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Measurement of sub threshold resonance contributions to fusion reactions: the case of the 13C(α, n)16O astrophysical neutron source

EPJ Web of Conferences, 2015, Vol.86, p.00023

2015

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TexAT detector upgrade for 14O(α,p)17F cross section measurement

Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms, 2023-08, Vol.541 (C), p.221-223

2023

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Measurement of the − 3 keV Resonance in the Reaction C 13 ( α , n ) O 16 of Importance in the s -Process

Physical review letters, 2012-12, Vol.109 (23), Article 232701

2012

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Direct fusion measurement of the 8B proton-halo nucleus at near-barrier energies

Physics letters. B, 2021-05, Vol.816 (C)

2021

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Texas Active Target (TexAT) detector for experiments with rare isotope beams

Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 2020-01, Vol.957 (C)

2020

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Sub-Coulomb He 3 transfer and its use to extract three-particle asymptotic normalization coefficients

Physical review. C, 2018-01, Vol.97 (1), Article 014313

2018

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ANASEN: The array for nuclear astrophysics and structure with exotic nuclei

Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 2017-10, Vol.870 (C), p.1-11

2017

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Sub-Coulomb He3 transfer and its use to extract three-particle asymptotic normalization coefficients

Physical review. C, 2018-01, Vol.97 (1)

2018

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Erratum: Measurement of d + Be 7 Cross Sections for Big-Bang Nucleosynthesis [Phys. Rev. Lett. 122 , 182701 (2019)]

Physical review letters, 2019-12, Vol.123 (23), Article 239902

2019

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Beta-delayed charged-particle spectroscopy using TexAT

Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 2020-03, Vol.964

2020

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Structure of 10 N in 9 C+p resonance scattering

Physics letters. B, 2017-03, Vol.769 (C)

2017

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Modular next generation fast-neutron detector for portal monitoring

Nuclear science and techniques, 2022, Vol.33 (1), p.140-148, Article 13

2022

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Nuclear structure beyond the neutron drip line: The lowest energy states in 9 He via their T = 5/2 isobaric analogs in 9 Li

Physics letters. B, 2016-03, Vol.754, p.323-327

2016

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Barrier height distributions – the inﬂuence of weak channels

EPJ Web of conferences, 2011-01, Vol.17, p.5006

2011

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First Observation of the β3αp Decay of ^{13}O via β-Delayed Charged-Particle Spectroscopy

Physical review letters, 2023-06, Vol.130 (22), p.222501-222501

2023

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Constraining the 6.05 MeV 0+ and 6.13 MeV 3- Cascade Transitions in the C12(a,y)016 Reaction Using the Asymptotic Normalization Coefficients

Physical review letters, 2015-02, Vol.114 (7)

2015

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Erratum: Measurement of d+^{7}Be Cross Sections for Big-Bang Nucleosynthesis [Phys. Rev. Lett. 122, 182701 (2019)]

Physical review letters, 2019-12, Vol.123 (23), p.239902-239902

2019

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Measurement of d+^{7}Be Cross Sections for Big-Bang Nucleosynthesis

Physical review letters, 2019-05, Vol.122 (18), p.182701-182701

2019

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ON THE MEASUREMENT OF THE super(13)C( alpha , n) super(16)O S-FACTOR AT NEGATIVE ENERGIES AND ITS INFLUENCE ON THE s-PROCESS

The Astrophysical journal, 2013-11, Vol.777 (2), p.1-21

2013

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ON THE MEASUREMENT OF THE 13 C(α, n ) 16 O S -FACTOR AT NEGATIVE ENERGIES AND ITS INFLUENCE ON THE s -PROCESS

The Astrophysical journal, 2013-10, Vol.777 (2), p.143

2013

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Reaction rate of the 13C(α,n)16O neutron source using the ANC of the -3 keV resonance measured with the THM

Journal of physics. Conference series, 2016-01, Vol.665 (1)

2016

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Reaction rate of the 13 C( α,n ) 16 O neutron source using the ANC of the -3 keV resonance measured with the THM

Journal of physics. Conference series, 2016-01, Vol.665, p.12013

2016

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Clustering in non-self-conjugate nuclei 10 Be and 18 O

Journal of physics. Conference series, 2014-12, Vol.569, p.12004

2014

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Clustering in non-self-conjugate nuclei 10Be and 18O

Journal of physics. Conference series, 2014-12, Vol.569 (1)

2014

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Clustering in non-self-conjugate nuclei super(10)Be and super(18)O

Journal of physics. Conference series, 2014-01, Vol.569, p.1-7

2014

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Measurement of sub threshold resonance contributions to fusion reactions: the case of the 13C(α, n)16O astrophysical neutron source

TexAT detector upgrade for 14O(α,p)17F cross section measurement

Measurement of the − 3 keV Resonance in the Reaction C 13 ( α , n ) O 16 of Importance in the s -Process

Direct fusion measurement of the 8B proton-halo nucleus at near-barrier energies

Texas Active Target (TexAT) detector for experiments with rare isotope beams

Sub-Coulomb He 3 transfer and its use to extract three-particle asymptotic normalization coefficients

ANASEN: The array for nuclear astrophysics and structure with exotic nuclei

Sub-Coulomb He3 transfer and its use to extract three-particle asymptotic normalization coefficients

Erratum: Measurement of d + Be 7 Cross Sections for Big-Bang Nucleosynthesis [Phys. Rev. Lett. 122 , 182701 (2019)]

Beta-delayed charged-particle spectroscopy using TexAT

Structure of 10 N in 9 C+p resonance scattering

Modular next generation fast-neutron detector for portal monitoring

Nuclear structure beyond the neutron drip line: The lowest energy states in 9 He via their T = 5/2 isobaric analogs in 9 Li

Barrier height distributions – the inﬂuence of weak channels

First Observation of the β3αp Decay of ^{13}O via β-Delayed Charged-Particle Spectroscopy

Constraining the 6.05 MeV 0+ and 6.13 MeV 3- Cascade Transitions in the C12(a,y)016 Reaction Using the Asymptotic Normalization Coefficients

Erratum: Measurement of d+^{7}Be Cross Sections for Big-Bang Nucleosynthesis [Phys. Rev. Lett. 122, 182701 (2019)]

Measurement of d+^{7}Be Cross Sections for Big-Bang Nucleosynthesis

ON THE MEASUREMENT OF THE super(13)C( alpha , n) super(16)O S-FACTOR AT NEGATIVE ENERGIES AND ITS INFLUENCE ON THE s-PROCESS

ON THE MEASUREMENT OF THE 13 C(α, n ) 16 O S -FACTOR AT NEGATIVE ENERGIES AND ITS INFLUENCE ON THE s -PROCESS

Reaction rate of the 13C(α,n)16O neutron source using the ANC of the -3 keV resonance measured with the THM

Reaction rate of the 13 C( α,n ) 16 O neutron source using the ANC of the -3 keV resonance measured with the THM

Clustering in non-self-conjugate nuclei 10 Be and 18 O

Clustering in non-self-conjugate nuclei 10Be and 18O

Clustering in non-self-conjugate nuclei super(10)Be and super(18)O

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