1994
DOI: 10.1103/physrevlett.72.2403
|View full text |Cite
|
Sign up to set email alerts
|

Experimental demonstration of dynamic focusing of a relativistic electron bunch by an overdense plasma lens

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

1
34
0

Year Published

1995
1995
2023
2023

Publication Types

Select...
6
1

Relationship

1
6

Authors

Journals

citations
Cited by 70 publications
(36 citation statements)
references
References 15 publications
1
34
0
Order By: Relevance
“…Angeles [12] which confirm the theory of the beam-plasma interaction. All three experiments were limited to the overdense plasma lens regime (n p > n b ), with plasma electron densities of order 10 11 cm -3 to 10 13 cm -3 .…”
Section: Previous Plasma Lens Experimentssupporting
confidence: 73%
See 1 more Smart Citation
“…Angeles [12] which confirm the theory of the beam-plasma interaction. All three experiments were limited to the overdense plasma lens regime (n p > n b ), with plasma electron densities of order 10 11 cm -3 to 10 13 cm -3 .…”
Section: Previous Plasma Lens Experimentssupporting
confidence: 73%
“…In principle, such strong fields are capable of focusing beams to very small spot sizes [2][3][4][5][6][7] and perhaps even capable of avoiding [8] the inherent (Oide) limitation [9] in discrete strong focusing. Several proof-of-principle experiments using low density particle beams have demonstrated plasma focusing [10][11][12]. Our goal is to demonstrate the effectiveness of plasma lenses in the parameter regime of interest for SLC and the next generation of high energy linear colliders.…”
Section: Introductionmentioning
confidence: 99%
“…Integrals with the products of the Bessel function, which enter in (17), are impossible in general to calculate analytically. But it is possible to carry out the approximate calculations for the case of small and large values of the arguments of the Bessel function.…”
Section: Model With Strong External Longitudinal Magnetic Fieldmentioning
confidence: 99%
“…7) f~b == 2 Yen;;~andforUCLAexperimenty == 7.5, 1~7.5cmandG~100G/cm, f~18 em which practically coincides with obtained experimental value. 17 For the FFTB experiment we get G~0 due to the factors 1/y2 and exp(-(k p O')2 /2) entered in the expression (12). The short bunches kpO' « 1 were used in the KEK-Tokyo University experiment and the field gradient G from (13) is equal G~2.4 kG/cm for conditions of this experiment.…”
Section: Fr~-2(2n) Mvowp-2: Sin(kpizi)mentioning
confidence: 99%
“…In an overdense plasma lens where n p n b , the space charge of the electron beam is fully neutralized by the plasma through the displacement of plasma electrons by the beam electrons, resulting in beam self-focusing through its own magnetic field [13][14][15][16][17]. In the underdense lens, where n p < ∼ n b , all plasma electrons are displaced by the beam electrons, and the focusing force is due to the remaining plasma ions [11,18].…”
Section: Introductionmentioning
confidence: 99%