Miguel Escudero
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
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Miguel Escudero has a total of 189 co-authors. Here are the top co-authors by number of shared publications:
- James Alvey
Kavli Institute for Cosmology Cambridge
14 shared publications - Dan Hooper
Fermi National Accelerator Laboratory
10 shared publications - Samuel J. Witte
University of Oxford
10 shared publications - Malcolm Fairbairn
King’s College London
9 shared publications - Nashwan Sabti
Johns Hopkins University
8 shared publications - Gonzalo Alonso-Álvarez
University of Toronto
6 shared publications
Latest Publications
- Open Access
- 13 October 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (7) , 075017
What does it take to have N eff < 3 at CMB times?
The vast majority of extensions of the Standard Model affecting the number of effective relativistic neutrino species ( N eff ) do so additively, namely, they enhance this quantity with some light state contributing to dark radiation. In this work, we consider precisely the opposite case: new physics scenarios that can lead to N eff < 3 that are consistent with all known cosmological, astrophysical, and laboratory data. We are motivated by three main reasons: (1) a recent measurement from Atacama Cosmology Telescope (ACT) and the South Pole Telescope (SPT) in combination with Planck that leads to N eff = 2.81 ± 0.12 , (2) by a new and powerful measurement of the primordial helium abundance, which anchors N eff to be very close to the Standard Model value one second after the big bang, (3) by the deployment of the Simons Observatory which will provide precise tests of the radiation content in the Universe and which may detect with a high significance cosmologies with N eff < 3 . We survey the main theoretical possibilities and find that only a few simple scenarios can consistently give N eff = 2.81 ± 0.12 . One class consists of thermal electrophilic relics with masses m ∼ 8 – 13 MeV . Another consists of out-of-equilibrium particles decaying to e + e − or γ γ , with a rather particular lifetime 0.05 s ≲ τ ≲ 3 min , mass 250 MeV ≲ m ≲ 600 MeV , and abundance ρ / ρ γ ∼ 0.1 at decay. Thermal electrophilic particles are especially interesting because they can account for the dark matter in the Universe and can be tested in experiments such as SENSEI, DAMIC-M, and Oscura, and their portals to the visible sector at experiments such as NA64 and LDMX. We conclude that if the Simons Observatory confirms that N eff ≃ 2.8 , it will point to very specific extensions of the Standard Model.
- 13 October 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (7) , 075017
Open AccessWhat does it take to have N eff < 3 at CMB times?
The vast majority of extensions of the Standard Model affecting the number of effective relativistic neutrino species ( N eff ) do so additively, namely, they enhance this quantity with some light state contributing to dark radiation. In this work, we consider precisely the opposite case: new physics scenarios that can lead to N eff < 3 that are consistent with all known cosmological, astrophysical, and laboratory data. We are motivated by three main reasons: (1) a recent measurement from Atacama Cosmology Telescope (ACT) and the South Pole Telescope (SPT) in combination with Planck that leads to N eff = 2.81 ± 0.12 , (2) by a new and powerful measurement of the primordial helium abundance, which anchors N eff to be very close to the Standard Model value one second after the big bang, (3) by the deployment of the Simons Observatory which will provide precise tests of the radiation content in the Universe and which may detect with a high significance cosmologies with N eff < 3 . We survey the main theoretical possibilities and find that only a few simple scenarios can consistently give N eff = 2.81 ± 0.12 . One class consists of thermal electrophilic relics with masses m ∼ 8 – 13 MeV . Another consists of out-of-equilibrium particles decaying to e + e − or γ γ , with a rather particular lifetime 0.05 s ≲ τ ≲ 3 min , mass 250 MeV ≲ m ≲ 600 MeV , and abundance ρ / ρ γ ∼ 0.1 at decay. Thermal electrophilic particles are especially interesting because they can account for the dark matter in the Universe and can be tested in experiments such as SENSEI, DAMIC-M, and Oscura, and their portals to the visible sector at experiments such as NA64 and LDMX. We conclude that if the Simons Observatory confirms that N eff ≃ 2.8 , it will point to very specific extensions of the Standard Model.
