REVIEW 2 major objections 4 minor 33 references
Silent coverage failures in rare-event searches and a degeneracy index that predicts them
T0 review · 2 major / 4 minor · reviewed 2026-08-11 · deepseek-v4-flash
Pith's one-line read Two numbers predict silent coverage failures in rare-event searches.
desk verdict A genuinely useful screening diagnostic for coverage risk under model misspecification, with a real boundary-identifiability gap that needs a convention; deserves a serious referee, not a desk reject. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is Eq. (7), the Poisson–Fisher degeneracy index. With the Poisson–Fisher inner product $\langle u,v\rangle_W=\sum_i u_i v_i/\nu_{0,i}$ and the tangent matrix $T$ whose columns are the local derivatives $\partial\nu/\partial\vartheta_a$, the fitted displacement is $\Delta\hat\vartheta=F^{-1}T^T W\,\delta\nu$ with $F=T^T W T$; then $\beta=\Delta\hat\mu/\sqrt{(F^{-1})_{\mu\mu}}$ and $\gamma^2=(\delta\nu-T\Delta\hat\vartheta)^T W(\delta\nu-T\Delta\hat\vartheta)$. The paper connects $\beta$ to endpoint coverage through the local Gaussian reference $c_L\simeq\Phi(z_{1-\alpha/2}-\beta)$ and $c_U\simeq\Phi(z_{1-\alpha/2}+\beta)$, and uses $\gamma$ to order the rejection probability of the saturated-Poisson deviance test. A constrained-nuisance extension adds auxiliary Fisher information $F_{\mathrm{aux}}$ to the total information and a tension term $\Delta\hat\vartheta^T F_{\mathrm{aux}}\Delta\hat\vartheta$ to the residual. Projection onto the full fitted tangent space is what makes the diagnostic nuisance-aware: a deformation parallel to a background or mass derivative is absorbed there, changing both the predicted damage and the residual available to a goodness-of-fit test.
What would settle it
A decisive test is a single-bin Poisson experiment with fixed background and an exactly signal-collinear positive excess scanned over amplitude: the index predicts $\beta>0$, $\gamma=0$, monotone decrease of lower-endpoint coverage in $\beta$, and goodness-of-fit rejection at the 5\% floor for every amplitude. If toy coverage at $\mu=0$ is non-monotone in $\beta$, or if the goodness-of-fit rejection probability rises above the floor for any of these deformations, the sign and detectability ordering is falsified; the paper's own reported miss at $\beta=4.2$ (predicted 0.005, measured 0.20) already shows that the Gaussian reference can fail without falsifying the qualitative ordering.
Extended reading notes
Core claim
The central discovery is the Poisson–Fisher degeneracy index $\mathcal{I}_{\mathrm{PF}}(\delta\nu;\vartheta_0)=(\beta,\gamma)$, a two-coordinate screening diagnostic for a candidate model deformation. Given a deformation $\delta\nu$ of the nominal expected-count vector, one projects it onto the complete fitted tangent space using the local Poisson–Fisher metric $W=\mathrm{diag}(1/\nu_{0,i})$; $\beta$ is the resulting signed shift in the parameter of interest in profiled standard-error units, and $\gamma$ is the Poisson–Fisher norm of the residual outside all fitted directions. The paper shows empirically that the sign of $\beta$ tells which interval endpoint loses coverage—positive $\beta$ threatens the lower (discovery) endpoint, negative $\beta$ threatens the upper (exclusion) endpoint—while $\gamma$ tracks the power of a saturated-Poisson deviance test. Across the counting, dark-matter, and $0\nu\beta\beta$ settings, a deformation with large $|\beta|$ and small $\gamma$ is the dangerous case: the interval can move while the fitted spectrum looks fine. The paper also shows that calibration under the nominal simulator does not protect against misspecification of that simulator, and that modelling an exactly collinear deformation as a constrained nuisance restores coverage at evaluated points, at a sensitivity cost quantified by a factor up to 1.6.
Load-bearing premise
The diagnostic assumes that a first-order local projection computed at a reference point remains informative for coverage behavior at the boundary $\mu=0$ and for nonlocal deformations, where profile-likelihood asymptotics are nonstandard and parameters such as the WIMP mass are unidentified.
