E 1.99: conf-9010264--1
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Light hypernuclei and hyperon-nucleon interaction |
1 |
E 1.99: conf-9010264--2
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Strange particle physics with intense pion beams Prospects for PILAC (Pion Linear Accelerator) |
1 |
E 1.99: conf-9010264--3
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Hypernuclear structure using the (. pi. ,K) |
1 |
E 1.99: conf-9010264--4
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Status of PILAC A pion linac facility for 1-GeV pion physics at LAMPF. |
1 |
E 1.99: conf-9010264--5
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The (. pi. sup + ,K sup + ) reaction Past, present, and future. |
1 |
E 1.99: conf-9010264--6
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What (if anything) can few-body strange systems teach us about quark-gluon hadronic substructure |
1 |
E 1.99: conf-9010264--7
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Prospects for studying the (. pi. sup minus ,K sup 0 ) reaction at PILAC |
1 |
E 1.99: conf-9010264--9
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Hypernuclear spectroscopy with the (. pi. ,K) reaction |
1 |
E 1.99: conf-9010265--1
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ELF (extremely-low-frequency) field interactions at the animal, tissue and cellular levels |
1 |
E 1.99: conf-9010266--1
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Neutron measurements in search of cold fusion |
1 |
E 1.99: conf-9010266--2
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Reproducible neutron emission measurements from Ti metal in pressurized D sub 2 gas |
1 |
E 1.99: conf-9010267--1
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Log-ratio circuit for beam position monitoring |
1 |
E 1.99: conf-9010267--3
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Advanced, time-resolved imaging techniques for electron-beam characterizations |
1 |
E 1.99: conf-9010267--4
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Analysis of the beam position measurement with button-type pickups in APS |
1 |
E 1.99: conf-9010267--5
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A high-frequency Schottky detector for use in the Tevatron |
1 |
E 1.99: conf-9010268--1
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Origin of regularities in the redshift distributions of distant galaxies and quasars |
1 |
E 1.99: conf-9010268--2
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The shape of the invisible halo N-body simulations on parallel supercomputers. |
1 |
E 1.99: conf-9010268--3
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A search for massive compact halo objects in our galaxy |
1 |
E 1.99: conf-9010270--1
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Some nonlinear problems in the manipulation of beams |
1 |
E 1.99: conf-9010270--2
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Invariant tori of the Poincare return map as solutions of functional difference equations |
1 |