2012
DOI: 10.1134/s1063785012030182
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Measuring coherent peaks of polarization bremsstrahlung from relativistic electrons in polycrystalline targets in backscattering geometry

Abstract: The spectra of polarization bremsstrahlung (PB) in the X- ray range induced by 7- MeV electrons in a polycrystalline copper target have been measured in the backscattering geometry for various orientations of the target relative to the electron beam. It is shown that the PB backscattering is sensitive to the texture of a target. The possibility of developing a new method based on the measurement of characteristics of the coherent PB component for the diagnostics of polycrystalline materials is consideredyesBel… Show more

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Cited by 12 publications
(9 citation statements)
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“…This behavior coincides qualitatively with the theoretical predictions of [18]. In previous works, this theory was partially validated for an isolated observation angle -π [19,21] but a dynamical approval was not performed and the evolution of the PXR characteristics was not observed.…”
Section: Resultssupporting
confidence: 84%
“…This behavior coincides qualitatively with the theoretical predictions of [18]. In previous works, this theory was partially validated for an isolated observation angle -π [19,21] but a dynamical approval was not performed and the evolution of the PXR characteristics was not observed.…”
Section: Resultssupporting
confidence: 84%
“…The presence of the characteristic radiation peaks interferes with the PB spectrum measurements near these energy values within the limits of the detector energy resolution. Previously obtained results [5][6][7][8] showed the significant contribution of the escape peak to the measured spectrum of the PB signal. The escape peak is a phantom peak presented in the measured spectrum and formed as a result of the inelastic scat tering of photons recorded by the Si detector.…”
Section: Measurementsmentioning
confidence: 99%
“…The electron beam was transported to the target 7 which was fixed into the vacuum cham ber 6 by means of three rotating magnets 4, two pairs of magnetic quadrupole lenses 5, and a corrector 6, which made it possible to focus the electron beam on the place where the target was located with a size of up to 3 mm and with a divergence of, at most, 5 mrad. These values satisfied the PB measurement conditions in the backscattering geometry, which were limited by the dimensions of the transverse cross section of the electron beam and its divergence [7][8][9]. The trans verse size, the position in the vacuum channel, and the current of the electron beam were controlled by the proportional chamber 11 and a Faraday cylinder 12.…”
Section: Introductionmentioning
confidence: 99%
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