2012
DOI: 10.3788/hplpb20122406.1287
|View full text |Cite
|
Sign up to set email alerts
|

Characteristics of high-power all-fiber laser

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
2
0

Year Published

2012
2012
2013
2013

Publication Types

Select...
2

Relationship

0
2

Authors

Journals

citations
Cited by 2 publications
(2 citation statements)
references
References 0 publications
0
2
0
Order By: Relevance
“…For simulation, the heavy ion beams are injected first into CSRm for the accumulation with e-cooling [6] and then the injected beams are accelerated. It is assumed that an initial momentum spread Δp/p after accelerating is 5×10 −4 and the bunch pulse length is about 472 ns with 200 MeV/u from Table 1, which is too long for optimal target heating, and has to be shortened by a factor of 10 or more.…”
Section: Beam Dynamics Simulation During Bunch Compressionmentioning
confidence: 99%
“…For simulation, the heavy ion beams are injected first into CSRm for the accumulation with e-cooling [6] and then the injected beams are accelerated. It is assumed that an initial momentum spread Δp/p after accelerating is 5×10 −4 and the bunch pulse length is about 472 ns with 200 MeV/u from Table 1, which is too long for optimal target heating, and has to be shortened by a factor of 10 or more.…”
Section: Beam Dynamics Simulation During Bunch Compressionmentioning
confidence: 99%
“…Table 1 shows the parameters of CSRm. The heavy ion beams are injected first into the CSRm for the accumulation with e-cooling [6] and then are accelerated. The accelerated beam can be compressed longitudinally.…”
Section: Beam Dynamics Simulation For Bunch Compression In Csrmmentioning
confidence: 99%