William A. Peters
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Research Interests
William A. Peters has a total of 376 co-authors. Here are the top co-authors by number of shared publications:
T. Baumann
National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
19 shared publicationsM. Thoennessen
National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
17 shared publicationsN. Frank
Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA
17 shared publicationsD. Bazin
National Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824, USA
15 shared publicationsA. Schiller
Department of Physics & Astronomy, Ohio University, Athens, Ohio 45701, USA
13 shared publications- Kyungyuk Y. Chae
Sungkyunkwan University
13 shared publications
Latest Publications
- Open Access
- 1 August 2019
- Published by IOP Publishing in Journal of Physics: Conference Series
- Vol. 1308 (1) , 012004
Particle decay of astrophysically-important 19Ne levels
The 15O(α,γ)19Ne reaction is an important trigger reaction leading to the rapid proton (rp) capture process in X-ray bursts. The primary uncertainty in determining its astrophysical rate is the uncertain α branching ratios of levels near Ex = 4.1 MeV in 19Ne. These states have been populated in a study of the 20Ne(p, d)19Ne reaction, and α branching ratios are reported in this manuscript.
- 1 August 2019
- Published by IOP Publishing in Journal of Physics: Conference Series
- Vol. 1308 (1) , 012004
Open AccessParticle decay of astrophysically-important 19Ne levels
The 15O(α,γ)19Ne reaction is an important trigger reaction leading to the rapid proton (rp) capture process in X-ray bursts. The primary uncertainty in determining its astrophysical rate is the uncertain α branching ratios of levels near Ex = 4.1 MeV in 19Ne. These states have been populated in a study of the 20Ne(p, d)19Ne reaction, and α branching ratios are reported in this manuscript.
- 1 March 2019
- Published by Elsevier in Journal of Medical Imaging and Radiation Sciences
- Vol. 50 (1) , S12-S13
High-Purity Actinium-225 Production from Radium-226 using a Superconducting Electron Linac
- 1 March 2019
- Published by Elsevier in Journal of Medical Imaging and Radiation Sciences
- Vol. 50 (1) , S12-S13
High-Purity Actinium-225 Production from Radium-226 using a Superconducting Electron Linac
- 22 February 2018
- Published by Elsevier
Contributors
- Open Access
- 7 August 2017
- Published by American Physical Society (APS) in Physical Review C
- Vol. 96 (2) , 029801
Comment on “Cross section of the reaction: A background for the measurement of geo-neutrinos”Harissopulos et al. [ Phys. Rev. C 72, 062801(R) (2005)] report a cross section from a measurement that used a moderated neutron detector not capable of measuring the neutron energy and therefore unable to determine the relative contribution from neutrons that populate the ground state or excited states in reactions above 5 MeV. Since the energies of ejected neutrons populating the excited states are 6 MeV lower than those populating the ground state, the corresponding efficiency of their neutron detector for these neutrons was a factor of 2 higher than assumed. Therefore, the reported cross sections above 5 MeV may be overcalculated by nearly 50%.- 7 August 2017
- Published by American Physical Society (APS) in Physical Review C
- Vol. 96 (2) , 029801
Open AccessComment on “Cross section of the reaction: A background for the measurement of geo-neutrinos”Harissopulos et al. [ Phys. Rev. C 72, 062801(R) (2005)] report a cross section from a measurement that used a moderated neutron detector not capable of measuring the neutron energy and therefore unable to determine the relative contribution from neutrons that populate the ground state or excited states in reactions above 5 MeV. Since the energies of ejected neutrons populating the excited states are 6 MeV lower than those populating the ground state, the corresponding efficiency of their neutron detector for these neutrons was a factor of 2 higher than assumed. Therefore, the reported cross sections above 5 MeV may be overcalculated by nearly 50%. - 20 May 2015
- Published by American Society of Clinical Oncology (ASCO) in Journal of Clinical Oncology
- Vol. 33 (15_suppl) , 5573
A phase Ib/II trial with expansion of patients at the MTD trial of olaparib plus weekly (metronomic) carboplatin and paclitaxel in relapsed ovarian cancer patients.