- Open Access
- 9 May 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (5) , 500
Nucleosynthesis and CMB bounds on photophilic ALPs: a fresh look
We provide a fresh look at the cosmological constraints on axion-like particles (ALPs) that couple predominantly to photons, focusing on lifetimes $$\tau _{a} \lesssim 10^{4}\, \textrm{s}$$ and masses $$m_a\lesssim 10\,\textrm{GeV}$$ . We consider Big Bang nucleosynthesis (BBN) and Cosmic Microwave Background (CMB) bounds and explore how these limits depend upon the unknown reheating temperature of the Universe, $$T_\textrm{reh}$$ . Compared with some previous studies, we account for the rare decays of these ALPs into light hadrons and show that this leads to extended constraints for several reheating temperatures. Our limits are cast in a model-independent way, and we identify regions of parameter space where these ALPs could alleviate small tensions in the determinations of $$N_\textrm{eff}$$ and the deuterium abundance. Our Mathematica BBN code is publicly available at .- 9 May 2026
- Published by Springer Nature in The European Physical Journal C
- Vol. 86 (5) , 500
Open AccessNucleosynthesis and CMB bounds on photophilic ALPs: a fresh look
We provide a fresh look at the cosmological constraints on axion-like particles (ALPs) that couple predominantly to photons, focusing on lifetimes $$\tau _{a} \lesssim 10^{4}\, \textrm{s}$$ and masses $$m_a\lesssim 10\,\textrm{GeV}$$ . We consider Big Bang nucleosynthesis (BBN) and Cosmic Microwave Background (CMB) bounds and explore how these limits depend upon the unknown reheating temperature of the Universe, $$T_\textrm{reh}$$ . Compared with some previous studies, we account for the rare decays of these ALPs into light hadrons and show that this leads to extended constraints for several reheating temperatures. Our limits are cast in a model-independent way, and we identify regions of parameter space where these ALPs could alleviate small tensions in the determinations of $$N_\textrm{eff}$$ and the deuterium abundance. Our Mathematica BBN code is publicly available at . - Top Cited PapersOpen Access
- 1 February 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (02)
Fast and flexible neutrino decoupling. Part I. The Standard Model
Cosmological determinations of the number of relativistic neutrino species, N eff , are becoming increasingly accurate, and further improvements are expected both from CMB and BBN data. Given this context, we update the evaluation of N eff and the current entropy density via the momentum-averaged approach. This allows for a numerically fast description of neutrino decoupling, easily portable to an array of new physics scenarios. We revisit all aspects of this approach, including collision terms with full electron mass dependence, finite temperature QED corrections to the equation of state, neutrino oscillations, and the modelling of neutrino ensembles with effective chemical potentials. For integrated observables, our results differ by less than 0.04% from the solution of the momentum-dependent evolution equation. We outline how to extend the approach to BSM settings, and will highlight its power in Part II. To facilitate the practical implementation, we release a Mathematica and python code within nudec_BSM_v2 , easily linkable to BBN codes.
- 1 February 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (02)
Top Cited PapersOpen AccessFast and flexible neutrino decoupling. Part I. The Standard Model
Cosmological determinations of the number of relativistic neutrino species, N eff , are becoming increasingly accurate, and further improvements are expected both from CMB and BBN data. Given this context, we update the evaluation of N eff and the current entropy density via the momentum-averaged approach. This allows for a numerically fast description of neutrino decoupling, easily portable to an array of new physics scenarios. We revisit all aspects of this approach, including collision terms with full electron mass dependence, finite temperature QED corrections to the equation of state, neutrino oscillations, and the modelling of neutrino ensembles with effective chemical potentials. For integrated observables, our results differ by less than 0.04% from the solution of the momentum-dependent evolution equation. We outline how to extend the approach to BSM settings, and will highlight its power in Part II. To facilitate the practical implementation, we release a Mathematica and python code within nudec_BSM_v2 , easily linkable to BBN codes.
