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Calvin R. Howell

Calvin R. Howell

· Professor of PhysicsVerified

Duke University · Physics

Active 1982–2025

h-index42
Citations7.1k
Papers53055 last 5y
Funding$1.3M
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About

Professor Calvin R. Howell's research is in the area of experimental nuclear physics with emphasis on the quantum chromodynamics (QCD) description of low-energy nuclear phenomena, including structure properties of nucleons and nuclei and reaction dynamics in few-nucleon systems. The macroscopic properties of nucleon structure and the residual strong nuclear force between neutrons and protons in nuclei emerge from QCD at distances where the color interactions between quarks and gluons are strong. However, the details of the mechanisms that generate the strong nuclear force are not well understood. Effective field theories (EFT) and Lattice QCD calculations provide theoretical frames that connect low-energy nuclear phenomena to QCD. Professor Howell and collaborators are conducting experiments on few-nucleon systems that test predictions of ab-initio theory calculations for the purpose of providing insight about the QCD descriptions of low-energy nucleon interactions and structure. His current projects include measurements of the electromagnetic and spin-dependent structure properties of nucleons via Compton scattering on the proton and few-nucleon systems and studies of two- and three-nucleon interactions using few-nucleon reactions induced by photons and neutrons. In the coming years, a focus will be on investigating the neutron-neutron interaction in reactions and inside nuclei. In addition, his work includes applications of nuclear physics to national nuclear security, medical isotope production, and plant biology. Most of his research is carried out at the High Intensity Gamma-ray Source and the tandem laboratory at TUNL.

Research topics

  • Computer Science
  • Physics
  • Optics
  • Particle physics
  • Nuclear physics
  • Atomic physics
  • Astronomy

Selected publications

  • Finite-Geometry Corrections for Neutron Scattering Cross Section Measurements

    2025-09-01

    reportOpen access

    In this report, we describe the corrections necessary for neutron scattering cross section measurements in experiments which use finite-geometry scattering samples.A new Geant4 based framework was developed to calculate these corrections which has been benchmarked against a well-measured test case.This framework also calculates the outgoing neutron energy dependence of the correction factors, which is crucial when resolving individual final states in the scatterer is not possible.

  • Energy dependence of chain fission product yields from neutron-induced fission of 235U, 238U, and 239Pu

    Nuclear Data Sheets · 2025-05-13 · 4 citations

    article
  • Energy Dependent Fission Product Yields

    2025-02-11

    reportOpen access

    This project utilized a 10-meter Fast Transfer System (called RABITTS) and Decay Station. FPYs are measured using neutron activation of U-235 and Pu-239 followed by gamma ray spectroscopy. We irradiated targets with mono-energetic neutrons produced at the TUNL tandem accelerator laboratory. The gamma spectra collected in these target irradiations are being analyzed to determine FPY values.

  • Characterization of 235U, 238U and 239Pu fission ionization chamber foils by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si42.svg" display="inline" id="d1e2151"><mml:mi>α</mml:mi></mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si288.svg" display="inline" id="d1e2157"><mml:mi>γ</mml:mi></mml:math>-ray spectrometry

    Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment · 2024-03-07 · 4 citations

    articleOpen access
  • Energy-Dependent Fission-Product Yields in the Region of Second-Chance Fission

    EPJ Web of Conferences · 2024-01-01

    articleOpen access

    The energy dependence of high-yield fission products has been measured using quasi-monoenergetic neutron beams at energies between 5.5 and 11.0 MeV. The absolute number of fissions during the irradiation period was determined via dual-fission ionization chambers, while the fission products were measured via direct g-ray spectroscopy. This paper presents absolute fission product yields from neutron-induced fission of 235 U, 238 U, and 239 Pu isotopes for five incident energies in the second chance fission region.