Editorial extensions
If this is right
- Robustness studies should report lower-endpoint, upper-endpoint, and whole-interval coverage separately; whole-interval coverage at $\mu=0$ tests only the lower endpoint and cannot validate a pure upper limit.
- Positive signal-like contamination degrades discovery-side coverage while making upper limits conservative, whereas negative signal bias from overestimated efficiency can make the upper endpoint undercover, so both deformation signs should be tested.
- Calibration under the nominal simulator, including a simulation-based method's internal coverage check, does not detect misspecification of that simulator relative to the data-generating process; a separate data-based model check is needed.
- A plausible deformation with large $|\beta|$ and small $\gamma$ should be promoted to a nuisance constrained by auxiliary data or a declared envelope; in the exactly collinear benchmark this restores coverage at evaluated grid points at up to a factor-1.6 sensitivity cost.
- The index can serve as pre-toy triage, but Eq. (8) is only a local reference; final coverage statements still require toy calibration, especially at boundaries and for nonlocal deformations.
Reading between the lines
- A natural extension is to compute the same projection with an observed-information metric for unbinned or learned likelihoods, giving $\beta$ and $\gamma$ for simulation-based inference pipelines without toy calibration.
- Because $\gamma$ orders the power of a residual check, it could guide test construction: binning and region-of-interest choices that increase $\gamma$ for a candidate deformation family should also increase the sensitivity of a goodness-of-fit test.
- The large-$|\beta|$, small-$\gamma$ corner is effectively an identifiability statement: near collinearity, no finite data-driven interval exists without external information, so the practical boundary is set by the strength of auxiliary constraints rather than by sample size.
- One testable extension is to turn the index into a calibration target, choosing deformation severities that reach a specified $\beta$ and using toy coverage to set analysis-specific 'large' and 'small' cutoffs, which the paper leaves open.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper studies how controlled model misspecification changes the frequentist coverage of intervals for a non-negative signal strength in low-count searches, using an exact Poisson counting benchmark, a dark-matter recoil spectrum, and a 0νββ peak search. It introduces the Poisson–Fisher degeneracy index I_PF = (β, γ): after projecting a candidate expected-count deformation onto the full fitted tangent space, β is the signed fitted signal shift in profiled standard-error units and γ is the Poisson–Fisher norm of the residual. The authors claim that locally the sign of β identifies which interval endpoint is threatened and that γ orders the detectability of the deformation by a saturated-Poisson goodness-of-fit test. They validate the qualitative predictions with toy Monte Carlo, show that calibration under the nominal simulator does not protect against misspecification, and demonstrate in an exactly collinear benchmark that promoting the deformation to a constrained nuisance restores coverage at the evaluated grid points at a quantifiable sensitivity cost.
Significance. If the screening diagnostic works as claimed, it would give experimental analyses a cheap, principled way to triage candidate model deformations before expensive toy calibration: large-|β|, small-γ directions are the dangerous ones and should be promoted to constrained nuisances. The paper's strengths include an explicit and simple formula (Eq. 7) for the index; a transparent controlled-severity protocol with stated sample sizes and binomial errors; exact Poisson summation in the counting benchmark; independent toy validation of the direction and rough severity of endpoint failures; and unusually honest reporting of the limitations of Eq. (8), including the large-β failure. The central qualitative claims—signed endpoint vulnerability and the importance of the full fitted tangent space—are supported by the clean counting and 0νββ examples as well as by the interior spectral tests. The main unresolved issue is the definition of the index at the boundary in settings with an unidentified secondary shape parameter, which affects part of the validation.
major comments (2)
- [Section 4, Eq. (7); Section 7, Fig. 9] The definition of β (and γ) at μ=0 for the spectral dark-matter analysis is not well-posed. At μ=0 the WIMP mass mχ is unidentified: the mχ column of the tangent matrix T vanishes, so F is singular, and the statement in Section 4 that "the projection is evaluated separately in each candidate local tangent space and the best-fitting branch is used" does not select a unique branch, because under the null all mχ branches give identical expected counts. The DM-tail points in Fig. 9 left, and the corresponding residual in Fig. 9 right, are therefore convention-dependent unless a branch-selection rule is specified (for example, a fixed reference mass, or the branch that maximizes |β|). This matters because the screening workflow is most valuable precisely at μ=0 and because the DM-tail point is used as boundary validation. Please specify the convention and recompute the affected points; if no unique convention is intended, state that boundary β is defined only up to branch and restrict the empirical boundary validation to settings with identified secondary parameters (counting and 0νββ).