- Open Access
- 1 February 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (02)
A limit on the total lepton number in the Universe from BBN and the CMB
At temperatures below the QCD phase transition, any substantial lepton number in the Universe can only be present within the neutrino sector. In this work, we systematically explore the impact of a non-vanishing lepton number on Big Bang Nucleosynthesis (BBN) and the Cosmic Microwave Background (CMB). Relying on our recently developed framework based on momentum averaged quantum kinetic equations for the neutrino density matrix, we solve the full BBN reaction network to obtain the abundances of primordial elements. We find that the maximal primordial total lepton number L allowed by BBN and the CMB is -0.12 (-0.10) ≤ L ≤ 0.13 (0.12) for NH (IH), while specific flavor directions can be even more constrained. This bound is complementary to the limits obtained from avoiding baryon overproduction through sphaleron processes at the electroweak phase transition since, although numerically weaker, it applies at lower temperatures and is obtained completely independently. We publicly release the C++ code COFLASY-C on GitHub ( https://github.com/mariofnavarro/COFLASY/tree/COFLASY-C ) which solves for the evolution of the neutrino quantum kinetic equations numerically.
- 1 February 2026
- Published by IOP Publishing in Journal of Cosmology and Astroparticle Physics
- Vol. 2026 (02)
Open AccessA limit on the total lepton number in the Universe from BBN and the CMB
At temperatures below the QCD phase transition, any substantial lepton number in the Universe can only be present within the neutrino sector. In this work, we systematically explore the impact of a non-vanishing lepton number on Big Bang Nucleosynthesis (BBN) and the Cosmic Microwave Background (CMB). Relying on our recently developed framework based on momentum averaged quantum kinetic equations for the neutrino density matrix, we solve the full BBN reaction network to obtain the abundances of primordial elements. We find that the maximal primordial total lepton number L allowed by BBN and the CMB is -0.12 (-0.10) ≤ L ≤ 0.13 (0.12) for NH (IH), while specific flavor directions can be even more constrained. This bound is complementary to the limits obtained from avoiding baryon overproduction through sphaleron processes at the electroweak phase transition since, although numerically weaker, it applies at lower temperatures and is obtained completely independently. We publicly release the C++ code COFLASY-C on GitHub ( https://github.com/mariofnavarro/COFLASY/tree/COFLASY-C ) which solves for the evolution of the neutrino quantum kinetic equations numerically.
- Open Access
Keeping It Renormalizable: Minimal Baryogenesis induced Asymmetric Dark Matter
Many asymmetric dark matter scenarios have been proposed to date. Among them, perhaps the most motivated ones are those in which the dark matter asymmetry is induced from the baryon/lepton asymmetries via chemical equilibration without any new sources of CP violation. However, most of the models put forward along these lines have been excluded by now and/or are based on complicated setups. In this letter, we present a new, simple, and viable scenario. It assumes only two new fields: a scalar singlet and an inert scalar doublet, and is based only on renormalizable interactions, that slowly generate the dark matter asymmetry from the Standard Model Higgs asymmetry. The model allows for the direct detection of dark matter in the upcoming generation of experiments, and the inert doublet is predicted to be light enough to be potentially produced and observed at the LHC and future colliders, $m_{H'}<580\,{\rm GeV}$.Open AccessKeeping It Renormalizable: Minimal Baryogenesis induced Asymmetric Dark Matter
Many asymmetric dark matter scenarios have been proposed to date. Among them, perhaps the most motivated ones are those in which the dark matter asymmetry is induced from the baryon/lepton asymmetries via chemical equilibration without any new sources of CP violation. However, most of the models put forward along these lines have been excluded by now and/or are based on complicated setups. In this letter, we present a new, simple, and viable scenario. It assumes only two new fields: a scalar singlet and an inert scalar doublet, and is based only on renormalizable interactions, that slowly generate the dark matter asymmetry from the Standard Model Higgs asymmetry. The model allows for the direct detection of dark matter in the upcoming generation of experiments, and the inert doublet is predicted to be light enough to be potentially produced and observed at the LHC and future colliders, $m_{H'}<580\,{\rm GeV}$. - Open Access