  • Energy Dependent Fission Product Yields (2nd year Milestone and Deliverables)

    2024-01-18

    reportOpen access1st authorCorresponding

    Introduction to the project: One of the Laboratory missions is to provide consistent, high-precision fission product; yield data critical for testing fission models and maintaining the safety and security of the nation’s nuclear weapons stockpile. However, high-quality, energy-differential fission product yield data is missing for certain actinides and neutron energies important to constrain the new U.S. Nuclear Data Program evaluation effort; It has been shown that the reactor antineutrino anomaly may be at least partially caused by roughly 20 fission products. The fission product yield data is missing or incomplete for many of these isotopes, thus it is necessary to accurately determine these values to better constrain the anomaly; Aitor Bracho is measuring very short-lived (seconds to minutes) fission product yields of 235U and 239Pu using monoenergetic neutron beams at En = 60 and 560 keV; Aitor Bracho is using a direct approach utilizing a state-of-the-art rabbit transfer system, superior HPGe detector, and digital acquisition systems for fission decay measurements. The goals of this project: lop experimental capabilities and data analysis techniques to carry out the gamma-ray spectra analysis necessary for fission product yield calculation; Provide high-precision and energy-dependent fission product data supporting fission theory, neutrino physics, and applied physics.

  • Photo-nuclear cross sections on $^{197}$Au, an update on the gold standard

    arXiv (Cornell University) · 2024-02-23

    preprintOpen access

    A method was developed for measuring photonuclear reactions concurrently at several discrete photon beam energies on a stack of different target materials via a single irradiation. Concentric ring targets of the materials (in order from front to back targets: Au, TiO$_2$, Zn, Os, and Au) were irradiated at the High Intensity Gamma-ray Source (HI$γ$S). As a proof of principle, we report the result of the cross section measurements from the front Au target. The excitation functions of the $^{197}$Au($γ$,n)$^{196}$Au and $^{197}$Au($γ$,3n)$^{194}$Au reactions were determined in the incident photon energy range of 13-31 MeV using quasi-monoenergetic photon beams provided at HI$γ$S. The cross sections of the combined ground state (2$^{-}$) and short-lived first isomeric state (m1, 5$^{+}$), and of the second isomeric state (m2, 12$^{-}$) in the $^{196}$Au production are obtained separately by subtracting the $γ$ rays from the internal conversion of the second isomeric state. The excitation function of the second isomeric state via the photon-induced reaction $^{197}$Au($γ$,n)$^{196m2}$Au was measured for the first time. By using the activation method rather than direct neutron counting, the exclusive cross sections for the ($γ$,n) and ($γ$,3n) reactions were determined. Comparing the yields from the front and back gold targets validates our ability to simulate the effect of photon scattering in the target stack and provides a method for assessing the systematic uncertainty of our technique.

  • Photonuclear cross sections for <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mmultiscripts><mml:mi>Au</mml:mi><mml:mprescripts/><mml:none/><mml:mn>197</mml:mn></mml:mmultiscripts></mml:math>: An update on the gold standard

