| Opening Address (p. 1) |
| by Davier, M |
| Horizons of high energy physics (p. 7) |
| by Llewellyn Smith, Christopher Hubert |
| RF linacs and power conversion (p. 23) |
| by Henke, H |
| Non-resonant field generation (p. 48) |
| by Aronson, S H |
| Lasers and plasmas in particle acceleration (p. 58) |
| by Bobin, J L |
| The interdependence of parameters for TeV linear colliders (p. 80) |
| by Palmer, R B |
| Status of the SLC (p. 122) |
| by Seeman, J T |
| Summary of working group 1 : on "semi-conventional" high-frequency linacs(p. 137) |
| by Schnell, Wolfgang |
| Summary of working group 1 on semi-conventional high-frequency linacs (p. 137) |
| by Schnell, W |
| Beam dynamics issues for linear colliders (p. 147) |
| by Ruth, Ronald D |
| Choice of parameters for linear colliders in multi-bunch mode (p. 161) |
| by Claus, J |
| Distortion of a short rf pulse in travelling-wave accelerating structures (p. 181) |
| by Geschonke, G |
| Distortion of a short rf pulse in travelling-wave accelerating structures (p. 181) |
| by Geschonke, Günther |
| Studies of a frequency scaled model transfer structure for a two-stage linear collider (p. 188) |
| by Garvey, T |
| Studies of a frequency scaled model transfer structure for a two-stage linear collider (p. 188) |
| by Garvey, Terence |
| High average power linear induction accelerator development (p. 195) |
| by Bayless, J R |
| Possible parameters of pulsers for linear induction linacs (p. 202) |
| by Bobylev, V I |
| Cost optimization of induction linac drivers for linear colliders (p. 205) |
| by Barletta, W A |
| Conventional power sources for colliders (p. 220) |
| by Allen, M A |
| High power gyrotrons as microwave sources for particle accelerators (p. 223) |
| by Tran, M Q |
| Phase control of the microwave radiation in free electron laser two-beam accelerator (p. 231) |
| by Goren, Y |
| Physics of relativistic klystrons (p. 239) |
| by Yu, S S |
| Lasertron development and tests of high gradient accelerating structures in Japan (p. 244) |
| by Shidara, T |
| Accelerator R and D at LAL-Orsay (p. 253) |
| by Le Duff, J |
| Lasertron computer simulation at Orsay : "RING" code(p. 259) |
| by Dubrovin, A |
| Gigatron (p. 264) |
| by Bizek, H M |
| The microlasertron (p. 272) |
| by Palmer, R B |
| Summary of working group 2 on transformer mechanisms (p. 291) |
| by Weiland, T |
| The wake field transformer experiment at DESY (p. 298) |
| by Bialowons, W |
| Hollow beam gun for the wake field transformer experiment at DESY (p. 308) |
| by Bialowons, W |
| Hollow beam measurements (p. 317) |
| by Bialowons, W |
| Computer simulations for the DESY wake field transformer experiment (p. 327) |
| by Bialowons, W |
| Feasibility studies for the switched power linac (p. 336) |
| by Knott, J E |
| Summary of working group 3 on acceleration using plasmas (p. 345) |
| by Evans, R G |
| Experimental work at UCLA on the plasma beat wave accelerator (p. 351) |
| by Clayton, C |
| Experimental work at UCLA on the plasma beat wave accelerator (p. 351) |
| by Joshi, C |
| Effect of electron density mismatch on the saturation amplitude of the plasma beat wave (p. 360) |
| by Martin, F |
| The IC/RAL beat-wave experiments (p. 375) |
| by Dangor, A E |
| The IC/RAL beat-wave experiments (p. 375) |
| by Dangor, A E |
| REB-CO2 laser interaction program, "sigma program", beat wave acceleration (p. 386) |
| by Kitagawa, Y |
| $REB-CO_{2}$ laser interaction program, "$\Sigma$ program", beat wave acceleration (p. 386) |
| by Kitagawa, Y |
| Interaction experiments in long and homogeneous plasmas (p. 392) |
| by Amiranoff, F |
| Electron density measurement in a plasma by three-wave interferometry (p. 397) |
| by Says, L P |
| Electron density measurement in a plasma by three-wave interferometry (p. 397) |