- [Section 7, first paragraph; Eq. (8)] The paper honestly reports the failure of Eq. (8) at β=4.2 (predicted coverage ≈0.005, measured 0.20), but the assessment plot in Fig. 9 left still draws the Gaussian reference curve through the full range of plotted points. This curve is not a predictive relation in the large-deformation regime, and its presence could visually overstate the quantitative support for the index. Since the paper's central claim is that β is a screening coordinate rather than a finite-sample calibration, please either remove the dashed curve from the coverage-vs-β plot, restrict it to a clearly marked local regime, or add an explicit caption note that the curve is not a calibration and is known to fail at large β. The qualitative ordering claim is acceptable if framed in this way.
minor comments (4)
- [Section 2.1 and Fig. 1] The spectral model description would benefit from explicitly listing which parameters are fitted (μ, mχ and, if any, background scale or shape parameters), so that the "complete fitted tangent space" in Eq. (7) is unambiguous.
- [Reference [1]] Reference [1] contains the typo "tonne−Years" and the misspelling "lux-zeplin"; these should be corrected to "tonne-years" and "LUX-ZEPLIN".
- [Section 6.3, Fig. 3] The legend entry "CLs / Bayesian upper limit: upper edge" may confuse readers because both constructions are pure upper limits whose lower-endpoint coverage is trivially 1 at all severities; please clarify this in the caption.
- [Section 7, right panel] The sentence "the right-panel tail and line residuals use the same reference points" is ambiguous: please specify that the DM-tail residual is evaluated at the boundary branch used for β, and the line residuals at the Q-value, to avoid confusion with the interior halo point.
Circularity Check
No circularity: the Poisson–Fisher index is an independent diagnostic validated against toy-calibrated coverage; its collinear γ=0 property is a mathematical consequence, not a fitted prediction.
full rationale
The central claim is that the sign of β and the size of γ, computed from Eq. (7) using only nominal model derivatives and a specified deformation, predict endpoint coverage and goodness-of-fit detectability. These predictions are validated against independent toy-calibrated coverage and saturated-Poisson deviance rejection probabilities in Figures 3, 6, and 9. No parameter is fitted to the validation data; Eq. (8) is explicitly labeled a local reference, and the paper reports a large quantitative miss at β=4.2 (predicted coverage 0.005, measured 0.20), which would be impossible if the validation were forced by construction. The observation that a deformation exactly collinear with the signal template has γ=0 is a direct mathematical consequence of γ being defined as the residual after projection; the goodness-of-fit test has no sensitivity to that component because the fit absorbs it. This is a property the index is designed to quantify, not a circular renaming. The paper contains no load-bearing self-citations: all cited statistical and experimental works are external and used as background or as benchmarks. A genuine limitation, honestly stated, is that at μ=0 the WIMP mass mχ is unidentified, making the mχ column of the tangent matrix zero and F singular; the paper's solution of evaluating each candidate local tangent space and using the 'best-fitting branch' does not uniquely define β at the boundary, since all branches give identical expected counts under the null. This is a definitional/correctness concern about boundary identifiability, not circularity, because the coverage measurements are still independent of the index definition. The paper accordingly advises toy calibration at boundaries and does not present Eq. (8) as a finite-sample guarantee. Overall, the derivation chain is self-contained and the predictions are externally tested rather than reduced to their inputs.