    Physical review. C · 2024-12-05 · 2 citations

    articleOpen access

    Cross sections for the $^{197}\mathrm{Au}(\ensuremath{\gamma},n)$ reaction are broadly used in nuclear physics as a standard for normalizing photonuclear reaction cross-section data at photon beam energies above approximately 8 MeV. In this paper, we report cross-section measurements for the $^{197}\mathrm{Au}{(\ensuremath{\gamma},n)}^{196}{\mathrm{Au}}^{g+m1}$ reaction at beam energies from 13 to 31 MeV. Our measurements provide the first cross-section data for this reaction at beam energies above 20 MeV, enabling the use of this reaction as a cross-section standard up to 30 MeV. Also, this work provides first cross-section measurements for the $^{197}\mathrm{Au}(\ensuremath{\gamma},n)^{196}\mathrm{Au}^{m2}$ reaction. In addition, we measured cross-section data for the $^{197}\mathrm{Au}(\ensuremath{\gamma},3n)^{194}\mathrm{Au}$ reaction, which can be used as a cross-section standard above about 25 MeV. These measurements were performed using a new target activation method that is based on the angle-energy correlation of the laser Compton-scattered photon beams at the High Intensity Gamma-ray Source ($\mathrm{HI}\ensuremath{\gamma}\mathrm{S}$). The technique enables measuring photonuclear reaction cross-sections at several discrete beam energies concurrently via a single irradiation on a stack of different targets. Measurements were carried out by irradiating a stack of concentric-ring targets consisting of Au, ${\mathrm{TiO}}_{2}$, Zn, Os, and Au (in order of the $\ensuremath{\gamma}$-ray beam direction). Our data for the $^{197}\mathrm{Au}(\ensuremath{\gamma},n)^{196}\mathrm{Au}^{g+m1}$ reaction in the energy range of 13 to 20 MeV are in good agreement with existing ones measured using monoenergetic $\ensuremath{\gamma}$-ray beams, but differ from data acquired using a bremsstrahlung $\ensuremath{\gamma}$-ray beam. Also, above 18 MeV, our data for the $^{197}\mathrm{Au}(\ensuremath{\gamma},n)^{196}\mathrm{Au}^{g+m1}$ and $^{197}\mathrm{Au}(\ensuremath{\gamma},n)^{196}\mathrm{Au}^{m2}$ reactions differ significantly from the most recent TENDL and JENDL evaluations, suggesting a need to update these data libraries. The TENDL evaluation and existing data are consistent with our data for the $^{197}\mathrm{Au}(\ensuremath{\gamma},3n)$ reaction, but differ significantly from the JENDL evaluation above 26 MeV.

  • Proceedings of the Workshop for Applied Nuclear Data Activities WANDA 2022

    2024-02-15 · 2 citations

    reportOpen access

    On February 28 – March 4, 2022, the Nuclear Data Interagency Working Group (NDIAWG) hosted the 5-day virtual Workshop for Applied Nuclear Data (WANDA2022) to facilitate interagency collaboration on nuclear data for applications. This year’s focus was nuclear data for space applications, but also included photon reactions and transport, reactions on unstable nuclei, and data adjustment topics. The annual WANDA workshops are planned by the Nuclear Data Working Group (NDWG) with the goal of assembling users and producers of nuclear data to provide input to identify and prioritize nuclear data needs and to suggest solutions to address those needs. The workshop consisted of talks by agency program managers, six topic focused road mapping sessions and a review of NDIAWG-funded projects. More than 350 attendees represented national laboratories, universities, and federal agencies, as well as international organizations and industry. The proceedings presented herein summarize the workshop’s content, highlight important outcomes, and document attendees’ recommendations.

  • Use of the HIFROST Dilution Refrigerator for the $T_{20}$ Experiment

    2024-07-30

    articleOpen access

    I discussed the importance of the $T_{20}$ quantity, a tensor analyzing power, and the basic experimental setup for a measurement of $\stackrel{\leftrightarrow}{d}$ ($\vec{\gamma}$, n)p, the deuteron photodisintegration. Multiple measurements have suggested the existence of a channel around 9 MeV above two nucleon masses. This diverges from calculations from current nuclear theory, and this experiment will focus on this new channel and yield information on the nature of any discrepancy. This experiment will immediately follow the experiment of the GDH measurement on the deuteron and use a lot of the same equipment. While the target will be polarized in the GDH experiment, the target will have the tensor component enhanced for the $T_{20}$ experiment. I will discuss the status of the experiment, as well as the current status of the dilution refrigerator, and the progress being made.

Recent grants

Frequent coauthors

  • W. Tornow

    547 shared
  • R. L. Walter

    Duke University

    230 shared
  • A. S. Crowell

    Triangle Universities Nuclear Laboratory

    213 shared
  • A. P. Tonchev

    Duke University

    172 shared
  • J. H. Kelley

    124 shared
  • B. Fallin

    Savannah River National Laboratory

    106 shared
  • G. J. Weisel

    101 shared
  • H. Witała

    Jagiellonian University

    92 shared

Awards & honors

  • Trinity College Honors Faculty Leadership in the Classroom a…
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