“…2. It was shown in [51], that in the case of planar channeling the crystal bending noticeably affects the spectrum only if the condition Θ c γ ≤ 1 is met the features of ChR if L c ∝ λ (here, L c = R/γ is the formation (coherence) length of the radiation emitted from an arc of the circle of the radius R), but becomes of the quasi-synchrotron type in the opposite limit [51,271]. The latter motion gives rise to the synchrotron-type radiation, i.e.…”
Section: Fig 216mentioning
confidence: 92%
“…Right bottom a Si 1−x Ge x superlattice crystalline undulator with four periods. 3) used in recent channeling experiments [50][51][52]. Hansen, A. Nylandsted and U. Uggerhøj (University of Aarhus)) strong that they are able to steer the particles much more effectively than even the most advanced superconductive magnets.…”
Section: Why a Crystalline Undulator?mentioning
confidence: 99%
“…The phenomenon of ChR of a charged projectile in a linear crystal, see e.g. non-periodic, one-arc) bent channel [21,22,51,137,255,272,273], are known, e + e - non-periodic, one-arc) bent channel [21,22,51,137,255,272,273], are known, e + e -…”
Section: Chr In Straight and Bent Crystalsmentioning
confidence: 99%
“…To conclude this section we mention that various aspects of radiation formed in crystals bent with the constant curvature radius R were discussed in [21,22,51,137,255,272,273] although with various degree of detail.…”
“…2. It was shown in [51], that in the case of planar channeling the crystal bending noticeably affects the spectrum only if the condition Θ c γ ≤ 1 is met the features of ChR if L c ∝ λ (here, L c = R/γ is the formation (coherence) length of the radiation emitted from an arc of the circle of the radius R), but becomes of the quasi-synchrotron type in the opposite limit [51,271]. The latter motion gives rise to the synchrotron-type radiation, i.e.…”
Section: Fig 216mentioning
confidence: 92%
“…Right bottom a Si 1−x Ge x superlattice crystalline undulator with four periods. 3) used in recent channeling experiments [50][51][52]. Hansen, A. Nylandsted and U. Uggerhøj (University of Aarhus)) strong that they are able to steer the particles much more effectively than even the most advanced superconductive magnets.…”
Section: Why a Crystalline Undulator?mentioning
confidence: 99%
“…The phenomenon of ChR of a charged projectile in a linear crystal, see e.g. non-periodic, one-arc) bent channel [21,22,51,137,255,272,273], are known, e + e - non-periodic, one-arc) bent channel [21,22,51,137,255,272,273], are known, e + e -…”
Section: Chr In Straight and Bent Crystalsmentioning
confidence: 99%
“…To conclude this section we mention that various aspects of radiation formed in crystals bent with the constant curvature radius R were discussed in [21,22,51,137,255,272,273] although with various degree of detail.…”
“…Various aspects of radiation formed in crystals bent with the constant curvature radius R were discussed in Refs. [18][19][20][21][22][23][24][25] although with various degree of detail.…”
Abstract. Results of numerical simulations of electron channeling and emission spectra are reported for straight and uniformly bent silicon crystal. The projectile trajectories are computed using the newly developed module [1] of the MBN Explorer package [2,3]. The electron channeling along Si(110) crystallographic planes is studied for the projectile energy 855 MeV.
ARUTYUNOV (a), N. A. KUDRYASHOV (a), 0. A. MISHIN (a), V. M. SAMSONOV (b), M. N. STRIKHANOV (a), and Yu. A. SYTSKO (a)Expressions for the intensity of specific radiation accompanying the deflection of high-energy particles by a bent crystal are presented. It is shown that when R + cc ( R is the bending radius) the corresponding formulas are transformed into those for channeling radiation in an unbent (straight) crystal. Dipole, synchrotron-like radiation, and polarization effects are analysed. Numerical calculations of the radiation and polarization in the bent planes using a realistic potential are made for beams with different parameters.Es werden Ausdriicke fur die Intensitat von Strahlungen angegeben, die die Ablenkung von hochenergetischen Teilchen durch einen gebogenen Kristall begleiten. Fur R + co ( R ist der Biegeradius) gehen die entsprechenden Formeln in diejenigen fur Kanalstrahlung in einem nichtgebogenen Kristall iiber. Es werden Dipol-und Synchrotron-artige Strahlung sowie Polarisationseffekte untersucht.Numerische Rechnungen zu Strahlung und Polarisation unter Verwendung eines realistischen Potentials fur die gebogenen Gitterebenen werden fur Strahlen mit unterschiedlichen Parametern durchgefiihrt. ')
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