- 27 June 2025
- Published by Elsevier in Physics Letters B
- Vol. 868
The simplest dark matter model at the edge of perturbativity
- 27 June 2025
- Published by Elsevier in Physics Letters B
- Vol. 868
Open AccessThe simplest dark matter model at the edge of perturbativity
- Open Access
- 13 June 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (6) , 1-56
Lepton flavor asymmetries: from the early Universe to BBN
Large primordial lepton flavor asymmetries with almost vanishing total baryon-minus-lepton number can evade the usual BBN and CMB constraints if neutrino oscillations lead to perfect flavor equilibration. Solving the momentum averaged quantum kinetic equations (QKEs) describing neutrino oscillations and interactions, we perform the first systematic investigation of this scenario, uncovering a rich flavor structure in stark contradiction to the assumption of simple flavor equilibration. We find (i) a particular direction in flavor space, ∆n e ≃ – 2/3 (– 1)∆n μ for normal (inverted) neutrino mass hierarchy, in which the flavor equilibration is efficient and primordial asymmetries are essentially unconstrained, (ii) a minimal washout factor, $$ {\left.\Delta {n}_e^2\right|}_{\textrm{BBN}} $$ ≤ 0.03 (0.016) ∑ α $$ {\left.\Delta {n}_{\alpha}^2\right|}_{\textrm{ini}} $$ yielding a conservative estimate for the allowed primordial asymmetries in a generic flavor direction, and (iii) particularly strong or weak washout if one of the initial flavor asymmetries vanishes due to non-adiabatic muon- or electron-driven MSW transitions. These results open up the possibility of a first-order QCD phase transition facilitated by large lepton asymmetries as well as baryogenesis from large and compensated ∆n e = ∆n μ asymmetries. Our systematic approach of deriving momentum averaged QKEs includes collision terms beyond the damping approximation, energy transfer between the neutrino and electron-photon plasma, and provides a fast and reliable way to investigate the impact of primordial lepton asymmetries at the time of BBN. We publicly release the Mathematica code COFLASY-M on https://github.com/mariofnavarro/COFLASY which solves the QKEs numerically.- 13 June 2025
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2025 (6) , 1-56
Open AccessLepton flavor asymmetries: from the early Universe to BBN
Large primordial lepton flavor asymmetries with almost vanishing total baryon-minus-lepton number can evade the usual BBN and CMB constraints if neutrino oscillations lead to perfect flavor equilibration. Solving the momentum averaged quantum kinetic equations (QKEs) describing neutrino oscillations and interactions, we perform the first systematic investigation of this scenario, uncovering a rich flavor structure in stark contradiction to the assumption of simple flavor equilibration. We find (i) a particular direction in flavor space, ∆n e ≃ – 2/3 (– 1)∆n μ for normal (inverted) neutrino mass hierarchy, in which the flavor equilibration is efficient and primordial asymmetries are essentially unconstrained, (ii) a minimal washout factor, $$ {\left.\Delta {n}_e^2\right|}_{\textrm{BBN}} $$ ≤ 0.03 (0.016) ∑ α $$ {\left.\Delta {n}_{\alpha}^2\right|}_{\textrm{ini}} $$ yielding a conservative estimate for the allowed primordial asymmetries in a generic flavor direction, and (iii) particularly strong or weak washout if one of the initial flavor asymmetries vanishes due to non-adiabatic muon- or electron-driven MSW transitions. These results open up the possibility of a first-order QCD phase transition facilitated by large lepton asymmetries as well as baryogenesis from large and compensated ∆n e = ∆n μ asymmetries. Our systematic approach of deriving momentum averaged QKEs includes collision terms beyond the damping approximation, energy transfer between the neutrino and electron-photon plasma, and provides a fast and reliable way to investigate the impact of primordial lepton asymmetries at the time of BBN. We publicly release the Mathematica code COFLASY-M on https://github.com/mariofnavarro/COFLASY which solves the QKEs numerically. - Open Access
- 10 April 2025
- Published by Sissa Medialab Srl
- Vol. 481, 023
