Status of the SLC : developments in linear collider physics(p. 19) |
by Krejcik, P |
Linear collider research and development (p. 24) |
by Siemann, R H |
Over-compression, a method to shape the longitudinal bunch distribution for a reduced energy spread (p. 47) |
by Decker, Franz Josef |
1.54 GeV ATF Linac for damping ring (p. 50) |
by Hayano, H |
Design of beam-transport line between the RFQ and the DTL for the JHP 1-GeV proton linac (p. 59) |
by Kato, T |
Final focus system with superconducting magnets in the interaction region of the TESLA linear collider (p. 68) |
by Klein, E |
Next Linear Collider Test Accelerator injector design and status (p. 89) |
by Yeremian, A D |
New engineering techniques used in a high-power model of the 432 MHz DTL (p. 134) |
by Naito, F |
rf characteristics of a high-power model of the 432 MHz DTL (p. 137) |
by Naito, F |
First operation of a 432-MHz, 3-MeV RFQ stabilized with PISLs (p. 166) |
by Ueno, A |
High-power test of a 432-MHz, 3-MeV RFQ stabilized with PISLs (p. 169) |
by Ueno, A |
Low-power rf characteristics of a 432-MHz, 3-MeV RFQ stabilized with PISLs (p. 172) |
by Ueno, A |
Performance of the CERN Linac 2 with a high intensity proton RFQ (p. 175) |
by Hill, C E |
Re-formation of the PF 2.5-GeV linac to 8 GeV (p. 184) |
by Enomoto, A |
Design of the beam transport system of the KEK B-factory injector (p. 190) |
by Kamitani, T |
High-intensity single-bunch beam of the PF 2.5-GeV linac (p. 193) |
by Ohsawa, S |
An 80 MeV injector for ATF linac (p. 236) |
by Hayano, H |
High gradient tests of 1.3 GHz superconducting cavities (p. 251) |
by Kako, E |
Higher order mode damping for a detuned structure (p. 260) |
by Kroll, N M |
High-gradient acceleration test using a resonant ring (p. 266) |
by Oogoe, T |
Low-power measurement on a HOM damped cavity for the ATF damping ring (p. 281) |
by Sakanaka, S |
High power test of HOM-free choke-mode damped accelerating structure (p. 293) |
by Shintake, T |
Tuning method for the accelerating structure with RFQ focusing and increasing voltage (p. 297) |
by Belyaev, O K |
Analysis of detuned structure by open mode expansion (p. 299) |
by Yamamoto, M |
High gradient tests of SLAC Linear Collider accelerator structures (p. 305) |
by Wang, J W |
A beam-based alignment technique for correction of accelerator structure misalignments (p. 311) |
by Kubo, K |
Radioactive beam facilities : a world view(p. 346) |
by D'Auria, J M |
Induction linacs for heavy ion fusion (p. 351) |
by Bangerter, R O |
Multi-bunch beam with thermionic gun for ATF (p. 375) |
by Naito, T |
Pulse modulator for 85 MW klystron in ATF linac (p. 415) |
by Akemoto, M |
Development of the B-factory linac 50-MW pulse klystron (p. 427) |
by Fukuda, S |
Use of SLEDs for high-gradient acceleration (p. 430) |
by Hanaki, H |
Upgrade of the PF 2.5-GeV linac klystron modulator for the KEKB (p. 436) |
by Honma, H |
Tuning measurement of multi-cavity klystrons in diode mode operation (p. 439) |
by Isagawa, S |
High-power test of pill-box and TW-in-ceramic type S-band rf windows (p. 457) |
by Michizono, S |
A new rf power distribution system for X-band linac equivalent to an rf pulse compression scheme of factor 2$^{n}$ (p. 463) |
by Mizuno, H |
rf high power tests of the X-band windows in the TWR (p. 466) |
by Mizuno, H |
FCI simulation on 100 MW class klystron at X-band (p. 469) |
by Odagiri, J |
Development of an rf pulse compressor using a traveling-wave resonator (p. 478) |
by Yamaguchi, S |
