Authors

S. Ali, The Catholic University of America
A. Ahmidouch, North Carolina A&T State University
G. R. Ambrose, University of Regina
A. Asaturyan, A. I. Alikhanyan National Science Laboratory
C. Ayerbe Gayoso, Old Dominion UniversityFollow
J. Benesch, Thomas Jefferson National Accelerator Facility
V. Berdnikov, Thomas Jefferson National Accelerator Facility
H. Bhatt, Mississippi State University
D. Bhetuwal, Mississippi State University
D. Biswas, Hampton University
P. Brindza, Thomas Jefferson National Accelerator Facility
M. Bukhari, Jazan University
M. Burton, James Madison University
R. Carlini, Thomas Jefferson National Accelerator Facility
M. Carmignotto, The Catholic University of America
M. E. Christy, Thomas Jefferson National Accelerator Facility
C. Cotton, University of Virginia
J. Crafts, The Catholic University of America
D. Day, University of Virginia
S. Danagoulian, North Carolina A&T State University
A. Dittmann, University of Illinois
D. H. Dongwi, Hampton University
B. Duran, Temple University
D. Dutta, Mississippi State University
R. Ent, Thomas Jefferson National Accelerator Facility
H. Fenker, Thomas Jefferson National Accelerator Facility
M. Fowler, Thomas Jefferson National Accelerator Facility
D. Gaskell, Thomas Jefferson National Accelerator Facility
A. Hamdi, University of Regina
N. Heinrich, University of Regina
W. Henry, Thomas Jefferson National Accelerator Facility
N. Hlavin, The Catholic University of America
T. Horn, Thomas Jefferson National Accelerator Facility
G. M. Huber, University of Regina
Y. Ilieva, University of South Carolina
J. Jarrell, James Madison University
S. Jia, Temple University
M. K. Jones, Thomas Jefferson National Accelerator Facility
M. Junaid, University of Regina
M. L. Kabir, Mississippi State University
N. Kalantarians, Virginia Union University
A. Karki, Mississippi State University
S. J.D. Kay, University of Regina
C. E. Keppel, Thomas Jefferson National Accelerator Facility
V. Kumar, University of Regina
S. Lassiter, Thomas Jefferson National Accelerator Facility
W. B. Li, University of Regina
D. Mack, Thomas Jefferson National Accelerator Facility
S. Malace, Thomas Jefferson National Accelerator Facility
J. McMahan, Hampton University
A. Mkrtchyan, The Catholic University of America
H. Mkrtchyan, A. I. Alikhanyan National Science Laboratory
P. Monaghan, Hampton University
C. Morean, The Catholic University of America
P. Nadel-Turonski, Thomas Jefferson National Accelerator Facility
G. Niculescu, James Madison University
M. I. Niculescu, James Madison University
A. Nadeeshani, Hampton University
E. Pooser, Thomas Jefferson National Accelerator Facility
A. Ramos, Florida International University
J. Reinhold, Florida International University
B. Sawatzky, Thomas Jefferson National Accelerator Facility
H. Szumila-Vance, Thomas Jefferson National Accelerator Facility
V. Tadevosyan, A. I. Alikhanyan National Science Laboratory
R. L. Trotta, The Catholic University of America
A. Usman, University of Regina
C. Yero, The Catholic University of America
M. Yurov, University of Virginia
S. Zhamkochyan, A. I. Alikhanyan National Science Laboratory
S. A. Wood, Thomas Jefferson National Accelerator Facility
J. Zhang, University of Virginia

Document Type

Article

Publication Date

2026

DOI

10.1016/j.nima.2025.171070

Publication Title

Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment

Volume

1083

Pages

171070

Abstract

The Super High Momentum Spectrometer (SHMS) has been built for Hall C at the Thomas Jefferson National Accelerator Facility (Jefferson Lab). With a momentum capability reaching 11 GeV/c, the SHMS provides measurements of charged particles produced in electron-scattering experiments using the maximum available beam energy from the upgraded Jefferson Lab accelerator. The SHMS is an ion-optics magnetic spectrometer comprised of a series of new superconducting magnets which transport charged particles through an array of triggering, tracking, and particle-identification detectors that measure momentum, energy, angle and position in order to allow kinematic reconstruction of the events back to their origin at the scattering target. The detector system is protected from background radiation by a sophisticated shielding enclosure. The entire spectrometer is mounted on a rotating support structure which permits measurements to be taken with a large acceptance over laboratory scattering angles from 5.5° to 40°, thus allowing a wide range of low cross-section experiments to be conducted. These experiments complement and extend the previous Hall C research program to higher energies.

Rights

© 2025 The Authors.

This is an open access article under the Creative Commons Attribution 4.0 International (CC BY 4.0) License.

Data Availability

Article states: "Data will be made available on request."

Original Publication Citation

Ali, S., Ahmidouch, A., Ambrose, G. R., Asaturyan, A., Ayerbe Gayoso, C. A., Benesch, J., Berdnikov, V., Bhatt, H., Bhetuwal, D., Biswas, D., Brindza, P., Bukhari, M., Burton, M., Carlini, R., Carmignotto, M., Christy, M. E., Cotton, C., Crafts, J., Day, D.,…Zhang, J. (2026). The SHMS 11 GeV/c spectrometer in Hall C at Jefferson Lab. Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 1083, Article 171070. https://doi.org/10.1016/j.nima.2025.171070

ORCID

0000-0001-8640-5380 (Ayerbe Gayoso)

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