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Production of light and intermediate mass fragments using various clusterization algorithms

Nuclear Theory · Submitted 27 Sep 2010

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

The authors' main claim MSTB and MSTP identifies the free nucleons as early as possible.

how it is stated · asserted 1.00 read the record →

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arXiv ID1009.5200 (version 1)
Pith IDSTW4HY5B, Pith's permanent record of this paper and its review
CitationEkta, Rajeev K. Puri, Suneel Kumar. "Production of light and intermediate mass fragments using various clusterization algorithms." arXiv:1009.5200 (2010). https://pith.science/paper/STW4HY5B
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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,769 input tokens, $0.0002 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.68 · human participants 0.01 · controlled comparison 0.26 · randomized assignment 0.02 · states quantitative result 0.17 · compares with prior results 0.77 · mentions code or data availability 0.02.

The abstract, sentence by sentence

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

For the present analysis we simulate the reaction 129Xe 54+197Au79 at E=50 MeV/nucleon respectively[3]. This reaction is simulated at different impact parameters using hard equation of state. The stored phase space is then analyzed by using MST, MSTP and MSTB algorithms. MSTB and MSTP identifies the free nucleons as early as possible. In the two cases, a check in the form of binding energy and momentum cut helps to identify the fragments quite early. The normal MST takes quite a long time to identify the stable fragments which are residual of excited fragments.

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 For the present analysis we simulate the reaction 129Xe 54+197Au79 at E=50 MeV/nucleon respectively[3]. method 0.87 0.84 0.02 asserted 0.97
s1 This reaction is simulated at different impact parameters using hard equation of state. method 0.99 0.85 0.03 asserted 1.00
s2 The stored phase space is then analyzed by using MST, MSTP and MSTB algorithms. method 0.99 0.86 0.05 asserted 1.00
s3 MSTB and MSTP identifies the free nucleons as early as possible. result 0.97 0.81 0.17 asserted 1.00
s4 In the two cases, a check in the form of binding energy and momentum cut helps to identify the fragments quite early. method 0.69 0.76 0.12 asserted 0.99
s5 The normal MST takes quite a long time to identify the stable fragments which are residual of excited fragments. result 0.93 0.80 0.13 asserted 1.00

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

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

For the present analysis we simulate the reaction 129Xe 54+197Au79 at E=50 MeV/nucleon respectively[3]. This reaction is simulated at different impact parameters using hard equation of state. The stored phase space is then analyzed by using MST, MSTP and MSTB algorithms. MSTB and MSTP identifies the free nucleons as early as possible. In the two cases, a check in the form of binding energy and momentum cut helps to identify the fragments quite early. The normal MST takes quite a long time to identify the stable fragments which are residual of excited fragments.

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