5573 Background: We established the olaparib tablet maximum tolerated dose, dose limiting toxicities (DLT’s) and response to therapy of carboplatin, paclitaxel and olaparib tablet given simultaneously, reported at ASCO 2014. This abstract will include data from both the phase 1b and the phase 2 expansion. Methods: A total of 54 subjects were evaluated in this trial, 14 in phase 1b and 40 in phase 2. Eligibility required measurable disease, adequate organ function and ECOG performance status of ≤ 2. Subjects had to have failed first line platinum containing chemotherapy. BRCA testing was conducted as available. Subjects received the metronomic therapy of paclitaxel 60mg/m2 IV and carboplatin AUC 2 IV weekly, 3 weeks out of 4, and olaparib tablets at the MTD of 150 mg bid administered orally for 3 consecutive days (D1-D3), every week for each cycle. Subjects were assessed for toxicity and response according to the protocol. Subjects that reached a confirmed complete remission were transitioned to olaparib t...
- 20 May 2015
- Published by American Society of Clinical Oncology (ASCO) in Journal of Clinical Oncology
- Vol. 33 (15_suppl) , 5573
A phase Ib/II trial with expansion of patients at the MTD trial of olaparib plus weekly (metronomic) carboplatin and paclitaxel in relapsed ovarian cancer patients.
5573 Background: We established the olaparib tablet maximum tolerated dose, dose limiting toxicities (DLT’s) and response to therapy of carboplatin, paclitaxel and olaparib tablet given simultaneously, reported at ASCO 2014. This abstract will include data from both the phase 1b and the phase 2 expansion. Methods: A total of 54 subjects were evaluated in this trial, 14 in phase 1b and 40 in phase 2. Eligibility required measurable disease, adequate organ function and ECOG performance status of ≤ 2. Subjects had to have failed first line platinum containing chemotherapy. BRCA testing was conducted as available. Subjects received the metronomic therapy of paclitaxel 60mg/m2 IV and carboplatin AUC 2 IV weekly, 3 weeks out of 4, and olaparib tablets at the MTD of 150 mg bid administered orally for 3 consecutive days (D1-D3), every week for each cycle. Subjects were assessed for toxicity and response according to the protocol. Subjects that reached a confirmed complete remission were transitioned to olaparib t...
- 1 October 2013
- Published by Office of Scientific and Technical Information (OSTI)
Annual Report FY2013-- A Kinematically Complete, Interdisciplinary, and Co-Institutional Measurement of the 19F(α,n) Cross-section for Nuclear Safeguards Science
The goal of this proposal is to enable neutron detection for precision Non-Destructive Assays (NDAs) of actinide-fluoride samples. Neutrons are continuously generated from a UFx matrix in a container or sample as a result of the interaction of alpha particles from uranium-decay α particles with fluorine nuclei in the matrix. Neutrons from 19F(α,n)22Na were once considered a poorly characterized background for assays of UFx samples via 238U spontaneous fission neutron detection [SMI2010B]. However, the yield of decay-α-driven neutrons is critical for 234,235U LEU and HEU assays, as it can used to determine both the total amount of uranium and the enrichment [BER2010]. This approach can be extremely valuable in a variety of safeguard applications, such as cylinder monitoring in underground uranium storage facilities, nuclear criticality safety studies, nuclear materials accounting, and other nonproliferation applications. The success of neutron-based assays critically depends on an accurate knowledge of the cross section of the (α,n) reaction that generates the neutrons. The 40% uncertainty in the 19F(α,n)22Na cross section currently limits the precision of such assays, and has been identified as a key factor in preventing accurate enrichment determinations [CRO2003]. The need for higher quality cross section data for (α,n) reactions has been amore » recurring conclusion in reviews of the nuclear data needs to support safeguards. The overarching goal of this project is to enable neutron detection to be used for precision Non- Destructive Assays (NDAs) of actinide-fluoride samples. This will significantly advance safeguards verification at existing declared facilities, nuclear materials accounting, process control, nuclear criticality safety monitoring, and a variety of other nonproliferation applications. To reach this goal, Idaho National Laboratory (INL), in partnership with Oak Ridge National Laboratory (ORNL), Rutgers University (RU), and the University of Notre Dame (UND), will focus on three specific items: (1) making a precision (better than 10 %) determination of the absolute cross section of the 19F(α,n)22Na reaction as a function of energy; (2) determining the spectrum of neutrons and γ-rays emitted from 19F(α,n)22Na over an energy range pertinent to NDA; and (3) performing simulations with this new cross section to extract the neutron yield (neutrons/gram/second) and resulting neutron- and gamma ray-spectra when α particles interact with fluorine nuclei in actinide samples, to aid in the design and reduce uncertainty of future NDA measurements and simulations.« less
- 1 October 2013
