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Titlebook: Detectors in Heavy-Ion Reactions; Proceedings of the S W. Oertzen Conference proceedings 1983 Springer-Verlag Berlin Heidelberg 1983 Drift.

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樓主: CILIA
11#
發(fā)表于 2025-3-23 12:21:35 | 只看該作者
12#
發(fā)表于 2025-3-23 14:11:27 | 只看該作者
13#
發(fā)表于 2025-3-23 19:53:17 | 只看該作者
,Diogene : A 4π pictorial drift chamber,om Fig. 3. A drawback of Diogene is that it does not measure neutral particles, thus leading to some lack of information about the events. The situation is however more or less the same with other large solid angle detectors. The facts that our coils are in aluminium (and not in copper) and that the
14#
發(fā)表于 2025-3-23 22:56:27 | 只看該作者
15#
發(fā)表于 2025-3-24 06:23:22 | 只看該作者
Gas filled heavy ion detectors, stage of development, continously modified and adapted to new experimental requirements. Heavy ion experiments require detection systems which are able to record simultaneously in only one detector several parameters, like time-of-arrival, position or energy, of particles covering a broad range of
16#
發(fā)表于 2025-3-24 07:25:41 | 只看該作者
New trends in low-pressure gaseous detectors,articles. Their properties are described. Amplification in steps is shown to be feasible at low pressure, providing higher gains and gating possibilities. Both techniques can be extended to single electron detection at gains >10.with possible applications to photon detectors. A new type of a 4π Trac
17#
發(fā)表于 2025-3-24 10:44:02 | 只看該作者
The GSI magnetic spectrometer,s were considered already in the design phase of the ion optical and geometrical layout of the spectrograph. The result is a modular setup with separated function magnets, with variable dispersion and a flexibility to adapt to the various requirements of the experments. The instrument was designed t
18#
發(fā)表于 2025-3-24 15:10:21 | 只看該作者
19#
發(fā)表于 2025-3-24 19:58:59 | 只看該作者
20#
發(fā)表于 2025-3-25 00:23:40 | 只看該作者
,Diogene : A 4π pictorial drift chamber,ire is 8, limiting theoretically the possible multiplicity to 80. The actual limit is certainly smaller due to double track resolution and the difficulty to reconstruct the pattern, which increases exponentially with the density of tracks. The drift chamber covers about 85 % of the full 4π solid ang
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