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Gray Models of convection in core collapse supernovae

Astrophysics · Submitted 24 May 1998

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

The authors' main claim By considering a series of models where the LTE/NLTE decoupling point is varied we show that the outcome of the numerical models is critically sensitive to the choice of the decoupling point when the gray approximation is employed.

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arXiv IDastro-ph/9805303 (version 1)
Pith IDIVDPIAQJ, Pith's permanent record of this paper and its review
CitationF. Douglas Swesty. "Gray Models of convection in core collapse supernovae." arXiv:astro-ph/9805303 (1998). https://pith.science/paper/IVDPIAQJ
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The compiled record

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-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 8,145 input tokens, $0.0003 reported.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.72 · human participants 0.01 · controlled comparison 0.24 · randomized assignment 0.01 · states quantitative result 0.05 · compares with prior results 0.96 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

One of the major difficulties encountered in modeling core collapse supernovae is obtaining an accurate description of the transport of neutrinos through the collapsed stellar core. The behavior of the neutrino distribution function transitions from an LTE distribution in the center of the core to a non-LTE distribution in the outer regions of the core. One method that has been recently employed in order to model the flow of neutrinos in 2-D models is the gray approximation. This approximation assumes that the neutrino distribution can be described by a function that is parameterized in terms of a neutrino temperature and a neutrino chemical potential. However, these parameters must be assumed. Furthermore, the parameters will also differ between the LTE and NLTE regions. Additionally, within the gray approximation the location at which the neutrino distribution function transitions from LTE to NLTE must be assumed. By considering a series of models where the LTE/NLTE decoupling point is varied we show that the outcome of the numerical models is critically sensitive to the choice of the decoupling point when the gray approximation is employed. We also examine the effects of the neutrino--electron scattering (NES) rate which is difficult to correctly formulate within the gray approximation. We show that NES has a dramatic affect on the the overall neutrino heating rate and the dynamics of the model. This result conflicts with the results of high resolution multi-group models which model neutrino transport without employing the gray approximation.

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 One of the major difficulties encountered in modeling core collapse supernovae is obtaining an accurate description of the transport of neutrinos through the collapsed stellar core. background 0.99 0.06 0.02 asserted 1.00
s1 The behavior of the neutrino distribution function transitions from an LTE distribution in the center of the core to a non-LTE distribution in the outer regions of the core. background 1.00 0.13 0.02 asserted 1.00
s2 One method that has been recently employed in order to model the flow of neutrinos in 2-D models is the gray approximation. background 0.79 0.06 0.02 asserted 0.98
s3 This approximation assumes that the neutrino distribution can be described by a function that is parameterized in terms of a neutrino temperature and a neutrino chemical potential. background 0.54 0.07 0.02 asserted 0.99
s4 However, these parameters must be assumed. limitation 0.72 0.06 0.02 asserted 1.00
s5 Furthermore, the parameters will also differ between the LTE and NLTE regions. limitation 0.61 0.10 0.02 asserted 0.99
s6 Additionally, within the gray approximation the location at which the neutrino distribution function transitions from LTE to NLTE must be assumed. limitation 0.65 0.07 0.04 asserted 1.00
s7 By considering a series of models where the LTE/NLTE decoupling point is varied we show that the outcome of the numerical models is critically sensitive to the choice of the decoupling point when the gray approximation is employed. result 0.97 0.96 0.59 asserted 1.00
s8 We also examine the effects of the neutrino--electron scattering (NES) rate which is difficult to correctly formulate within the gray approximation. contribution 0.84 0.67 0.04 asserted 0.97
s9 We show that NES has a dramatic affect on the the overall neutrino heating rate and the dynamics of the model. result 1.00 0.94 0.30 asserted 1.00
s10 This result conflicts with the results of high resolution multi-group models which model neutrino transport without employing the gray approximation. interpretation 0.49 0.60 0.26 asserted 1.00

What kind of paper the classifier reports this is: simulation study 1.00 · evidence from simulation or computation 1.00.

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not examined
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  • references and citing sentences
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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

One of the major difficulties encountered in modeling core collapse supernovae is obtaining an accurate description of the transport of neutrinos through the collapsed stellar core. The behavior of the neutrino distribution function transitions from an LTE distribution in the center of the core to a non-LTE distribution in the outer regions of the core. One method that has been recently employed in order to model the flow of neutrinos in 2-D models is the gray approximation. This approximation assumes that the neutrino distribution can be described by a function that is parameterized in terms of a neutrino temperature and a neutrino chemical potential. However, these parameters must be assumed. Furthermore, the parameters will also differ between the LTE and NLTE regions. Additionally, within the gray approximation the location at which the neutrino distribution function transitions from LTE to NLTE must be assumed. By considering a series of models where the LTE/NLTE decoupling point is varied we show that the outcome of the numerical models is critically sensitive to the choice of the decoupling point when the gray approximation is employed. We also examine the effects of the neutrino--electron scattering (NES) rate which is difficult to correctly formulate within the gray approximation. We show that NES has a dramatic affect on the the overall neutrino heating rate and the dynamics of the model. This result conflicts with the results of high resolution multi-group models which model neutrino transport without employing the gray approximation.

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