1970
DOI: 10.1063/1.1658739
|View full text |Cite|
|
Sign up to set email alerts
|

X-Ray Production in Laser-Heated Plasmas

Abstract: The efficiency of converting focused laser radiation into kilovolt x rays by means of a high-z planar plasma has been calculated. For electron temperatures of several keV, the rapid expansion of the plasma limits the effective absorption and reradiation times to a few tenths of a nanosecond. This short time limits the fractional degree of ionization to 30%–60%, depending on the temperature, for heavy target ions such as gold, and in this case the predominant ions have ionization energies less than the electron… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
12
1
1

Year Published

1972
1972
2019
2019

Publication Types

Select...
5
3
1

Relationship

0
9

Authors

Journals

citations
Cited by 32 publications
(14 citation statements)
references
References 15 publications
0
12
1
1
Order By: Relevance
“…Actually, it can be shown that the main source of radiation is due to bound-bound processes. Bernstein and Comisar 34 give an empirical formula for evaluating the ratio of the various emitting processes. In the case of line ͑bound-bound transitions͒ versus recombination ͑free-bound transitions͒ emissions, the ratio of the radiated powers is…”
Section: Limitations Of the Modelmentioning
confidence: 99%
“…Actually, it can be shown that the main source of radiation is due to bound-bound processes. Bernstein and Comisar 34 give an empirical formula for evaluating the ratio of the various emitting processes. In the case of line ͑bound-bound transitions͒ versus recombination ͑free-bound transitions͒ emissions, the ratio of the radiated powers is…”
Section: Limitations Of the Modelmentioning
confidence: 99%
“…Next generation high-power laser systems are expected to routinely reach intensities in the I ≈ 10 22 − 10 23 W/cm 2 region [1,2,3,4]. In a configuration where such an intense pulse interacts with a solid target, gamma rays will be generated mostly by the processes of electron-nucleus bremsstrahlung [5], and by radiation reaction effects including non-linear inverse Compton scattering (ICS) [6,7], where the fast electrons scatter on the high field of the laser pulse itself [8]. In this paper, we present a study of the latter process, relevant especially at the higher end of the considered intensity range, where the radiation has to be treated in the context of quantum electrodynamics (QED), with the further outlook of even higher intensities which would exhibit additional important effects such as the creation of electron-positron pairs and QED cascades [9,10,11,12,13,14,15,16].…”
Section: Introductionmentioning
confidence: 99%
“…As a result of the interaction of nanosecond pulses of laser radiation with matter, for power densities of radiation higher that 10 12 Wcm~2, a high-temperature plasma is produced with a maximum temperature of the order of 10 6 K (a laser plasma) that is an intensive source of soft X rays, including the low-energy part of a spectrum with the photon energy around 1 keV (Bernstein & Comisar 1970;Colombant & Tonon 1973;Nagel et al 1974). For this reason a laser-produced plasma is used in the systems of laser plasma X-ray sources (Wallis 1980;Key 1984;Nagel 1986;Gerritsen etal.…”
Section: Introductionmentioning
confidence: 99%