TABLE A.2 University Accelerators
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Beam Characteristics |
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Facility |
Species |
Energies |
Technology |
Research Areas |
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Florida State University Tandem Lilac |
Protons, light to medium heavy ions |
2-10 MeV/u |
Superconducting cavities Polarized lithium beam |
Nuclear structure and decay Spin effects in nucleus-nucleus collisions |
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State University of New York at Stony Brook Tandem-Linac |
Protons, light to medium heavy ions |
2-10 MeV/u |
Superconducting cavities |
Nuclear structure Heavy-ion reactions Atom trapping and spectroscopy |
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University of Notre Dame (IN) Accelerator Facility |
Protons, light to medium heavy ions |
2-21 MeV 0.1-8 MeV/u |
Radioactive beams Intense low-energy stable beams |
Nuclear structure and reactions Fundamental symmetries Nuclear astrophysics |
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Texas A&M University Cyclotron Institute K500 Superconducting Cyclotron |
Protons, light to heavy ions |
2-70 MeV/u |
Intermediate-energy heavy ions Selected radioactive beams |
Nuclear structure and reaction dynamics Nuclear astrophysics with radioactive beams Fundamental symmetries |
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University of Washington Tandem Linac |
Protons, light to medium heavy ions |
2-16 MeV 2-10 MeV/u |
Superconducting cavities Terminal ion source |
Nuclear reactions with heavy ions Tests of fundamental symmetries |
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Triangle Universities Nuclear Laboratory (NC) Tandem Accelerator |
Protons, light ions, neutrons, photons |
1-10 MeV/u |
High-resolution light-ion beams Polarized beams |
Fundamental symmetries Inter-nucleon reactions and light nuclei Nuclear astrophysics |
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University of Wisconsin Tandem Accelerator |
Protons, light ions |
2-12 MeV 1-7 MeV/u |
Polarized beams |
Few-body systems Fundamental symmetries Spin degrees of freedom in nuclei |
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Yale University (CT), Wright Nuclear Structure Laboratory Tandem Accelerator |
Protons, light to heavy ions |
1-40 MeV 1-15 MeV/u |
High-resolution beams |
Nuclear structure Heavy-ion reactions Nuclear astrophysics |
The Indiana University Cyclotron Facility is active in areas of beam-cooling technologies and polarized proton beams. Two cyclotrons provide protons with energies up to 200 MeV for direct beams, as well as serving as the injector complex for the Cooler Ring. This ring can accelerate protons to an energy of 500 MeV. In addition, the Cooler Ring has a state-of-the-art electron-cooling system capable of providing high-resolution, very dense beams. A new synchrotron injector into the Cooler was recently completed, providing a two-orders-of-magnitude increase in beam intensity. Distinguishing characteristics of the facility include polarized beams in all machines and internal polarized gas-jet targets in the cooler.