E 1.99: conf-750335--37
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Storage accelerator bending magnet without median plane symmetry |
1 |
E 1.99: conf-750335--38
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Pulsed negative hydrogen source for currents up to one ampere |
1 |
E 1.99: conf-750335--39
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Harp, a short pulse, high current electron beam accelerator |
1 |
E 1.99: conf-750335--40
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Superconducting magnets and cryogenics |
1 |
E 1.99:conf-750335--41
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Uses of accelerators in energy R and D |
1 |
E 1.99: conf-750335--43
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Advances in electrostatic accelerators |
1 |
E 1.99: conf-750335--45
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Preliminary design of a 30 MeV deuteron linear accelerator for the production of intense beams of 14 MeV neutrons |
1 |
E 1.99: conf-750335--47
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Effects in low periodicity lattices resulting from low β insertions |
1 |
E 1.99: conf-750335--49
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Incoherent transverse space charge effects during injection, rf capture and early acceleration in AGS |
1 |
E 1.99: conf-750335--50
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Digital controlled frequency for synchrotron acceleration |
1 |
E 1.99:conf-750335--51
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Design of the Zero Gradient Synchrotron booster II ring magnet |
1 |
E 1.99: conf-750335--52
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Comparison of cold and warm vacuum systems for intersecting storage rings |
1 |
E 1.99:conf-750335--53
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Transport of dc and bunched beams through a 25 MV folded tandem accelerator |
1 |
E 1.99: conf-750335--54
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Resonance excitation by distortion of the β-function coupled with a single beam space charge force |
1 |
E 1.99: conf-750335--55
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Search for the ''abnormal nuclear state'' heavy, A > 200, ion acceleration in the AGS |
1 |
E 1.99: conf-750335--56
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Measurement of the linear coupling in the Brookhaven AGS |
1 |
E 1.99: conf-750335--57
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Spill control and intensity monitoring for the Bevatron--Bevalac external particle beams |
1 |
E 1.99: conf-750335--58
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High charge state heavy ion production from a PIG source |
1 |
E 1.99: conf-750335--60
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Feasibility and advantages of commercial process I/O systems for accelerator control |
1 |
E 1.99: conf-750335--61
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ESCAR superconducting magnet system |
1 |