| by Says, L P |
| Theoretical work on plasma accelerators at UCLA (p. 401) |
| by Katsouleas, T C |
| Saturation mechanisms in the plasma beat wave accelerator (p. 412) |
| by Mora, P |
| Limitation of the beat-wave generation due to the modulational and decay instabilities (p. 418) |
| by Pesme, D |
| Limitation of the beat-wave generation due to the modulational and decay instabilities (p. 418) |
| by Pesme, D |
| Energy cascading in the beat-wave accelerator (p. 443) |
| by McKinstrie, C J |
| Energy cascading in the beat-wave accelerator (p. 443) |
| by McKinstrie, C J |
| Dephasing effects in beat-wave acceleration (p. 458) |
| by Salomaa, R R E |
| Dephasing effects in beat-wave acceleration (p. 458) |
| by Salomaa, R R E |
| Wake-field of charged particles in a plasma (p. 472) |
| by Acopian, E A |
| Charged particle acceleration by microwave field in plasma (p. 476) |
| by Acopian, E A |
| High longitudinal electric fields and double layers in laser produced plasmas for particle acceleration (p. 480) |
| by Hora, Heinrich |
| Summary report of working group 4 on e+e- sources, low emittance production and preservation, part I, damping rings (p. 491) |
| by Pellegrini, C |
| Summary report of working group 4 on $e^{+}e^{-}$ sources, low emittance production and preservation (p. 493) |
| by Pellegrini, C |
| Summary report of working group 4 on e+e- sources, low emittance production and preservation, part II, high brightness guns (p. 497) |
| by Le Duff, J |
| Photocathodes in accelerator applications (p. 501) |
| by Fraser, J S |
| Short-pulse high-current-density photoemission in high electric fields (p. 506) |
| by Fischer, J |
| Short-pulse high-current-density photoemission in high electric fields (p. 506) |
| by Fischer, J |
| New idea for laser production of very high electron densities (p. 516) |
| by Girardeau-Montaut, J P |
| Multipoint $Si^{+}_{-}$ cesiated photocathodes for lasertron devices (p. 525) |
| by El-Manouni, A |
| Multipoint Sip+ cesiated photocathodes for lasertron devices (p. 525) |
| by El Manouni, A |
| A study of tolerances for low emittance damping rings (p. 530) |
| by Krejcik, P |
| Notes on the principles of low-emittance sources (p. 537) |
| by Cavenago, M |
| Linear emittance damper with megagauss fields (p. 544) |
| by Barletta, W A |
| Summary report of the working group 5 on final focus and interaction point (p. 551) |
| by Chen, P |
| Plasma lenses for focusing particle beams (p. 554) |
| by Riege, H |
| Noise in plasma lenses for high energy particle beams (p. 573) |
| by Evans, R G |
| A flat-beam final-focus system (p. 577) |
| by Chao, A |
| A study of the feasibility of an open resonator as a device for focusing a bunched beam (p. 587) |
| by Brambilla, Elena |
| Quantum beamstrahlung from gaussian bunches (p. 593) |
| by Chen, P |
| Particle in cell simulations of disruption (p. 605) |
| by Fawley, W M |
| Small disruption revisited (p. 610) |
| by Pérez y Jorba, J |
| Application of high power, intense electron beams to ultra high energy electron accelerators (p. 623) |
| by Nation, J A |
| Open accelerating structures (p. 633) |
| by Palmer, R B |
| Crystal x-ray accelerator (p. 642) |
| by Tajima, T |
| Crystal as linac structure for x-rays (p. 649) |
| by Tajima, T |
| Crystal as a linac structure for x-rays (p. 649) |
| by Tajima, T |
| Ferroelectrics and their possible use in accelerator physics (p. 660) |
| by Zioutas, Konstantin |
| 2 MeV gamma rays from laser-accelerated electrons (p. 675) |
| by Sherman, N K |
| MeV gamma rays from laser-accelerated electrons (p. 675) |
| by Sherman, N K |
| Progress towards a laser accelerator (p. 685) |
| by Sherman, N K |
| A diffraction radiation model for energy losses (p. 689) |
| by Palumbo, L |
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