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Title: Spectroscopic measurement of H(1S) and H sub 2 (v double prime ,J double prime ) in an H sup minus ion source plasma

Abstract

Low pressure H{sub 2} discharges have been used for some time as sources of H{sup {minus}} ions. These discharges contain many different species of particles which interact with each other and with the walls of the discharge chamber. Models exist that predict the populations of the various species for given macroscopic discharge parameters. However, many of the cross sections and wall catalyzation coefficients are unknown or somewhat uncertain. Therefore, it is of interest to measure the populations of as many of these species as possible, in order to determine the validity of the models. These models predict that H{sup {minus}} is created predominantly by the two-step process of vibrational excitation of hydrogen molecules followed by dissociative attachment of slow electrons to these vibrationally-excited hydrogen molecules. Many different collisional processes must be included in the models to explain the dependence of the various populations upon macroscopic parameters. This work presents results of spectroscopic measurements of the density and translational temperature of hydrogen atoms and of specific rotationally- and vibrationally-excited states of electronic ground-state H{sub 2}, in a discharge optimized for H{sup {minus}} production, as well as conventional measurements of the various charged species within the plasma. The spectroscopic measurements are performedmore » directly by narrowband, single-photon absorption in the vacuum ultraviolet.« less

Authors:
Publication Date:
Research Org.:
Lawrence Berkeley Lab., CA (USA)
Sponsoring Org.:
USDOE; USDOE, Washington, DC (USA)
OSTI Identifier:
5836451
Report Number(s):
LBL-30541
ON: DE91011879
DOE Contract Number:
AC03-76SF00098
Resource Type:
Technical Report
Resource Relation:
Other Information: Thesis (Ph.D.)
Country of Publication:
United States
Language:
English
Subject:
74 ATOMIC AND MOLECULAR PHYSICS; HYDROGEN; ABSORPTION SPECTROSCOPY; DISSOCIATION; EXPERIMENTAL DATA; HYDROGEN IONS 1 MINUS; HYSTERESIS; ION SOURCES; MOLECULES; ULTRAVIOLET SPECTRA; VIBRATIONAL STATES; ANIONS; CHARGED PARTICLES; DATA; ELEMENTS; ENERGY LEVELS; EXCITED STATES; HYDROGEN IONS; INFORMATION; IONS; NONMETALS; NUMERICAL DATA; SPECTRA; SPECTROSCOPY; 640302* - Atomic, Molecular & Chemical Physics- Atomic & Molecular Properties & Theory

Citation Formats

Stutzin, G.C. Spectroscopic measurement of H(1S) and H sub 2 (v double prime ,J double prime ) in an H sup minus ion source plasma. United States: N. p., 1990. Web. doi:10.2172/5836451.
Stutzin, G.C. Spectroscopic measurement of H(1S) and H sub 2 (v double prime ,J double prime ) in an H sup minus ion source plasma. United States. doi:10.2172/5836451.
Stutzin, G.C. Wed . "Spectroscopic measurement of H(1S) and H sub 2 (v double prime ,J double prime ) in an H sup minus ion source plasma". United States. doi:10.2172/5836451. https://www.osti.gov/servlets/purl/5836451.
@article{osti_5836451,
title = {Spectroscopic measurement of H(1S) and H sub 2 (v double prime ,J double prime ) in an H sup minus ion source plasma},
author = {Stutzin, G.C.},
abstractNote = {Low pressure H{sub 2} discharges have been used for some time as sources of H{sup {minus}} ions. These discharges contain many different species of particles which interact with each other and with the walls of the discharge chamber. Models exist that predict the populations of the various species for given macroscopic discharge parameters. However, many of the cross sections and wall catalyzation coefficients are unknown or somewhat uncertain. Therefore, it is of interest to measure the populations of as many of these species as possible, in order to determine the validity of the models. These models predict that H{sup {minus}} is created predominantly by the two-step process of vibrational excitation of hydrogen molecules followed by dissociative attachment of slow electrons to these vibrationally-excited hydrogen molecules. Many different collisional processes must be included in the models to explain the dependence of the various populations upon macroscopic parameters. This work presents results of spectroscopic measurements of the density and translational temperature of hydrogen atoms and of specific rotationally- and vibrationally-excited states of electronic ground-state H{sub 2}, in a discharge optimized for H{sup {minus}} production, as well as conventional measurements of the various charged species within the plasma. The spectroscopic measurements are performed directly by narrowband, single-photon absorption in the vacuum ultraviolet.},
doi = {10.2172/5836451},
journal = {},
number = ,
volume = ,
place = {United States},
year = {Wed Aug 01 00:00:00 EDT 1990},
month = {Wed Aug 01 00:00:00 EDT 1990}
}