How large could CP violation in $B$ meson mixing be? Implications for baryogenesis and future searchesIt is well-known that CP violation is one of the necessary ingredients to generate the observed matter-antimatter asymmetry of the Universe. Neutral $B$ mesons naturally exhibit CP violating oscillations, such that the amount of CP violation in their mixing can be directly related to the baryon asymmetry through the $B$-mesogenesis mechanism. With this in mind, it is interesting to analyze the extent to which CP is violated in $B$ meson mixing within different scenarios beyond the Standard Model. In particular, we consider: (i) the effects of heavy new physics in the mass mixing following a model-independent approach, (ii) the implications of CKM unitarity deviations with the inclusion of vector-like quarks, and (iii) the role of new contributions to the decay width mixing. The available parameter space for the relevant CP asymmetries is presented, studying their compatibility with the $B$-mesogenesis framework and comparing it with the expected experimental sensitivity for these quantities at LHCb and Belle II.- 10 April 2025
- Published by Sissa Medialab Srl
- Vol. 481, 023
Open AccessHow large could CP violation in $B$ meson mixing be? Implications for baryogenesis and future searchesIt is well-known that CP violation is one of the necessary ingredients to generate the observed matter-antimatter asymmetry of the Universe. Neutral $B$ mesons naturally exhibit CP violating oscillations, such that the amount of CP violation in their mixing can be directly related to the baryon asymmetry through the $B$-mesogenesis mechanism. With this in mind, it is interesting to analyze the extent to which CP is violated in $B$ meson mixing within different scenarios beyond the Standard Model. In particular, we consider: (i) the effects of heavy new physics in the mass mixing following a model-independent approach, (ii) the implications of CKM unitarity deviations with the inclusion of vector-like quarks, and (iii) the role of new contributions to the decay width mixing. The available parameter space for the relevant CP asymmetries is presented, studying their compatibility with the $B$-mesogenesis framework and comparing it with the expected experimental sensitivity for these quantities at LHCb and Belle II. - Open Access
- 26 December 2024
- Published by American Physical Society (APS) in Physical Review D
- Vol. 110 (12)
Critical look at the cosmological neutrino mass bound
Cosmological neutrino mass bounds are becoming increasingly stringent. The latest limit within Λ CDM from Planck 2018 + ACT lensing + DESI is ∑ m ν < 0.072 eV at 95% CL, very close to the minimum possible sum of neutrino masses ( ∑ m ν > 0.06 eV ), hinting at vanishing or even “negative” cosmological neutrino masses. In this context, it is urgent to carefully evaluate the origin of these cosmological constraints. In this paper, we investigate the robustness of these results in three ways: (i) we check the role of potential anomalies in Planck CMB and DESI BAO data; (ii) we compare the results for frequentist and Bayesian techniques, as very close to physical boundaries subtleties in the derivation and interpretation of constraints can arise; (iii) we investigate how deviations from Λ CDM , potentially alleviating these anomalies, can alter the constraints. From a profile likelihood analysis, we derive constraints in agreement at the ∼ 10 % level with Bayesian posteriors. We find that the weak preference for negative neutrino masses is mostly present for Planck 18 data, affected by the well-known “lensing anomaly.” It disappears when the new Planck 2020 HiLLiPoP is used, leading to significantly weaker constraints. Additionally, the pull toward negative masses in DESI data stems from the z = 0.7 bin, which contains a BAO measurement in ∼ 3 σ tension with Planck expectations. Without this bin, and in combination with HiLLiPoP, the bound relaxes to ∑ m ν < 0.11 eV at 95% CL. The recent preference for dynamical dark energy alleviates this tension and further weakens the bound. As we are at the dawn of a neutrino mass discovery from cosmology, it will be very exciting to see if this trend is confirmed by future data. Published by the American Physical Society 2024
- 26 December 2024
- Published by American Physical Society (APS) in Physical Review D
- Vol. 110 (12)
Open AccessCritical look at the cosmological neutrino mass bound
