Instantaneous determination of atomic line profiles by a rapid-frequency-scan dye laser

1986 ◽  
Author(s):  
Mitsuo Maeda ◽  
Chikahisa Honda ◽  
Katsunori Muraoka ◽  
Masanori Akazaki
Keyword(s):  
Dye Laser ◽  
Atomic Line ◽  
Line Profiles ◽  
Frequency Scan

Resolution enhancement of ¯pHe^+ atomic line profiles measured with a pulsed dye laser and a Fizeau wavelength meter

2003 ◽  
Vol 28 (24) ◽  
pp. 2479 ◽  
Author(s):  
Masaki Hori ◽  
Ryugo S. Hayano ◽  
Eberhard Widmann ◽  
Hiroyuki A. Torii
Keyword(s):  
Resolution Enhancement ◽  
Dye Laser ◽  
Pulsed Dye Laser ◽  
Atomic Line ◽  
Line Profiles

Determination of velocity distribution of metallic atoms in plasma devices with a rapid-frequency-scan dye laser

1984 ◽  
Vol 33 (3) ◽  
pp. 171-177 ◽  
Author(s):  
C. Honda ◽  
M. Maeda ◽  
K. Nishimura ◽  
K. Muraoka ◽  
M. Akazaki
Keyword(s):  
Velocity Distribution ◽  
Dye Laser ◽  
Frequency Scan

Quantum Resonances: Line Profiles and Dynamics

2003 ◽  
Vol 68 (3) ◽  
pp. 529-553 ◽  
Author(s):  
Ivana Paidarová ◽  
Philippe Durand
Keyword(s):  
Hydrogen Atom ◽  
Operator Theory ◽  
Quantum Dynamics ◽  
Line Profiles ◽  
Static Electric Field ◽  
Reversal Effect ◽  
Quantum Resonances ◽  
Energy Dependent ◽  
Effective Hamiltonians

The wave operator theory of quantum dynamics is reviewed and applied to the study of line profiles and to the determination of the dynamics of interacting resonances. Energy-dependent and energy-independent effective Hamiltonians are investigated. The q-reversal effect in spectroscopy is interpreted in terms of interfering Fano profiles. The dynamics of an hydrogen atom subjected to a strong static electric field is revisited.

Fluorescence Determination of Low Formaldehyde Concentrations in Air by Dye Laser Excitation

1975 ◽  
Vol 14 (2) ◽  
pp. 310 ◽  
Author(s):  
K. H. Becker ◽  
U. Schurath ◽  
T. Tatarczyk
Keyword(s):  
Laser Excitation ◽  
Dye Laser ◽  
Fluorescence Determination

Evaluation Methods of Line Profiles

2014 ◽  
pp. 171-211
Keyword(s):  
Fourier Transforms ◽  
Qualitative Assessment ◽  
Peak Width ◽  
Line Profiles ◽  
Line Broadening ◽  
Evaluation Procedures ◽  
Fitting Procedures ◽  
Microstructure Model ◽  
Diffraction Peaks

The evaluation procedures of X-ray line profiles are overviewed in this chapter. These methods can be classified into four groups, namely (1) the most simple methods that evaluate only the breadths of diffraction peaks, (2) procedures using the Fourier-transforms of line profiles for the determination of the parameters of microstructures, (3) variance methods evaluating the restricted moments of peaks, and (4) procedures fitting the whole diffraction pattern. The crystallite size distribution and the densities of lattice defects cannot be determined from the peak width alone as the rule of summation of breadths of size, strain, and instrumental profiles depends on their shape. However, the breadth methods can be used for a qualitative assessment of the main origins of line broadening (size, dislocations, planar faults) (e.g. for checking the model of microstructure used in whole powder pattern fitting procedures). The application of Fourier and variance methods is limited if the diffraction peaks are overlapping. In the case of pattern fitting procedures, usually a microstructure model is needed for the calculation of the theoretical fitting functions. The reliability of these methods increases with increasing the number of fitted peaks.

scholarly journals Radial Velocity Profiles for Anisotropic Spherically Symmetric Clusters: An Example

1988 ◽  
Vol 126 ◽  
pp. 691-692
Author(s):  
Herwig Dejonghe
Keyword(s):  
Distribution Function ◽  
Radial Velocity ◽  
Velocity Dispersion ◽  
Mass Density ◽  
Distribution Functions ◽  
Spherically Symmetric ◽  
Line Profiles ◽  
Anisotropic Models ◽  
The Family

A 1-parameter family of anisotropic models is presented. They all satisfy the Plummer law in the mass density, but have different velocity dispersions. Moreover, the stars are not confined to a particular subset of the total accessible phase space. This family is mathematically simple enough to be explored analytically in detail. The family is rich enough though to allow for a 3-parameter generalization which illustrates that even when both the mass density and the velocity dispersion profiles are required to be the same, a degeneracy in the possible distribution functions persists. The observational consequences of the degeneracy can be studied by calculating the observable radial velocity line profiles obtained with different distribution functions. It turns out that line profiles are relatively sensitive to changes in the distribution function. They therefore can be considered to be more natural observables when a determination of the distribution function is desired.

scholarly journals Non-LTE Model Atmosphere Analysis of Central Stars

1983 ◽  
Vol 103 ◽  
pp. 343-357 ◽  
Author(s):  
R.H. Méndez ◽  
R. P. Kudritzki ◽  
K. P. Simon
Keyword(s):  
Absorption Line ◽  
Model Atmosphere ◽  
Helium Abundance ◽  
Line Profiles ◽  
Atmospheric Parameters ◽  
Central Stars

This review will be concentrated on the determination of the main atmospheric parameters (Teff, log g, helium abundance) of PN nuclei, and of other subluminous objects, by fitting the observed absorption line profiles with theoretical profiles obtained from non-LTE model atmosphere calculations.

scholarly journals Stimulated Processes in a Half-collision

1986 ◽  
Vol 5 (6) ◽  
pp. 393-406
Author(s):  
H. H. Telle
Keyword(s):  
Kinetic Energy ◽  
Quantum State ◽  
Ground State ◽  
Diatomic Molecules ◽  
Dye Laser ◽  
Interatomic Potentials ◽  
Repulsive Potential ◽  
Induced Absorption ◽  
Tunable Dye Laser

Selective photodissociation of diatomic molecules is used to prepare the separating species in a well defined quantum state with narrowly determined final kinetic energy of the particles. During the course of separation to products the repulsive potential is probed by a tunable dye laser, that is by induced absorption in case the dissociation proceeds on a potential leading to ground state products, or by induced emission or absorption for all other cases. The determination of interatomic potentials from the observed spectra is discussed.

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