Experimental Nuclear Structure

The Ursinus College Nuclear Structure Group collaborates with nuclear scientists on experiments at accelerator laboratories like the John D. Fox Laboratory at Florida State University (FSU) and the Facility for Rare Isotope Beams at Michigan State University (FRIB). Our experimental work is focused on understanding the interplay between collective nuclear behavior, such as vibrations and rotations of the entire system, and the behavior of the individual protons and neutrons within it.

Our work is funded by National Science Foundation Grant No. PHY-2208804, “RUI: Shell Structure and Collective Excitations in Exotic Nuclei”.

Inverse-Kinematics Proton Scattering and Coulomb Excitation at the NSCL/FRIB

We have been studying the systematic behavior of proton and neutron contributions to collective excitations of N=28 isotones “south” of ⁴⁸Ca since 2003. Most recently, we have been using the GRETINA gamma-ray tracking array and the NSCL/Ursinus liquid hydrogen target for these studies. There significant experimental evidence for the erosion of the N=28 shell approaching ⁴²Si.

Ratios of neutron to proton transition matrix elements M_n/M_p expressed relative to N/Z for even-even N = 28 isotones compared with shell-model predictions.

Inverse-kinematics proton scattering from ^42,44S, ^41,43P, and the collapse of the N=28 major shell closure, L. A. Riley, D. Bazin, J. Belarge, P. C. Bender, B. A. Brown, P. D. Cottle, B. Elman, A. Gade, S. D. Gregory, E. B. Haldeman, K. W. Kemper, B. R. Klybor, M. A. Liggett, S. Lipschutz, B. Longfellow, E. Lunderberg, T. Mijatovic, J. Pereira, L. M. Skiles, R. Titus, A. Volya, D. Weisshaar, J. C. Zamora, and R. G. T. Zegers, Phys. Rev. C 100, 044312 (2019), arXiv:1910.07986.

In spring and summer of 2023, we began the process of expanding this experimental picture to ⁴²Si at FRIB with a Coulomb excitation experiment. We hope to return soon for the complementary proton-scattering measurement.

Mill Heinze (UC 2024), Jake Kosa (UC 2024), and Alyssa Himmelreich (UC 2026) in the “Data U” where users monitor their data during experiments at FRIB.

The Gretina gamma-ray tracking array installed at the focus of the S800 magnetic spectrograph at FRIB.

Neutron Transfer at John D. Fox Superconducting Linear Accelerator Laboratory at Florida State University (FSU)

We are using the Super Enge Split-Pole Spectrograph (SPS) at FSU to measure high-resolution proton momentum spectra and proton angular distributions from (d,p) reactions in an effort to investigate the energies of neutron orbitals beyond the N=28 shell and how they vary with proton number. We began with a measurement of ⁵⁰Ti(d, p)⁵¹Ti.

(a) Measured f 5/2 and p 1/2 single neutron energy centroids, relative to the p_3/2 energy compared with covariant density functional theory. (b) Single neutron binding energies calculated using covariant density functional theory.

⁵⁰Ti(d, p)⁵¹Ti: Single-neutron energies in the N = 29 isotones, and the N = 32 subshell closure, L. A. Riley, J. M. Nebel-Crosson, K. T. Macon, G. W. McCann, L. T. Baby, D. Caussyn, P. D. Cottle, J. Esparza, K. Hanselman, K. W. Kemper, E. Temanson, and I. Wiedenhöver, Phys. Rev. C 103, 064309 (2021), arXiv:2106.05781.

In summer of 2021, we made a measurement of ⁵⁴Fe(d, p)⁵⁵Fe.

(a) Measured f 5/2 and p 1/2 single neutron energy centroids, relative to the p_3/2 energy compared with covariant density functional theory. (b) Single neutron binding energies calculated using covariant density functional theory.

⁵⁴Fe(d, p)⁵⁵Fe and the evolution of single neutron energies in the N=29 isotones, L. A. Riley, I. C. S. Hay, L. T. Baby, A. L. Conley, P. D. Cottle, J. Esparza, K. Hanselman, B. Kelly, K. W. Kemper, K. T. Macon, G. W. McCann, M. W. Quirin, R. Renom, R. L. Saunders, M. Spieker, and I. Wiedenhöver, Phys. Rev. C 106, 064308 (2022), arXiv.2212.04384.

In summer of 2022 we completed a remeasurement of ⁵²Cr(d,p)⁵³Cr to complete the picture of g_9/2 strength in the N = 29 isotones.

g_9/2 neutron strength in the N=29 isotones and the ⁵²Cr(d, p)⁵³Cr reaction, L. A. Riley, D. T. Simms, L. T. Baby, A. L. Conley, P. D. Cottle, J. Esparza, K. Hanselman, I. C. S. Hay, M. Heinze, B. Kelly, K. W. Kemper, G. W. McCann, R. Renom, M. Spieker, and I. Wiedenhöver, Phys. Rev. C 108, 044306 (2023), arXiv.2310.06722.

In summer 2023, we used the CeBrA demonstrator array of CeBr gamma-ray detectors to collect proton-gamma-ray coincidence data from the same reaction. Gamma-ray angular distributions can be used to clarify angular momentum and parity assignments to excited states.

The CeBrA demonstrator for particle-gamma coincidence experiments at the FSU Super-Enge Split-Pole Spectrograph, A. L. Conley, B. Kelly, M. Spieker, R. Aggarwal, S. Ajayi, L. T. Baby, S. Baker, C. Benetti, I. Conroy, P. D. Cottle, I. B. D’Amato, P. DeRosa, J. Esparza, S. Genty, K. Hanselman, I. Hay, M. Heinze, D. Houlihan, M. I. Khawaja, P. S. Kielb, A.N. Kuchera, G.W. McCann, A. B. Morelock, E. Lopez-Saavedra, R. Renom, L. A. Riley, G. Ryan, A. Sandrik, V. Sitaraman, E. Temanson, M. Wheeler, C. Wibisono, I. Wiedenhöver, Nucl. Instr. Meth. A1058, 168827 (2023), arXiv.2311.00831.