Assumptions & free parameters
free parameters (3)
- Stress-test severity endpoints (s=1) for each deformation
- Nuisance calibration grid and finite-calibration guard =
η in [-0.20, 0.20], five points, 90.5% quantile
- Goodness-of-fit type-I error =
5% marginal prior-predictive
assumptions (5)
- domain assumption Data follow a Poisson likelihood n ~ Poisson(κμ + b)
- domain assumption Misspecification is representable as an additive deformation of expected counts δν
- domain assumption Local identifiability and positive-definite Fisher information F at the reference point
- ad hoc to paper Local Gaussian approximation relating β to endpoint coverage (Eq. 8)
- ad hoc to paper Saturated Poisson deviance is approximately quadratic with noncentrality γ²
invented entities (1)
-
Poisson-Fisher degeneracy index I_PF = (β, γ)
independent evidence
Cite this review
Pith. "Pith review of Silent coverage failures in rare-event searches and a degeneracy index that predicts them." pith.science (2026). https://pith.science/paper/ZSIGOGNS
@misc{pith2026260809203,
author = {Pith},
title = {Pith review of: Silent coverage failures in rare-event searches and a degeneracy index that predicts them},
year = {2026},
howpublished = {\url{https://pith.science/paper/ZSIGOGNS}},
note = {Machine review of arXiv:2608.09203}
}
abstract
Searches for new physics in low-background experiments infer a non-negative signal strength from few events and often report an upper limit. Nominal frequentist coverage requires both a valid interval construction and an adequate data model. We study how controlled model departures affect lower- and upper-endpoint coverage for six interval procedures in an exact Poisson counting experiment, dark-matter recoil spectra, and a neutrinoless-double-beta-decay peak search. We introduce the Poisson--Fisher degeneracy index $\mathcal I_{\mathrm{PF}}(\delta\nu;\vartheta_0)=(\beta,\gamma)$, which maps a specified expected-count deformation, after projection onto the complete fitted tangent space, to $\beta$, the signed fitted signal shift in profiled standard-error units, and $\gamma$, the Poisson--Fisher norm of the unabsorbed residual. Locally, the sign of $\beta$ identifies the threatened endpoint, while larger $\gamma$ implies greater detectability by the saturated-Poisson goodness-of-fit test used here at a fixed $5\%$ type-I error rate. Across the studied deformations, positive signal-like bias degrades discovery-side coverage while making upper limits conservative; negative signal bias from overestimated signal efficiency can make the upper endpoint undercover. Calibration under the nominal simulator does not protect against misspecification of that simulator relative to the data-generating process. A plausible deformation with large $|\beta|$ and small $\gamma$ may therefore evade diagnosis and should be represented by a nuisance constrained with auxiliary information or included in a defensible envelope. In the exactly collinear constrained-nuisance benchmark, modelling the deformation restores coverage at the evaluated grid points, at a quantifiable cost in interval sensitivity.
Reference graph
Works this paper leans on
-
[1]
LZ Collaboration, Aalbers, J.,et al.: Dark matter search results from 4.2 Tonne−Years of exposure of the lux-zeplin (lz) experiment. Phys. Rev. Lett. 135, 011802 (2025) https://doi.org/10.1103/4dyc-z8zf
-
[2]
XENON Collaboration, Aprile, E.,et al.: First dark matter search with nuclear recoils from the XENONnT experiment. Phys. Rev. Lett.131, 041003 (2023) https://doi.org/10.1103/PhysRevLett.131.041003 arXiv:2303.14729
arXiv 2023
-
[3]
SuperCDMS Collaboration, Agnese, R.,et al.: Results from the super cryogenic dark matter search experiment at Soudan. Phys. Rev. Lett.120, 061802 (2018) https://doi.org/10.1103/PhysRevLett.120.061802 arXiv:1708.08869
arXiv 2018
-
[4]