Measurement of wakefield suppression in a detuned x-band accelerator structure (p. 481) |
by Adolphsen, C E |
Multibunch emittance growth and its corrections in S-band linear collider (p. 514) |
by Gao, J |
Beam simulation code using accurate gap field distributions in a drift tube linac (p. 523) |
by Kato, T |
Reducing longitudinal emittance growth in RFQ accelerators (p. 526) |
by Koscielniak, Shane Rupert |
Experimental program with beam in TESLA test facility (p. 532) |
by Mosnier, A |
Wake-field issues concerning the KEK B-factory injector linac (p. 535) |
by Ogawa, Y |
Beam dynamics for the CLIC test facility (p. 544) |
by Braun, H |
A modified space charge routine for Linac beam dynamics codes (p. 552) |
by Lapostolle, Pierre M |
Pressure-distribution analysis of the vaccum system for the KEKB injector linac (p. 567) |
by Kakihara, K |
Relativistic-klystron two-beam-accelerator as a power source for a 1 TeV next linear collider : a systems study(p. 597) |
by Yu, S |
Beam emittance preservation in linear colliders (p. 616) |
by Guignard, Gilbert |
Linear collider structures (p. 621) |
by Higo, T |
Tutorial on beam-based feedback systems for linacs (p. 626) |
by Hendrickson, L |
High-precision spot size monitors for e+e- linear colliders (p. 633) |
by Shintake, T |
Developments of high power rf components (p. 638) |
by Takata, K |
The heavy ion linac for the CERN lead ion facility (p. 654) |
by Warner, D J |
The polarized electron source of the Stanford Linear Accelerator Center (p. 676) |
by Schultz, D |
Cavity construction and low power tests of the INS split coaxial RFQ for radioactive nuclei (p. 689) |
by Arai, S |
Construction and commissioning of the RFQ for the CERN lead-ion facility (p. 722) |
by Bezzon, G P |
Beam transport design for the linac system in the INS radioactive beam facility (p. 725) |
by Niki, K |
The matching line between the RFQ and the IH Linac of the CERN lead ion facility (p. 731) |
by Facco, A |
Performances of the LEBT of the CERN lead ion Linac (p. 734) |
by Lombardi, A M |
The IH Linac of the CERN lead injector (p. 743) |
by Angert, N |
Beam dynamics design of the INS split coaxial RFQ for radioactive nuclei (p. 762) |
by Tokuda, N |
Model measurement and present status of interdigital-H linac at INS (p. 765) |
by Tomizawa, M |
Proof-of-principle experiments of laser wake-field acceleration (p. 798) |
by Nakajima, K |
Control system for a bunch/profile monitor at the KEK e+/e- linac (p. 819) |
by Furukawa, K |
New control system for the KEK linac (p. 822) |
by Kamikubota, N |
R&D of the ATF timing system (p. 831) |
by Korhonen, T T |
Development of components for an S-band electron linac rf feedback control (p. 837) |
by Otake, Y |
Dependence of the wall-current monitor on the beam position (p. 848) |
by Komatsu, J |
High precision beam position monitor using a re-entrant coaxial cavity (p. 851) |
by Bossart, Rudolf |
Monitor of seismic vibration for the KEK linac (p. 863) |
by Kamikubota, N |
BPM electronics for the B-factory e$^{-}$/e$^{+}$ linac at KEK (p. 872) |
by Lazos, A |
Bunch by bunch beam monitor for ATF injector linac (p. 887) |
by Naito, T |
Emittance measurements of a high-current single-bunch electron beam at the pre-injector of the KEK 2.5-GeV linac (p. 911) |
by Suwada, T |
Beam position monitor of the ATF-DR (p. 914) |
by Tejima, M |
Progress in advanced accelerator concepts (p. 935) |
by Sessler, Andrew M |
FEM drive beam injector for CLIC (p. 945) |
by Corsini, R |
Measurements of the longitudinal beam parameters in the Fermilab linac |
by Popovic, M |