Cosmological neutrino mass bounds are becoming increasingly stringent. The latest limit within Λ CDM from Planck 2018 + ACT lensing + DESI is ∑ m ν < 0.072 eV at 95% CL, very close to the minimum possible sum of neutrino masses ( ∑ m ν > 0.06 eV ), hinting at vanishing or even “negative” cosmological neutrino masses. In this context, it is urgent to carefully evaluate the origin of these cosmological constraints. In this paper, we investigate the robustness of these results in three ways: (i) we check the role of potential anomalies in Planck CMB and DESI BAO data; (ii) we compare the results for frequentist and Bayesian techniques, as very close to physical boundaries subtleties in the derivation and interpretation of constraints can arise; (iii) we investigate how deviations from Λ CDM , potentially alleviating these anomalies, can alter the constraints. From a profile likelihood analysis, we derive constraints in agreement at the ∼ 10 % level with Bayesian posteriors. We find that the weak preference for negative neutrino masses is mostly present for Planck 18 data, affected by the well-known “lensing anomaly.” It disappears when the new Planck 2020 HiLLiPoP is used, leading to significantly weaker constraints. Additionally, the pull toward negative masses in DESI data stems from the z = 0.7 bin, which contains a BAO measurement in ∼ 3 σ tension with Planck expectations. Without this bin, and in combination with HiLLiPoP, the bound relaxes to ∑ m ν < 0.11 eV at 95% CL. The recent preference for dynamical dark energy alleviates this tension and further weakens the bound. As we are at the dawn of a neutrino mass discovery from cosmology, it will be very exciting to see if this trend is confirmed by future data. Published by the American Physical Society 2024
- Open Access
- 24 December 2024
- Published by American Physical Society (APS) in Physical Review D
- Vol. 110 (11)
How large could the violation in neutral -meson mixing be? Implications for baryogenesis and upcoming searchesC P violation in neutral B meson oscillations is an experimental observable that could be directly related to the baryon asymmetry of the Universe through the B -mesogenesis mechanism. As this phenomenon is highly suppressed in the Standard Model, it could also be a sensitive probe for many new physics scenarios that modify neutral meson mixing. Motivated by these facts, and the timely B physics program at the LHC and Belle II, we analyze how large C P violation in the mixing of neutral B d and B s meson systems could be. We answer this question, in light of current experimental data, within three different scenarios, namely: (i) generic heavy new physics only affecting the mass mixing M 12 q , (ii) vectorlike quark extensions that introduce deviations of 3 × 3 CKM unitarity, and (iii) light new physics modifying the decay mixing Γ 12 q . We find that enhancements of the semileptonic asymmetries, that measure the amount of C P violation in mixing, at the level of 10 − 3 for the B d system and 10 − 4 for the B s system can be achieved within scenarios (i) and (ii), while they are much more suppressed in realistic UV completions triggering scenario (iii). With respect to cosmology, the difficulty of finding large C P asymmetries in our analysis puts the B -mesogenesis mechanism in tension. Finally, we conclude that upcoming experimental searches for C P violation in B meson mixing at LHCb and Belle II are unlikely to detect a new physics signal for the most generic models. Published by the American Physical Society 2024
- 24 December 2024
- Published by American Physical Society (APS) in Physical Review D
- Vol. 110 (11)
Open AccessHow large could the violation in neutral -meson mixing be? Implications for baryogenesis and upcoming searchesC P violation in neutral B meson oscillations is an experimental observable that could be directly related to the baryon asymmetry of the Universe through the B -mesogenesis mechanism. As this phenomenon is highly suppressed in the Standard Model, it could also be a sensitive probe for many new physics scenarios that modify neutral meson mixing. Motivated by these facts, and the timely B physics program at the LHC and Belle II, we analyze how large C P violation in the mixing of neutral B d and B s meson systems could be. We answer this question, in light of current experimental data, within three different scenarios, namely: (i) generic heavy new physics only affecting the mass mixing M 12 q , (ii) vectorlike quark extensions that introduce deviations of 3 × 3 CKM unitarity, and (iii) light new physics modifying the decay mixing Γ 12 q . We find that enhancements of the semileptonic asymmetries, that measure the amount of C P violation in mixing, at the level of 10 − 3 for the B d system and 10 − 4 for the B s system can be achieved within scenarios (i) and (ii), while they are much more suppressed in realistic UV completions triggering scenario (iii). With respect to cosmology, the difficulty of finding large C P asymmetries in our analysis puts the B -mesogenesis mechanism in tension. Finally, we conclude that upcoming experimental searches for C P violation in B meson mixing at LHCb and Belle II are unlikely to detect a new physics signal for the most generic models. Published by the American Physical Society 2024