1988
DOI: 10.1103/physrevb.38.4352
|View full text |Cite
|
Sign up to set email alerts
|

Planar channeling radiation from 54110-MeV electrons in diamond and silicon

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
13
0

Year Published

1991
1991
2015
2015

Publication Types

Select...
8

Relationship

1
7

Authors

Journals

citations
Cited by 38 publications
(13 citation statements)
references
References 13 publications
0
13
0
Order By: Relevance
“…The consequence of this study was that we had to design a set-up able to do very small momentum steps (10 −3 ) without changing the geometrical characteristics of the electron beam. The experiment was performed during a part of the time allocated to the study of the "planar channelling radiation from 54 to 110 MeV electrons in diamond and silicon" [6] at the Accélérateur Linéaire de Saclay (ALS). The 1-μm thick silicon crystal (lattice constant 5.431 Å) was aligned along the 110 direction (inter-atomic distance along the row d = 3.84 Å).…”
mentioning
confidence: 99%
“…The consequence of this study was that we had to design a set-up able to do very small momentum steps (10 −3 ) without changing the geometrical characteristics of the electron beam. The experiment was performed during a part of the time allocated to the study of the "planar channelling radiation from 54 to 110 MeV electrons in diamond and silicon" [6] at the Accélérateur Linéaire de Saclay (ALS). The 1-μm thick silicon crystal (lattice constant 5.431 Å) was aligned along the 110 direction (inter-atomic distance along the row d = 3.84 Å).…”
mentioning
confidence: 99%
“…10, curves 1 and 2). Additional peaks of radiation were choosed with intensities and widths similar to the experimental data in [1][2][3][4]. Additional radiation peaks are clearly observed; the spectrum retains its structure.…”
Section: Energy Distribution Of Low Energy Radiation With Measurementmentioning
confidence: 99%
“…When crystalline targets are used, characteristic peaks arise induced by radiation upon channeling [1][2][3][4] and coherent bremsstrahlung [5,6], in the background of usual bremsstrahlung.…”
Section: Introductionmentioning
confidence: 99%
“…Equation (16) Nevertheless, Eq. (16) has something to tell in CBR : when ψ increases the CBR spectral peaks move together toward larger ω, while the energies under the peaks remain constant [22]. Thus the total CBR energy does not depend on ψ.…”
Section: Classical Radiationmentioning
confidence: 99%