Technical Report:

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  • To check the adequacy and develop the theoretical models used in a semiempirical determination of the probabilities of rovibronic transitions, it is proposed to carry out a comparative optimization analysis of experimental data on the relative probabilities and radiative lifetimes of two or more isotopes. A program package has been developed for a semiempirical determination of an entire matrix set of probabilities of vibronic radiative transitions that makes it possible to conduct a study of the adequacy of a theoretical model (adiabatic approximation and type of approximation of the electron moment as a function of internuclear distance {ital M}{sup ({italmore » r})}{sub {ital n}{prime}{ital n}{double prime}}) and to check the stability and uniqueness of the solution of the inverse problem of semiempirical determination of {ital M}{sub {ital n}{prime}{ital n}{double prime}} ({ital r}). For the first time the relative probabilities of {ital d}{sup 3}{Pi}{sup {minus}}{sub {ital u}}, {ital v}{prime}, {ital N}{r arrow}{ital a}{sup 3}{Sigma}{sup +}{sub {ital g}}, {ital v}{double prime}, {ital N} of spontaneous emission of the D{sub 2} molecule have been measured, and new data on the same transitions in H{sub 2} have been obtained. It was found that the isotope effect in the probabilities of the indicated transitions of the hydrogen molecule is adequately described within the limits of experimental accuracy in the framework of the adiabatic approximation.« less
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  • Molecular vibrational excitation generated by recombination of molecular ions on barium electrode surfaces is presented. Negative hydrogen ion formation by vibrationally excited molecules rebounding from the surface is also calculated (AIP).
  • The recombination and dissociation of H{sup +}{sub 2} and H{sup +}{sub 3} ions incident upon metal surfaces leads to H, H{sub 2}({ital v}{double prime}), and H{sup {minus}} products rebounding from the surface. A four-step model for H{sup +}{sub 2} -ion recombination generates H{sub 2}({ital v}{double prime}) via resonant electron capture through the {ital b} {sup 3}{Sigma}{sup +}{sub {ital u}} and {ital X} {sup 1}{Sigma}{sup +}{sub {ital g}} states. A molecular trajectory analysis provides final-state H{sub 2}({ital v}{double prime}) distributions for incident energies of 1, 4, 10, and 20 eV. The calculated H{sub 2}:H{sup +}{sub 2} yields compare favorably with themore » observed yields. A similar four-step model for incident H{sup +}{sub 3} proceeds via resonant capture to form the H{sub 3}(2{ital p} {sup 2}{ital E}{prime}{r arrow}2{ital p} {sup 2}{ital A}{sub 1}) ground state, in turn dissociating into H+H{sub 2}({ital v}{double prime}), with the fragment molecule rebounding to give the final H{sub 2}({ital v}{double prime}) distribution. Comparing the final populations {ital v}{double prime}{ge}5 for incident H{sup +}{sub 2} or H{sup +}{sub 3} shows that the H{sup +}{sub 3} ion will be more useful than H{sup +}{sub 2} for H{sup {minus}} generation via dissociative attachment. Molecular ions incident upon low-work-function surfaces generate additional H{sub 2}({ital v}{double prime}) via resonant electron capture through excited electronic states and provide two additional sources of H{sup {minus}} production: Direct H{sup {minus}} production by H dissociation products rebounding from the surface and H{sup {minus}} production through the formation of H{sup {minus}}{sub 2} in the surface selvage that in turn dissociates into H+H{sup {minus}}.« less
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