GERDA Collaboration, Agostini, M.,et al.: Final results of GERDA on the search for neutrinoless double-βdecay. Phys. Rev. Lett.125, 252502 (2020) https://doi. org/10.1103/PhysRevLett.125.252502 arXiv:2009.06079
arXiv 2020
-
[5]
Nature604, 53–58 (2022) https: //doi.org/10.1038/s41586-022-04497-4 arXiv:2104.06906
CUORE Collaboration, Adams, D.Q.,et al.: Search for Majorana neutrinos exploiting millikelvin cryogenics with CUORE. Nature604, 53–58 (2022) https: //doi.org/10.1038/s41586-022-04497-4 arXiv:2104.06906
arXiv 2022
-
[6]
KamLAND-Zen Collaboration, Abe, S.,et al.: Search for the Majorana nature of neutrinos in the inverted mass ordering region with KamLAND-Zen. Phys. Rev. Lett.130, 051801 (2023) https://doi.org/10.1103/PhysRevLett.130.051801 arXiv:2203.02139
arXiv 2023
-
[7]
Wilks, S.S.: The large-sample distribution of the likelihood ratio for testing com- posite hypotheses. Ann. Math. Stat.9(1), 60–62 (1938) https://doi.org/10.1214/ aoms/1177732360
arXiv 1938
-
[8]
Chernoff, H.: On the distribution of the likelihood ratio. Ann. Math. Stat.25(3), 573–578 (1954) https://doi.org/10.1214/aoms/1177728725
arXiv 1954
Show all 33 references
-
[9]
Cowan, G., Cranmer, K., Gross, E., Vitells, O.: Asymptotic formulae for likelihood-based tests of new physics. Eur. Phys. J. C71, 1554 (2011) https: //doi.org/10.1140/epjc/s10052-011-1554-0 arXiv:1007.1727. Erratum: Eur. Phys. J. C 73 (2013) 2501
2011 arXiv
-
[10]
Self, S.G., Liang, K.-Y.: Asymptotic properties of maximum likelihood estimators 21 and likelihood ratio tests under nonstandard conditions. J. Am. Stat. Assoc. 82(398), 605–610 (1987) https://doi.org/10.1080/01621459.1987.10478472
1987
-
[11]
Feldman, G.J., Cousins, R.D.: Unified approach to the classical statistical analysis of small signals. Phys. Rev. D57, 3873–3889 (1998) https://doi.org/10.1103/ PhysRevD.57.3873 arXiv:physics/9711021
1998 arXiv
-
[12]
Read, A.L.: Presentation of search results: the CL s technique. J. Phys. G: Nucl. Part. Phys.28, 2693–2704 (2002) https://doi.org/10.1088/0954-3899/28/10/313
2002 doi
-
[13]
Junk, T.: Confidence level computation for combining searches with small statis- tics. Nucl. Instrum. Meth. A434, 435–443 (1999) https://doi.org/10.1016/ S0168-9002(99)00498-2 arXiv:hep-ex/9902006
1999 arXiv
-
[14]
Cranmer, K., Brehmer, J., Louppe, G.: The frontier of simulation-based infer- ence. Proc. Natl. Acad. Sci. USA117(48), 30055–30062 (2020) https://doi.org/ 10.1073/pnas.1912789117 arXiv:1911.01429
2020 arXiv
-
[15]
In: Proceedings of the 37th International Conference on Machine Learning (ICML)
Dalmasso, N., Izbicki, R., Lee, A.B.: Confidence sets and hypothesis test- ing in a likelihood-free inference setting. In: Proceedings of the 37th International Conference on Machine Learning (ICML). Proceedings of Machine Learning Research, vol. 119, pp. 2323–2334. PMLR, Onli...
2020
-
[16]
In: Proceedings of the 26th Interna- tional Conference on Artificial Intelligence and Statistics (AISTATS)
Masserano, L., Dorigo, T., Izbicki, R., Kuusela, M., Lee, A.B.: Simulator-based inference with W ALDO: Confidence regions by leveraging prediction algorithms and posterior estimators for inverse problems. In: Proceedings of the 26th Interna- tional Conference on Artificial Int...
2023
-
[17]
Electron
Dalmasso, N., Masserano, L., Zhao, D., Izbicki, R., Lee, A.B.: Likelihood-free frequentist inference: bridging classical statistics and machine learning for reliable simulator-based inference. Electron. J. Stat.18(2), 5045–5090 (2024) https://doi. org/10.1214/24-EJS2307 arXiv:...
2024 arXiv
-
[18]
In: Proceedings of the 41st International Conference on Machine Learning
Patel, Y., McNamara, D., Loper, J., Regier, J., Tewari, A.: Variational infer- ence with coverage guarantees in simulation-based inference. In: Proceedings of the 41st International Conference on Machine Learning. Proceedings of Machine Learning Research, vol. 235, pp. 39861–3...
