Laser optogalvanic photodetachment spectroscopy - A new technique for studying photodetachment thresholds with application to I/-/
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Webster, C. R.↗
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The photodetachment cross-section and threshold energy of negative ions in carbon dioxide
Threshold energy and sunlight photodetachment measurements on negative carbon dioxide ions, using a 2.5 kw light pressure xenon lamp, show that: (1) Electron affinity of CO3(+) is larger than 2.7 e.V. and that an isomeric form of CO3(+) is likely an error; (2) The photodetachment cross section of CO3(-) will roughly be like a step function across the range of 4250 to 2500A, having its threshold energy at 4250A; (3) Sunlight photodetachment rate for CO3(-) is probably much smaller than elsewhere reported; and (4) The probability of having photodetached electrons re-attach to form negative ions is less than 1%. Mass identifying drift tube tests confirm that the slower ion is CO3(-), formed through the O(-) + 2CO2 yields CO3(-) + CO2 reaction.
Helmy, E. M.↗
Effect of blackbody radiation on the threshold for two-electron photodetachment of H/-/
The threshold law of the titled process, which is of the same form as that for electron-impact ionization of H, can experimentally be contaminated by simultaneous single photodetachment and Rydberg excitation of the residual atom, followed by ionization of the Rydberg atom by (room-temperature) blackbody photons. This gives a signal indistinguishable from direct double photodetachment. The correction is here calculated and shown to be finite at the double photodetachment threshold, and to have, possibly, an implication about the form of the threshold law itself. However, at room temperature its contribution is found to be small as it pertains to a recently initiated experiment at the Los Alamos Meson Physics Facility for available energies greater than a millivolt above threshold. The temperature dependence of the correction is shown to be large (k/B/T) to the 7/2; thus at higher temperatures the effect may be observable.
Temkin, A.↗
Photodetachment of electrons from phosphide ion - The electron affinity of PH2.
Measurement of the relative cross section for photodetachment of electrons from PH2(-) in the wavelength region 725 to 1020 nm (1.71 to 1.22 eV). An ion cyclotron resonance spectrometer was used to generate, trap, and detect the negative ions, and two light sources were employed to study photodetachment: a 1000-W xenon arc lamp with a grating monochromator and a continuously tunable laser. A single sharp threshold in the cross-section curve was observed, and a detailed analysis yielded an electron affinity value of 1.25 plus or minus 0.03 eV.
Smyth, K. C.↗
Photodetachment of an electron from selenide ion - The electron affinity and spin-orbit coupling constant for SeH.
The relative cross section for the gas phase photodetachment of an electron from SeH(-) was determined in the wavelength region 428 to 578 nm. An ion cyclotron resonance spectrometer was used to generate, trap, and detect the negative ions, and a 1000-W xenon arc lamp with a grating monochromator was employed as the light source. The cross section exhibited two sharp thresholds, whose positions remained unchanged for the photodetachment of SeD(-). As a result of these thresholds, the electron affinity and the spin-orbit coupling constant were evaluated.
Smyth, K. C.↗
Photodetachment of thermally relaxed CO3/-/
The CO3(-) ion is the most abundant negative ion species in the night-time D region (65-85 km above earth's surface). The absolute photodetachment cross section and the solar detachment rate of ground electronic and vibrational energy state of this ion have been determined by using an electron-detecting drift-tube method. The CO3(-) ion is identified by mass and mobility measurements and its cross section is obtained. The solar photodetachment rate is found to be 0.022. The experiment may be of interest to the modeling of the ionized atmosphere.
Hong, S. P.↗
Photodetachment cross sections of negative ions - The range of validity of the Wigner threshold law
The threshold behavior of the photodetachment cross section of negative ions as a function of photon frequency is usually described by the Wigner law. This paper reports the results of a model calculation using the zero-core-contribution (ZCC) approximation. Theoretical expressions for the leading correction to the Wigner law are developed, giving the range of validity of the Wigner law and the expected accuracy. The results are relevant to extraction of electron affinities from experimental photodetachment data.