- Published by Office of Scientific and Technical Information (OSTI)
Annual Report FY2013-- A Kinematically Complete, Interdisciplinary, and Co-Institutional Measurement of the 19F(α,n) Cross-section for Nuclear Safeguards Science
The goal of this proposal is to enable neutron detection for precision Non-Destructive Assays (NDAs) of actinide-fluoride samples. Neutrons are continuously generated from a UFx matrix in a container or sample as a result of the interaction of alpha particles from uranium-decay α particles with fluorine nuclei in the matrix. Neutrons from 19F(α,n)22Na were once considered a poorly characterized background for assays of UFx samples via 238U spontaneous fission neutron detection [SMI2010B]. However, the yield of decay-α-driven neutrons is critical for 234,235U LEU and HEU assays, as it can used to determine both the total amount of uranium and the enrichment [BER2010]. This approach can be extremely valuable in a variety of safeguard applications, such as cylinder monitoring in underground uranium storage facilities, nuclear criticality safety studies, nuclear materials accounting, and other nonproliferation applications. The success of neutron-based assays critically depends on an accurate knowledge of the cross section of the (α,n) reaction that generates the neutrons. The 40% uncertainty in the 19F(α,n)22Na cross section currently limits the precision of such assays, and has been identified as a key factor in preventing accurate enrichment determinations [CRO2003]. The need for higher quality cross section data for (α,n) reactions has been amore » recurring conclusion in reviews of the nuclear data needs to support safeguards. The overarching goal of this project is to enable neutron detection to be used for precision Non- Destructive Assays (NDAs) of actinide-fluoride samples. This will significantly advance safeguards verification at existing declared facilities, nuclear materials accounting, process control, nuclear criticality safety monitoring, and a variety of other nonproliferation applications. To reach this goal, Idaho National Laboratory (INL), in partnership with Oak Ridge National Laboratory (ORNL), Rutgers University (RU), and the University of Notre Dame (UND), will focus on three specific items: (1) making a precision (better than 10 %) determination of the absolute cross section of the 19F(α,n)22Na reaction as a function of energy; (2) determining the spectrum of neutrons and γ-rays emitted from 19F(α,n)22Na over an energy range pertinent to NDA; and (3) performing simulations with this new cross section to extract the neutron yield (neutrons/gram/second) and resulting neutron- and gamma ray-spectra when α particles interact with fluorine nuclei in actinide samples, to aid in the design and reduce uncertainty of future NDA measurements and simulations.« less
- 6 July 2012
- Published by American Physical Society (APS) in Physical Review C
- Vol. 86 (1) , 019802
Reply to “Comment on ‘Neutron knockout of12Bepopulating neutron-unbound states in11Be’ ”
In the preceding Comment, Fortune argues that, in our original paper [Peters et al., Phys. Rev. C 83, 057304 (2011)], we did not or could not separate the two neutron-unbound states in near 4 MeV. However, including the suggested contribution of the 3.887-MeV state decaying via 18 keV to the state in does not fit the data; neither do any other attempts incorporating any contribution of this decay channel. The best fit was achieved with a single resonance of decay energy 80(2) keV.- 6 July 2012
- Published by American Physical Society (APS) in Physical Review C
- Vol. 86 (1) , 019802
Reply to “Comment on ‘Neutron knockout of12Bepopulating neutron-unbound states in11Be’ ”
In the preceding Comment, Fortune argues that, in our original paper [Peters et al., Phys. Rev. C 83, 057304 (2011)], we did not or could not separate the two neutron-unbound states in near 4 MeV. However, including the suggested contribution of the 3.887-MeV state decaying via 18 keV to the state in does not fit the data; neither do any other attempts incorporating any contribution of this decay channel. The best fit was achieved with a single resonance of decay energy 80(2) keV.- 12 June 2012
- Published by American Physical Society (APS) in Physical Review C
- Vol. 85 (6)
Al+elastic and inelastic scattering reactions and galactic abundances ofAlGalactic 26Al is the first radioactive nucleus to be positively identified by $\gamma${}-ray astronomy with detection of the 1.809~MeV $\gamma${} ray associated with its decay. This nucleus is destroyed in astrophysical environments in the 26Al(p,$\gamma${})27Si and inelastic 26Al+p scattering reactions where properties of 27Si levels determine reaction rates. To investigate these properties, elastic and inelastic 26Al+p scattering reactions were measured between Ec.m.~= 0.5\char21{}1.5~MeV at the Holifield Radioactive Ion Beam Facility (HRIBF) at Oak Ridge National Laboratory (ORNL). A candidate for a new resonance in the 26Al(p,$\gamma${})27Si reaction was identified. Upper limits were also set on the strengths of postulated resonances and on the cross section of the inelastic reaction, but there is little effect on current reaction rate calculations.
