E 1.99:slac-pep-note-139
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The PEP electron-positron ring |
1 |
E 1.99:slac-pep-note-140
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Event rates to be expected at PEP |
1 |
E 1.99:slac-pep-note-142
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Non-magnetic detector for measuring sigma/sub T/ and charged multiplicities in e⁺⁻ annihilation |
1 |
E 1.99:slac-pep-note-143
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Precise measurement of the total cross section |
1 |
E 1.99:slac-pep-note-145
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Contribution of the two-photon annihilation process in the measurement of sigma/sub t/ (e⁺e/sup /minus//. -->. hadrons at PEP) |
1 |
E 1.99:slac-pep-note-149
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The detection of low-energy charged particles with particle identification up to 3. 5 GeV/c |
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E 1.99:slac-pep-note-151
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A streamer chamber detector for PEP |
1 |
E 1.99:slac-pep-note-152
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Comments on the simultaneous measurement of charged and neutral components of multi-hadron events |
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E 1.99:slac-pep-note-156
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Liquid argon gamma ray detector Variations of the Willis chamber. |
1 |
E 1.99:slac-pep-note-158
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Tests of. mu. -e universality for weak neutral currents at PEP |
1 |
E 1.99:slac-pep-note-160
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A suggested detector |
1 |
E 1.99:slac-pep-note-161
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Study of the reaction e⁺e/sup/minus// /yield/. mu. ⁺. mu. /sup/minus// with an iron solenoid spectrometer |
1 |
E 1.99:slac-pep-note-163
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Direct measurement of muon polarization in e⁺e/sup − /yields/ μ/sup /minus//mu/⁺ |
1 |
E 1.99:slac-pep-note-164
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Strange particle experiments at PEP |
1 |
E 1.99:slac-pep-note-165
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Parity-violating momentum correlations as a means of observing weak interactions in e⁺e⁻ → hadrons |
1 |
E 1.99:slac-pep-note-168
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Note on longitudinal beam polairzation |
1 |
E 1.99:slac-pep-note-169
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Resonance method to produce a polarisation asymmetry in electron-positron storage rings |
1 |
E 1.99:slac-pep-note-170
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Two methods to measure the e/sup /plus minus// polarization at PEP |
1 |
E 1.99:slac-pep-note-172
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A first look at a polarimeter for EPIC or PEP |
1 |
E 1.99:slac-pep-note-173
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An alternate way of measuring beam polarization at an e⁺e/sup /minus// colliding beam facility |
1 |