E 1.99:conf-8608108-3
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Systematics of energy levels and other properties of highly charged ions |
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E 1.99:conf-8608108-4
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What is new in convoy electron physics |
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E 1.99:conf-8608108-5
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An overview of low-energy ion-atom collisions |
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E 1.99: conf-8608109-1
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Predictive models for thermal hazards. [lowest constant surface temperature at which material of given size and shape will self-heat to catastrophic destruction] |
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E 1.99: conf-8608111-1
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Massive sulfide deposits and hydrothermal solutions incremental reaction modeling of mineral precipitation and sulfur isotopic evolution. |
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E 1.99: conf-8608113-summs
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Workshop on short-term health effects of reactor accidents Chernobyl. |
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E 1.99: conf-8608121-1
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Design and characterization for absolute x-ray spectrometry in the 100-10,000 eV region |
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E 1.99: conf-8608121-3
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Development of an x-ray fluorescence microprobe at the National Synchrotron Light Source, Brookhaven National Laboratory Early results. |
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E 1.99:conf-8608123-1
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Damping rings for achieving ultra-small electron beam emittance |
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E 1.99: conf-8608123-2
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Lasers for open structures |
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E 1.99: conf-8608123-3
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Laser focusing of high-energy charged-particle beams |
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E 1.99: conf-8608123-4
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Radio frequency phase in the FEL section of a TBA |
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E 1.99: conf-8608123-5
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Multi-TeV muon colliders |
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E 1.99: conf-8608123-6
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What is the most efficient high-energy accelerator |
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E 1.99: conf-8608123-7
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The SLAC lasertron project |
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E 1.99: conf-8608123-8-rev
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A Solid state accelerator |
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E 1.99: conf-8608123-9
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Status of Switched-Power Linac studies at BNL (Brookhaven National Laboratory) and CERN (European Organization for Nuclear Research) |
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E 1.99: conf-8608123-10
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The ANL experiment for a wake field accelerator using an rf structure |
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E 1.99: conf-8608123-11-rev
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The microlasertron An efficient switched-power source of mm wavelength radiation. |
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E 1.99: conf-8608124-1
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Numerical models for the evaluation of geothermal systems |
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