Farley, John W.↗
Franck-Condon factors for photodetachment from LiO(-), NaO(-), and KO(-)
The 1Sigma(+), 3Sigma(+), 1Pi, and 3Pi states of the negative ions and the 2Pi and 2Sigma(+) states of the neutral alkali oxides are studied at high levels of theory. The calculations show that ground state of the negative ions changes from 3Pi for LiO(-) to 1Sigma(+) for KO(-). Although the calculations give a 3Pi ground state for NaO(-), we cannot rule out the possibility that the very low-lying 1Sigma(+) state is the true ground state. The Franck-Condon factors for photodetachment of an electron from the 1Sigma(+) and/or 3Pi states of the negative ion are presented to help interpret photodetachment experiments. Our best results for the A 2Sigma(+) - X 2Pi separations in LiO and NaO are 2496 and 2061/cm, which are in excellent agreement with that deduced (2516 and 2018/cm) from experiment.
Bauschlicher, Charles W., Jr.↗
Theoretical photodetachment cross section for the negative atomic oxygen ion
Theoretical photodetachment cross section for negative atomic oxygen ion
SCATTERING CROSS SECTION↗
Photodetachment of NO sub 2.
Photodetachment of electrons from nitrogen dioxide ions by light in violet portion of visible spectrum, noting wavelength dependence
Warneck, P.↗
Laboratory measurements of photodetachment cross sections of selected negative ions Final report, 27 Jun. 1968 - 26 Jun. 1969
Photodetachment cross sections measured for selected negative ions present in upper atmospheric D-region
Warneck, P.↗
Photodetachment energies of negative ions by ion cyclotron resonance spectroscopy - Electron affinities of neutral radicals
Ion cyclotron resonance spectroscopy technique for determining electrons photodetachment energy from negative ions in gas phase
Brauman, J. I.↗
Photodetachment of various condensed cases at low temperatures utilizing ultraviolet light
Low temperature photodetachment of carbon dioxide, ammonia, and nitrous oxide condensed gas molecules utilizing ultraviolet light
Ellmann, D. C.↗
Photodetachment of negative ions using a continuously tunable laser and an ion cyclotron resonance spectrometer
Negative ions photodetachment by continuously tunable laser and ion cyclotron resonance spectrometer
Brauman, J. I.↗
Photodetachment of electrons from amide and arsenide ions - The electron affinities of NH2., and AsH2.
The relative cross section for the gas-phase photodetachment of electrons has been determined for NH2(-) in the wavelength region of 1195 to 1695 nm and for AsH2(-) in the region from 620 to 1010 nm. An ion cyclotron resonance spectrometer was used to generate, trap, and detect negative ions. A 1000-W xenon arc lamp with a grating monochromator was used as the light source, except for one series of experiments in which a tunable laser was employed. Single sharp thresholds were observed in both cross sections, and the following electron affinity values were determined: 0.744 (plus or minus 0.022) eV for NH2. and 1.27 (plus or minus 0.03) eV for AsH2.
Smyth, K. C.↗
Electron-atom spin asymmetry and two-electron photodetachment - Addenda to the Coulomb-dipole threshold law
Temkin (1982) has derived the ionization threshold law based on a Coulomb-dipole theory of the ionization process. The present investigation is concerned with a reexamination of several aspects of the Coulomb-dipole threshold law. Attention is given to the energy scale of the logarithmic denominator, the spin-asymmetry parameter, and an estimate of alpha and the energy range of validity of the threshold law, taking into account the result of the two-electron photodetachment experiment conducted by Donahue et al. (1984).
Temkin, A.↗
Photodetachment of the positronium negative ion
The photodetachment cross section of the negative positronium ion is calculated. The description of the initial bound state is simplified by representing it by an asymptotic form whose normalization comes from the most accurate Hylleraas wave function of the ion. The final state is assumed to be a plane wave.
Bhatia, A. K.↗
The Photodetachment of Ps ion and Low-Energy e(+) -H Collisions
Two calculations in the area of positron collisions are presented. The first is the calculation of the photodetachment cross section of the positronium negative ion (Ps-) using accurate variational wave functions for both the initial bound-state and the final P continuum state. The second is the calculation of partial wave cross sections for Ps(1s)-formation in ef -H(ls) collisions using the hyperspherical hidden crossing method. Since the S-wave Stiickelberg phase is close to pi, the very small S-wave Ps(1s) formation cross section can be understood in terms of destructive interference. Other examples in positron collisions are given where it is either known or expected that destructive interference is the cause of the small S-wave Ps(1s) formation cross section. In addition, examples are presented of processes in atomic physics where the Stiickelberg phase is a multiple of pi/2.
Ward, S.J.↗