- 12 June 2012
- Published by American Physical Society (APS) in Physical Review C
- Vol. 85 (6)
Al+elastic and inelastic scattering reactions and galactic abundances ofAlGalactic 26Al is the first radioactive nucleus to be positively identified by $\gamma${}-ray astronomy with detection of the 1.809~MeV $\gamma${} ray associated with its decay. This nucleus is destroyed in astrophysical environments in the 26Al(p,$\gamma${})27Si and inelastic 26Al+p scattering reactions where properties of 27Si levels determine reaction rates. To investigate these properties, elastic and inelastic 26Al+p scattering reactions were measured between Ec.m.~= 0.5\char21{}1.5~MeV at the Holifield Radioactive Ion Beam Facility (HRIBF) at Oak Ridge National Laboratory (ORNL). A candidate for a new resonance in the 26Al(p,$\gamma${})27Si reaction was identified. Upper limits were also set on the strengths of postulated resonances and on the cross section of the inelastic reaction, but there is little effect on current reaction rate calculations.
- Open Access
- 8 May 2012
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 108 (19) , 192701
Halo Nucleus: A Spectroscopic Study via Neutron TransferThe best examples of halo nuclei, exotic systems with a diffuse nuclear cloud surrounding a tightly bound core, are found in the light, neutron-rich region, where the halo neutrons experience only weak binding and a weak, or no, potential barrier. Modern direct-reaction measurement techniques provide powerful probes of the structure of exotic nuclei. Despite more than four decades of these studies on the benchmark one-neutron halo nucleus , the spectroscopic factors for the two bound states remain poorly constrained. In the present work, the reaction has been used in inverse kinematics at four beam energies to study the structure of . The spectroscopic factors extracted using the adiabatic model were found to be consistent across the four measurements and were largely insensitive to the optical potential used. The extracted spectroscopic factor for a neutron in an state coupled to the ground state of is 0.71(5). For the first excited state at 0.32 MeV, a spectroscopic factor of 0.62(4) is found for the halo neutron in a state.- 8 May 2012
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 108 (19) , 192701
Open AccessHalo Nucleus: A Spectroscopic Study via Neutron TransferThe best examples of halo nuclei, exotic systems with a diffuse nuclear cloud surrounding a tightly bound core, are found in the light, neutron-rich region, where the halo neutrons experience only weak binding and a weak, or no, potential barrier. Modern direct-reaction measurement techniques provide powerful probes of the structure of exotic nuclei. Despite more than four decades of these studies on the benchmark one-neutron halo nucleus , the spectroscopic factors for the two bound states remain poorly constrained. In the present work, the reaction has been used in inverse kinematics at four beam energies to study the structure of . The spectroscopic factors extracted using the adiabatic model were found to be consistent across the four measurements and were largely insensitive to the optical potential used. The extracted spectroscopic factor for a neutron in an state coupled to the ground state of is 0.71(5). For the first excited state at 0.32 MeV, a spectroscopic factor of 0.62(4) is found for the halo neutron in a state. - Open Access
- 9 March 2012
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 108 (10) , 102501
First Observation of Ground State Dineutron Decay:We report on the first observation of dineutron emission in the decay of . A single-proton knockout reaction from a beam was used to populate the ground state of . is bound with respect to the emission of one neutron and unbound to two-neutron emission. The dineutron character of the decay is evidenced by a small emission angle between the two neutrons. The two-neutron separation energy of was measured to be 1.35(10) MeV, in good agreement with shell model calculations, using standard interactions for this mass region.- 9 March 2012
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 108 (10) , 102501
Open AccessFirst Observation of Ground State Dineutron Decay:We report on the first observation of dineutron emission in the decay of . A single-proton knockout reaction from a beam was used to populate the ground state of . is bound with respect to the emission of one neutron and unbound to two-neutron emission. The dineutron character of the decay is evidenced by a small emission angle between the two neutrons. The two-neutron separation energy of was measured to be 1.35(10) MeV, in good agreement with shell model calculations, using standard interactions for this mass region.