E 1.99: conf-860629-14
|
Longitudinal emittance measurement at the ATS |
1 |
E 1.99: conf-860629-15
|
Influence of equipartitioning on the emittance of intense charged-particle beams |
1 |
E 1.99: conf-860629-16
|
Polarized H⁻ source development at BNL |
1 |
E 1.99: conf-860629-17
|
Progress in the development of H⁻ ion sources |
1 |
E 1.99: conf-860629-18
|
Status of the BNL 200 MeV Linac |
1 |
E 1.99: conf-860629-19
|
Novel accelerators employing high-current electron beams numerical simulations |
1 |
E 1.99: conf-860629-21
|
Beamstrahlung monitor for SLC final focus using gamma ray energies |
1 |
E 1.99: conf-860629-22
|
Beamstrahlung monitor for SLC final focus using visible wavelengths |
1 |
E 1.99: conf-860629-23
|
Design of an RFQ-based, H⁻ injector for the BNL/FNAL 200 MeV proton linacs |
1 |
E 1.99: conf-860629-24
|
RFQ'S in research and industry |
1 |
E 1.99: conf-860629-25
|
Unified formulation for linear accelerator design |
1 |
E 1.99: conf-860629-26
|
Present optics options for TeV colliders |
1 |
E 1.99: conf-860629-27
|
Progress on plasma accelerators |
1 |
E 1.99: conf-860629-28
|
Beam dynamics, efficiency and power of the SLAC lasertron simulation results. |
1 |
E 1.99: conf-860629-29
|
Operational experience with SLAC energy upgrade |
1 |
E 1.99: conf-860629-31
|
SLAC low emittance accelerator test facility |
1 |
E 1.99: conf-860629-32
|
Maximum efficiency of a conventional klystron output cavity |
1 |
E 1.99: conf-860629-33
|
Deflection by the image current and charges of a beam scraper |
1 |
E 1.99: conf-860629-34
|
SLC energy spectrum monitor using synchrotron radiation |
1 |
E 1.99: conf-860629-35
|
Beam-beam deflections as an interaction point diagnostic for the SLC |
1 |