1961
DOI: 10.1016/0029-5582(61)91015-x
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Emission of fast particles in a heterogeneous medium

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1971
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Cited by 64 publications
(16 citation statements)
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“…To ensure a small square emitting area, our TR target represented a vertical stripe of one Al foil with a width of 2.5 mm. When one electron hits the target, it emits TR with a conical shape (Ter-Mikaelyan, 1961) (Fig. 3).…”
Section: Experimental Set-upmentioning
confidence: 99%
“…To ensure a small square emitting area, our TR target represented a vertical stripe of one Al foil with a width of 2.5 mm. When one electron hits the target, it emits TR with a conical shape (Ter-Mikaelyan, 1961) (Fig. 3).…”
Section: Experimental Set-upmentioning
confidence: 99%
“…Unfortunately, the radiation intensity is low: The probability of producing a photon is ∼ 10 −2 / interface. To build up a detectable signal, one typically allows the particle to pass through a periodic stack of several hundred or thousand foils of fixed thickness each separated by a fixed spacing of gas or vacuum [13,14]. If the field amplitudes at each interface are added in phase, it can be shown that the result is an interference pattern, with peaks appearing at frequencies governed by a resonance condition determined by the foil thickness l 1 and spacing l 2 [15,16,17,18].…”
Section: Introductionmentioning
confidence: 99%
“…Transition radiation (TR) is emitted when a relativistic particle passes through the interface between two media [1]. The emission has a conical shape with a maximum intensity at an angle yffi1/g, with respect to the direction of the incident particle, and half-intensity angle of Dyffiyffi1/g, where g ¼ (1Àv 2 /c 2 ) À1/2 is the relativistic factor [2].…”
Section: Introductionmentioning
confidence: 99%