2024
-
[19]
Transactions on Machine Learning Research (TMLR) (2022) arXiv:2110.06581 22
Hermans, J., Delaunoy, A., Rozet, F., Wehenkel, A., Begy, V., Louppe, G.: A crisis in simulation-based inference? beware, your posterior approximations can be unfaithful. Transactions on Machine Learning Research (TMLR) (2022) arXiv:2110.06581 22
2022 arXiv
-
[20]
arXiv preprint (2022) arXiv:2209.01845
Cannon, P., Ward, D., Schmon, S.M.: Investigating the impact of model misspecification in neural simulation-based inference. arXiv preprint (2022) arXiv:2209.01845
2022 arXiv
-
[21]
In: Advances in Neural Information Processing Systems, vol
Ward, D., Cannon, P., Beaumont, M., Fasiolo, M., Schmon, S.M.: Robust neu- ral posterior estimation and statistical model criticism. In: Advances in Neural Information Processing Systems, vol. 35 (2022)
2022
-
[22]
Advances in Neural Information Processing Systems (NeurIPS)32(2019) arXiv:1904.06019
Tibshirani, R.J., Foygel Barber, R., Cand` es, E.J., Ramdas, A.: Conformal predic- tion under covariate shift. Advances in Neural Information Processing Systems (NeurIPS)32(2019) arXiv:1904.06019
2019 arXiv
-
[23]
Foygel Barber, R., Cand` es, E.J., Ramdas, A., Tibshirani, R.J.: Conformal predic- tion beyond exchangeability. Ann. Stat.51(2), 816–845 (2023) https://doi.org/ 10.1214/23-AOS2276 arXiv:2202.13415
2023 arXiv
-
[24]
Astropart
Lewin, J.D., Smith, P.F.: Review of mathematics, numerical factors, and correc- tions for dark matter experiments based on elastic nuclear recoil. Astropart. Phys. 6, 87–112 (1996) https://doi.org/10.1016/S0927-6505(96)00047-3
1996 doi
-
[25]
Green, A.M.: Astrophysical uncertainties on the local dark matter distribution and direct detection experiments. J. Phys. G: Nucl. Part. Phys.44(8), 084001 (2017) https://doi.org/10.1088/1361-6471/aa7819 arXiv:1703.10102
2017 arXiv
-
[26]
Lecture Notes in Statistics, vol
Amari, S.-i.: Differential-Geometrical Methods in Statistics. Lecture Notes in Statistics, vol. 28. Springer, New York (1985). https://doi.org/10.1007/ 978-1-4612-5056-2
1985
-
[27]
Cox, D.R., Reid, N.: Parameter orthogonality and approximate conditional infer- ence. J. R. Stat. Soc. B49(1), 1–39 (1987) https://doi.org/10.1111/j.2517-6161. 1987.tb01422.x
1987 doi
-
[28]
In: Proceedings of the Fifth Berkeley Symposium on Mathematical Statistics and Probability, vol
Huber, P.J.: The behavior of maximum likelihood estimates under nonstandard conditions. In: Proceedings of the Fifth Berkeley Symposium on Mathematical Statistics and Probability, vol. 1, pp. 221–233. University of California Press, Berkeley, CA (1967)
1967
-
[29]
Econometrica 50(1), 1–25 (1982) https://doi.org/10.2307/1912526
White, H.: Maximum likelihood estimation of misspecified models. Econometrica 50(1), 1–25 (1982) https://doi.org/10.2307/1912526
1982 doi
-
[30]
Biometrika69(1), 19–27 (1982) https://doi.org/10.1093/biomet/69.1.19
Kent, J.T.: Robust properties of likelihood ratio tests. Biometrika69(1), 19–27 (1982) https://doi.org/10.1093/biomet/69.1.19
1982 doi
-
[31]
Quantitative Economics13(3), 907–954 (2022) https://doi.org/10.3982/QE1930
Bonhomme, S., Weidner, M.: Minimizing sensitivity to model misspecification. Quantitative Economics13(3), 907–954 (2022) https://doi.org/10.3982/QE1930
2022 doi
-
[32]
ATLAS Collaboration, Aad, G.,et al.: Measurement of higgs boson production 23 in the diphoton decay channel inppcollisions at center-of-mass energies of 7 and 8 tev with the atlas detector. Phys. Rev. D90, 112015 (2014) https://doi.org/ 10.1103/PhysRevD.90.112015 arXiv:1408.7084
2014 arXiv
-
[33]
CMS Collaboration, Khachatryan, V.,et al.: Observation of the diphoton decay of the higgs boson and measurement of its properties. Eur. Phys. J. C74, 3076 (2014) https://doi.org/10.1140/epjc/s10052-014-3076-z arXiv:1407.0558 24
2014 arXiv
Reviewed August 11, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.