Titlebook: Experimental Physics; Methods and Apparatu D. V. Skobel’tsyn (Director) Book 1969 Consultants Bureau, New York 1969 experiment.experimental

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The Conflict Between Art and Societyfeatures of these are their high sensitivity and low inertia, which enables individual light quanta emitted in the scintillator to be recorded over a short period of time. In this article we shall consider questions relating to the use of scintillation and Cerenkov counters for studying nuclear even

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https://doi.org/10.1007/978-94-009-0459-0load (“cathode follower,” Fig. 2), has a much lower output resistance and a greater transmission coefficient at low frequencies than a cathode follower [1, 2], With increasing plate load R. of the tube L., these advantages of the white stage become greater; however, as will be shown by the calculati

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https://doi.org/10.1007/978-1-4684-0673-3experiment; experimental physics; feedback; particles; photon; physics; statistics

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Apparatus for Recording Neutral Particles by Reference to Decay Gamma Quanta,cademy of Sciences (FIAN), records and measures the energy of two 100 to 650 MeV . quanta simultaneously incident on its detectors; this apparatus may thus be employed in order to study any processes in which such . quanta are formed.

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https://doi.org/10.1007/978-3-662-31584-2In this article we shall consider a physical system for recording charged particles formed as a result of the interaction of a beam of primary particles with target nuclei. Between the target and the detector is a magnetic spectrometer in which the secondary particles are analyzed with respect to momentum.

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Experimental Method of Determining the Efficiency Function of an Apparatus Containing a Magnetic SpIn this article we shall consider a physical system for recording charged particles formed as a result of the interaction of a beam of primary particles with target nuclei. Between the target and the detector is a magnetic spectrometer in which the secondary particles are analyzed with respect to momentum.

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Wilson Chamber for Studying Photomeson Processes,The use of chamber methods (Wilson, bubble, and diffusion chambers) in electron accelerators is usually limited either owing to the long dead time, as in the case of Wilson chambers, or owing to the unacceptably large ion overloadings, as in the case of the diffusion and (particularly) bubble chambers.