1991
DOI: 10.1109/27.125028
|View full text |Cite
|
Sign up to set email alerts
|

Plasma physics issues in gas discharge laser development

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1

Citation Types

0
7
0

Year Published

1999
1999
2018
2018

Publication Types

Select...
5
4
1

Relationship

0
10

Authors

Journals

citations
Cited by 22 publications
(7 citation statements)
references
References 86 publications
(9 reference statements)
0
7
0
Order By: Relevance
“…This behavior indicates an increasing gain in the laser up to a pressure of 4.5 bar, due to an increased efficiency in the formation of the ArF molecule due to three-body collisions [20], [24]- [27], [29], [30] and an increased efficiency in the power deposition [31]. The intensity decrease at higher pressures is probably caused by a worse discharge quality due to the higher pressure and an increased quenching of the ArF molecules by Ne [20], [24]- [27].…”
Section: B Gas Composition 1) Optical Performance Versus F Concentramentioning
confidence: 99%
“…This behavior indicates an increasing gain in the laser up to a pressure of 4.5 bar, due to an increased efficiency in the formation of the ArF molecule due to three-body collisions [20], [24]- [27], [29], [30] and an increased efficiency in the power deposition [31]. The intensity decrease at higher pressures is probably caused by a worse discharge quality due to the higher pressure and an increased quenching of the ArF molecules by Ne [20], [24]- [27].…”
Section: B Gas Composition 1) Optical Performance Versus F Concentramentioning
confidence: 99%
“…This technique would yield a wide range of attainable temperatures and flow conditions. As compared with arc or laser powered discharge heating [1,2], non-resonant pulsed optical lattices offer the possibility to study high temperature gases without the ionization and molecular dissociation reactions associated with discharges. Traditional shock tubes, often used for high temperature flow studies [3,4], are characterized by very short interaction/probe times and significant deviations from thermal equilibrium.…”
Section: Introductionmentioning
confidence: 99%
“…External electromagnetic fields are thus often used for accelerating them, narrowing their thermal velocity distribution, also for deflecting, focussing, or keeping parallel the beam in order to transport and utilize it effectively. Charged particle beams were first used for atomic and nuclear physics, and are now also applied to plasma diagnostics, space propulsion applications, film deposition [21] and ion implantation for microelectronics, to perform precision electron beam welding, rapid cutting of thermosetting plastics, cross-linking of thermoplastics to improve their physical properties, promote or increase plasma chemical activity, to invert the population of a gas laser and give rise to light amplification (from the soft X-ray region to the far infrared) [13], to control thermonuclear reactions via plasma heating [5], to process of surface treatment and depollution of high-volume exhaust streams [13], to support externally nonself-sustained discharges, or to study stellar plasma. Some of these listed applications combine an electron beam interacting with a plasma.…”
Section: Introductionmentioning
confidence: 99%