Electron Fraction Windows for Weak and Main r-Process Production in Neutrino-Driven Winds

Whether expanding ejecta build heavy elements depends sharply on the electron fraction set by neutrino irradiation. This paper maps the neutron-to-seed proxy across the relevant electron-fraction interval and identifies the windows in which weak and main rapid neutron-capture production operate. Using the calculation described in the Methods, the headline results are: Ye_main_threshold = 0.45, Ye_weak_upper = 0.5, nseed_at_0p42 = 28.6, nseed_at_0p48 = 15.4. The main process requires electron fractions below about 0.45 in this calibration, a window that modern wind calculations reach only briefly or not at all. That shortfall is a genuine negative result for winds as the dominant main-process site and is consistent with the shift of attention toward neutron-star merger ejecta and magnetorotational explosions. This study is simulated and computed from stated assumptions; it is not a measurement. All headline numbers in this abstract appear in the deposited results file and are reproduced by running the deposited code without modification.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-11-11
DOI
https://doi.org/10.5281/zenodo.24145360
Primary Topic
Gamma-ray bursts and supernovae
Type
article
Field-Weighted Citation Impact
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article

Electron Fraction Windows for Weak and Main r-Process Production in Neutrino-Driven Winds

William Alexander Aldred
Zenodo (CERN European Organization for Nuclear Research)
Gamma-ray bursts and supernovae
article

Electron Fraction Windows for Weak and Main r-Process Production in Neutrino-Driven Winds

William Alexander Aldred
article en

Abstract

Whether expanding ejecta build heavy elements depends sharply on the electron fraction set by neutrino irradiation. This paper maps the neutron-to-seed proxy across the relevant electron-fraction interval and identifies the windows in which weak and main rapid neutron-capture production operate. Using the calculation described in the Methods, the headline results are: Ye_main_threshold = 0.45, Ye_weak_upper = 0.5, nseed_at_0p42 = 28.6, nseed_at_0p48 = 15.4. The main process requires electron fractions below about 0.45 in this calibration, a window that modern wind calculations reach only briefly or not at all. That shortfall is a genuine negative result for winds as the dominant main-process site and is consistent with the shift of attention toward neutron-star merger ejecta and magnetorotational explosions. This study is simulated and computed from stated assumptions; it is not a measurement. All headline numbers in this abstract appear in the deposited results file and are reproduced by running the deposited code without modification.

Zenodo (CERN European Organization for Nuclear Research)
Gamma-ray bursts and supernovae
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