1919
DOI: 10.1002/andp.19193630702
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Über die Verbreiterung von Spektrallinien

Abstract: B 7. ANNALEN DER PHYSIK. VIEB!CE FOME. BAND 58. 1. Uber d4e Vsr6rdtgluumg von S'elctraEUrvlm; urn J. HoEtsrnark. 1) Chr. Fiichtbauer und W. Hoffinann, Ann. d. Pbys. 43. 2) J. Stark, Elektrieche Spektrslanalyse chemiacher Atomc. p. 96. 1914. Leipzig 1914.#ber die Verbreiterung von Spektrallinien.

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Cited by 524 publications
(252 citation statements)
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“…Here we present a statistical technique for deriving the spectrum of random fluctuations of the combined force and tidal fields generated by statistical ensembles of extended substructures with known mass and size functions. Our work follows up the method originally devised by Holtsmark (1919) to study the motion of charged particles in an ionized plasma.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…Here we present a statistical technique for deriving the spectrum of random fluctuations of the combined force and tidal fields generated by statistical ensembles of extended substructures with known mass and size functions. Our work follows up the method originally devised by Holtsmark (1919) to study the motion of charged particles in an ionized plasma.…”
Section: Discussionmentioning
confidence: 99%
“…To attack this problem we shall follow a statistical method originally introduced by Holtsmark (1919) to describe the motion of charged particles in a plasma.…”
Section: Stochastic Fluctuations Of the Fieldmentioning
confidence: 99%
“…This is very nearly equal to the field produced by an ion of charge p which is at a mean ion-ion distance r~ = (1~i iN~I3 Y~' 3 from the perturbed ion , Since in a neutral plasma containing , e.g., only a single ion species , the electron density ie related to the ion density by N = the electronic Holtsmark field F 0 -2.603eN~'~~ (2) 0 is related to that produced by ions by p ~~' 3 F~.…”
Section: IXmentioning
confidence: 95%
“…Electron broadening in the impact approximation results in a pure Lorentzian wing decay, assuming random collisions, whereas a somewhat faster decay is typically observed due to the influence of the ion microfields (see [17] or [18] for details). For the Holtsmark microfield distribution function [19] the wing decay is ∝ ∆λ −5/2 . To obtain the FWHM for transitions with a shift in the central component (e.g., Ba-β (n=4→2), Pa-β (n=5→3)) the line fitting model consists of one central and two shifted modified Lorentzian components in order to resolve the central dip, as shown in Figure 1 (left).…”
Section: Line Profile Modelmentioning
confidence: 99%