Estimation of the effect of Tsallis non-extensive statistics on the 14C(n,γ)15C reaction rate

The total cross-section of the radiative neutron capture reaction 14 С( n ,γ 0+1 ) 15 C—for energies ranging from 10 meV to 5 MeV—is considered. Calculations performed in the framework of the modified potential cluster model with forbidden states show an agreement of total cross-section σ (23.3 keV) = 4.75 μb with the presently recommended value 4.86(48) μb by Ma et al., 2020. The efficiency of carbon isotope 15 C production is illustrated by the 14 С( n ,γ 0+1 ) 15 C reaction rate calculated at temperatures from T 9 = 0.001 to T 9 = 10. The conventional Maxwell–Boltzmann weighted reaction rate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="m1"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mfenced open="〈" close="〉" separators="|"> <mml:mrow> <mml:mi>σ</mml:mi> <mml:mi>v</mml:mi> </mml:mrow> </mml:mfenced> </mml:mrow> <mml:mtext>MB</mml:mtext> </mml:msub> </mml:mrow> </mml:math> of the present work is comparable, with less than 10% accuracy, with the latest calculations by Ma et al., 2020 and Bhattacharyya et al., 2021. The estimation of non-extensive effects is implemented using our data on the reaction rate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="m2"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mfenced open="〈" close="〉" separators="|"> <mml:mrow> <mml:mi>σ</mml:mi> <mml:mi>v</mml:mi> </mml:mrow> </mml:mfenced> </mml:mrow> <mml:mtext>MB</mml:mtext> </mml:msub> </mml:mrow> </mml:math> as reference values. The efficiency of carbon isotope production in radiative capture reactions 12-14 С( n ,γ) 13-15 C is estimated based on the calculated reaction rates. The influence of the Maxwellian-weighted 12-14 C( n ,γ) 13-15 C reaction rates on the ratios 12 C/ 13 C and 13 C/ 14 C is examined. Tsallis statistics is applied for the first time to the calculation of the 14 С( n ,γ 0 ) 15 C reaction rate with values of non-extensive parameter 0.7 ≤ q ≤ 1.3 on the background of Maxwell–Boltzmann statistics corresponding to q = 1. The reaction rate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="m3"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mfenced open="〈" close="〉" separators="|"> <mml:mrow> <mml:mi>σ</mml:mi> <mml:mi>v</mml:mi> </mml:mrow> </mml:mfenced> </mml:mrow> <mml:mi>q</mml:mi> </mml:msub> </mml:mrow> </mml:math> shows a factor ∼4 increase for q = 0.7 and a factor ∼0.6 decrease for q = 1.3 compared to q = 1.

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Journal
Frontiers in Physics
Published
2025-11-25
DOI
https://doi.org/10.3389/fphy.2025.1688864
Primary Topic
Nuclear physics research studies
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article

Estimation of the effect of Tsallis non-extensive statistics on the 14C(n,γ)15C reaction rate

N. A. Burkova, A. S. Tkachenko, B. M. Yeleusheva, S. B. Dubovichenko
Frontiers in Physics
Nuclear physics research studies
article

Estimation of the effect of Tsallis non-extensive statistics on the 14C(n,γ)15C reaction rate

N. A. Burkova, A. S. Tkachenko, B. M. Yeleusheva, S. B. Dubovichenko
article en

Abstract

The total cross-section of the radiative neutron capture reaction 14 С( n ,γ 0+1 ) 15 C—for energies ranging from 10 meV to 5 MeV—is considered. Calculations performed in the framework of the modified potential cluster model with forbidden states show an agreement of total cross-section σ (23.3 keV) = 4.75 μb with the presently recommended value 4.86(48) μb by Ma et al., 2020. The efficiency of carbon isotope 15 C production is illustrated by the 14 С( n ,γ 0+1 ) 15 C reaction rate calculated at temperatures from T 9 = 0.001 to T 9 = 10. The conventional Maxwell–Boltzmann weighted reaction rate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="m1"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mfenced open="〈" close="〉" separators="|"> <mml:mrow> <mml:mi>σ</mml:mi> <mml:mi>v</mml:mi> </mml:mrow> </mml:mfenced> </mml:mrow> <mml:mtext>MB</mml:mtext> </mml:msub> </mml:mrow> </mml:math> of the present work is comparable, with less than 10% accuracy, with the latest calculations by Ma et al., 2020 and Bhattacharyya et al., 2021. The estimation of non-extensive effects is implemented using our data on the reaction rate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="m2"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mfenced open="〈" close="〉" separators="|"> <mml:mrow> <mml:mi>σ</mml:mi> <mml:mi>v</mml:mi> </mml:mrow> </mml:mfenced> </mml:mrow> <mml:mtext>MB</mml:mtext> </mml:msub> </mml:mrow> </mml:math> as reference values. The efficiency of carbon isotope production in radiative capture reactions 12-14 С( n ,γ) 13-15 C is estimated based on the calculated reaction rates. The influence of the Maxwellian-weighted 12-14 C( n ,γ) 13-15 C reaction rates on the ratios 12 C/ 13 C and 13 C/ 14 C is examined. Tsallis statistics is applied for the first time to the calculation of the 14 С( n ,γ 0 ) 15 C reaction rate with values of non-extensive parameter 0.7 ≤ q ≤ 1.3 on the background of Maxwell–Boltzmann statistics corresponding to q = 1. The reaction rate <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" id="m3"> <mml:mrow> <mml:msub> <mml:mrow> <mml:mfenced open="〈" close="〉" separators="|"> <mml:mrow> <mml:mi>σ</mml:mi> <mml:mi>v</mml:mi> </mml:mrow> </mml:mfenced> </mml:mrow> <mml:mi>q</mml:mi> </mml:msub> </mml:mrow> </mml:math> shows a factor ∼4 increase for q = 0.7 and a factor ∼0.6 decrease for q = 1.3 compared to q = 1.

Frontiers in PhysicsVol. 13
Al-Farabi Kazakh National University (KZ), Almaty Technological University (KZ)
Openalex Percentile: Top 84%
Nuclear physics research studies
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