pure quantum fluctuationversion cannot solve the measurement problem. To achieve true collapse, “intrinsic probability” must be interpreted as a classical true-random component of the substrate condensate,whose power D becomes a new free parameter. In this case, the model becomes a CSL witha specific mediating field, and its heating rate directly interfaces with existing experimentalconstraints (X-ray spontaneous emission, cantilever noise, LISA Pathfinder). We presenta complete parameter space analysis, including the “localization-heating squeeze” identityP/λ = ℏ2/(2m0rC2), which explains why models with rC ∼ 1 fm are strictly ruled out, whilethose with rC ∼ 10−7 m survive.
The continuous spontaneous localization (CSL) model has been proposed as a possible solution to the quantum measurement problem by modifying the Schrödinger equation. In this work, we apply the CSL model to two cosmological models of the early Universe: the matter bounce scenario and slow roll inflation. In particular, we focus on the generation of the classical primordial inhomogeneities and anisotropies that arise from the dynamical evolution, provided by the CSL mechanism, of the quantum state associated to the quantum fields. In each case, we obtained a prediction for the shape and the parameters characterizing the primordial spectra (scalar and tensor), i.e. the amplitude, the spectral index and the tensor-to-scalar ratio. We found that there exist CSL parameter values, allowed by other non-cosmological experiments, for which our predictions for the angular power spectrum of the CMB temperature anisotropy are consistent with the best fit canonical model to the latest data released by the Planck Collaboration.
According to cosmological inflation, the inhomogeneities in our Universe are of quantum-mechanical origin. This scenario is phenomenologically very appealing as it solves the puzzles of the standard hot big bang model and naturally explains why the spectrum of cosmological perturbations is almost scale invariant. It is also an ideal playground to discuss deep questions among which is the quantum measurement problem in a cosmological context. Although the large squeezing of the quantum state of the perturbations and the phenomenon of decoherence explain many aspects of the quantum-to-classical transition, it remains to understand how a specific outcome can be produced in the early Universe, in the absence of any observer. The continuous spontaneous localization (CSL) approach to quantum mechanics attempts to solve the quantum measurement question in a general context. In this framework, the wave function collapse is caused by adding new nonlinear and stochastic terms to the Schr\"odinger equation. In this paper, we apply this theory to inflation, which amounts to solving the CSL parametric oscillator case. We choose the wave function collapse to occur on an eigenstate of the Mukhanov-Sasaki variable and discuss the corresponding modified Schr\"odinger equation. Then, we compute the power spectrum of the perturbations and show that it acquires a universal shape with two branches, one which remains scale invariant and one with nS=4{n}_{\mathrm{S}}=4nS​=4, a spectral index in obvious contradiction with the cosmic microwave background anisotropy observations. The requirement that the non-scale-invariant part be outside the observational window puts stringent constraints on the parameter controlling the deviations from ordinary quantum mechanics. Due to the absence of a CSL amplification mechanism in field theory, this also has the consequence that the collapse mechanism of the inflationary fluctuations is not efficient. Then, we determine the collapse time. On small scales the collapse is almost instantaneous, and we recover exactly the behavior of the CSL harmonic oscillator (a case for which we present new results), whereas, on large scales, we find that the collapse is delayed and can take several e-folds to happen. We conclude that recovering the observational successes of inflation and, at the same time, reaching a satisfactory resolution of the inflationary ``macro-objectification'' issue seems problematic in the framework considered here. This work also provides a complete solution to the CSL parametric oscillator system, a topic we suggest could play a very important role to further constrain the CSL parameters. Our results illustrate the remarkable power of inflation and cosmology to constrain new physics.
We propose a novel model for the natural extrapolation of the continuous spontaneous localization (CSL) theory, in order to account for the origin of primordial inhomogeneities during inflation. This particular model is based on three main elements: (i) the semiclassical gravity framework, (ii) a collapse-generating operator associated to a relativistic invariant scalar of the energy-momentum tensor, and (iii) an extension of the CSL parameter(s) as a function of the spacetime curvature. Furthermore, employing standard cosmological perturbation theory at linear order, and for a reasonable range within the parameter space of the model, we obtain a nearly scale invariant power spectrum consistent with recent observational CMB data. This opens a vast landscape of different options for the application of the CSL theory to the cosmological context, and possibly sheds light on searches for a full covariant version of the CSL theory.