2017
DOI: 10.1103/physrevlett.119.024801
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Observation of Quasichanneling Oscillations

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Cited by 23 publications
(33 citation statements)
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“…This simulation code is developed for ab-initio Monte Carlo simulations of charged particle trajectories in an interplanar or interaxial potential in a crystalline medium (either bent or not) with both multiple and single scattering on nuclei and electrons. The method developed by the code has already been tested vs. experimental results in [11,12,13,15,47]. The perfect alignment with bent planes, i.e., θ cr = 0, was experimentally determined by the highest intensity of the channeling peak, recorded during the angular scan.…”
Section: Experimental Results and Analysismentioning
confidence: 99%
“…This simulation code is developed for ab-initio Monte Carlo simulations of charged particle trajectories in an interplanar or interaxial potential in a crystalline medium (either bent or not) with both multiple and single scattering on nuclei and electrons. The method developed by the code has already been tested vs. experimental results in [11,12,13,15,47]. The perfect alignment with bent planes, i.e., θ cr = 0, was experimentally determined by the highest intensity of the channeling peak, recorded during the angular scan.…”
Section: Experimental Results and Analysismentioning
confidence: 99%
“…Such a simple dependence on k 0 disappears when the conditions (25), (29), and (33) become violated. In particular, when one considers the reflection of ultrarelativistic electrons (or positrons) from a crystal (see, e.g., [45][46][47][48][49][50][51][52][69][70][71][72]), the trajectory of the particle can be replaced by (30) in evaluating the radiation of twisted photons provided that the photon energy satisfies the estimate…”
Section: Trajectories With a Break On The Detector Axismentioning
confidence: 99%
“…Even larger K can be achieved not for the volume reflected but for the volume captured electrons in a bent crystal (see, e.g., [46,47,[49][50][51][52]). For the processes we consider, the twisted photons with large total angular momentum can be generated only when q → 1.…”
Section: Trajectories With a Break On The Detector Axismentioning
confidence: 99%
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“…2 an image of the YAG screen is shown for the aligned orientation where the beam hits the crystal parallel to the plane at the crystal entrance face. The almost circular light peak to the right in the image originates from the channeled particles, near which the so-called quasi-channeling oscillations can be seen [12], and to the left is seen the volume reflected particles and/or the fraction of particles that is not channeled due to the finite beam divergence and its surface transmission. After identifying the direction of the plane, we switched to the secondary beam which has a significantly higher divergence of around σ ≈ 75 μrad.…”
Section: Methodsmentioning
confidence: 99%