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Old Data, New Forensics: The First Second of SN 1987A Neutrino Emission

High Energy Astrophysical Phenomena · Submitted 13 Jun 2023

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

The authors' main claim However, even considering the low neutrino counts, the models generally disagree with data. What can cause this?

how it is stated · asserted 0.98 read the record →

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arXiv ID2306.08024 (version 2)
Pith IDUR6M3YYM, Pith's permanent record of this paper and its review
CitationFrancesco Capozzi, John F. Beacom, Luke F. Roberts, Shirley Weishi Li. "Old Data, New Forensics: The First Second of SN 1987A Neutrino Emission." arXiv:2306.08024 (2023). https://pith.science/paper/UR6M3YYM
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 5,497 input tokens.

What the abstract itself states, as probabilities: claims first 0.88 · states limitation 0.57 · human participants 0.02 · controlled comparison 0.23 · randomized assignment 0.01 · states quantitative result 0.30 · compares with prior results 0.85 · mentions code or data availability 0.03.

The abstract, sentence by sentence

arXiv listing abstract v2. Results and the main claim are underlined; .

The next Milky Way supernova will be an epochal event in multi-messenger astronomy, critical to tests of supernovae, neutrinos, and new physics. Realizing this potential depends on having realistic simulations of core collapse. We investigate the neutrino predictions of nearly all modern models (1-, 2-, and 3-d) over the first $\simeq$1 s, making the first detailed comparisons of these models to each other and to the SN 1987A neutrino data. Even with different methods and inputs, the models generally agree with each other. However, even considering the low neutrino counts, the models generally disagree with data. What can cause this? We show that neither neutrino oscillations nor different progenitor masses appear to be a sufficient solution. We outline urgently needed work.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 The next Milky Way supernova will be an epochal event in multi-messenger astronomy, critical to tests of supernovae, neutrinos, and new physics. background 1.00 0.05 0.03 asserted 0.99
s1 Realizing this potential depends on having realistic simulations of core collapse. background 0.84 0.05 0.02 asserted 0.99
s2 We investigate the neutrino predictions of nearly all modern models (1-, 2-, and 3-d) over the first $\simeq$1 s, making the first detailed comparisons of these models to each other and to the SN 1987A neutrino data. contribution 0.98 0.94 0.07 asserted 0.98
s3 Even with different methods and inputs, the models generally agree with each other. result 1.00 0.74 0.10 asserted 0.97
s4 However, even considering the low neutrino counts, the models generally disagree with data. What can cause this? result 0.92 0.70 0.34 asserted 0.98
s5 We show that neither neutrino oscillations nor different progenitor masses appear to be a sufficient solution. result 0.97 0.89 0.38 asserted 0.90
s6 We outline urgently needed work. future work 1.00 0.62 0.10 unclear 0.55

What kind of paper the classifier reports this is: simulation study 0.88 · evidence from simulation or computation 0.69.

What was examined, and what was not

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

The next Milky Way supernova will be an epochal event in multi-messenger astronomy, critical to tests of supernovae, neutrinos, and new physics. Realizing this potential depends on having realistic simulations of core collapse. We investigate the neutrino predictions of nearly all modern models (1-, 2-, and 3-d) over the first $\simeq$1 s, making the first detailed comparisons of these models to each other and to the SN 1987A neutrino data. Even with different methods and inputs, the models generally agree with each other. However, even considering the low neutrino counts, the models generally disagree with data. What can cause this? We show that neither neutrino oscillations nor different progenitor masses appear to be a sufficient solution. We outline urgently needed work.

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References
How the literature uses it

14 arXiv papers cite this in 34 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 citing it · 28 sentences without a confident label

Contests it 1 paper
  • Instead, in Ref. [ref] the number of events and their energies were separately tested, which means, among other issues, that the event energies of a SN model for the first 1.5 s were compared with data within an 0.5 s period.

    Supernova Simulations Confront SN 1987A Neutrinos · First second of emission · contest 0.86

Uses its method or tool 1 paper
Compares with it 1 paper
Cites it as background 2 papers

What it cites · 102 sentences without a confident label

Contests 5 papers
Uses the method or tool of 9 papers
Uses data or values from 10 papers
Compares with 1 paper
  • For the five luminosity profiles from Ref. [ref] , as shown in Fig. [ref], two are significantly lower than ours at all times, making them closer to the Kam-II data.

    Supernova Simulations Confront SN 1987A Neutrinos · Model selection compared to Fiorillo et al. (2023) · 0.95

Cites as support 3 papers
Cites as background 4 papers
  • In core-collapse supernovae [ref] , the white-dwarf-like iron core of a massive star collapses to form a proto-neutron star (PNS), releasing nearly all of the gravitational binding energy difference, $E_tot ≃(3/5) G M_PNS^2/R_PNS ≃3 ×10^53 erg$, in neutrinos of all flavors with comparable fluences.

    Explosion Mechanisms of Core-Collapse Supernovae · Review of Supernova Models · 1.00

  • In core-collapse supernovae [ref] , the white-dwarf-like iron core of a massive star collapses to form a proto-neutron star (PNS), releasing nearly all of the gravitational binding energy difference, $E_tot ≃(3/5) G M_PNS^2/R_PNS ≃3 ×10^53 erg$, in neutrinos of all flavors with comparable fluences.

    Progenitors of core-collapse supernovae · Review of Supernova Models · 1.00

  • In core-collapse supernovae [ref] , the white-dwarf-like iron core of a massive star collapses to form a proto-neutron star (PNS), releasing nearly all of the gravitational binding energy difference, $E_tot ≃(3/5) G M_PNS^2/R_PNS ≃3 ×10^53 erg$, in neutrinos of all flavors with comparable fluences.

    Core-Collapse Supernova Explosion Theory · Review of Supernova Models · 1.00

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