1916
DOI: 10.1002/andp.19163551002
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Zur Theorie der Dispersion in Gasen und Dämpfen

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Cited by 10 publications
(6 citation statements)
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“…An exact solution of this problem is hopeless; therefore, system [4] is solved approximately. 3 The absolute value of the polarization a in accordance with [5] reaches the order of magnitude of the cube of the wavelength of light X only in the immediate vicinity of precise resonance (co = co 0 ); for distances co -co 0 greater than the real line width modulus a is smaller than X 3 and then decreases rapidly. Therefore, for frequencies of incident light which are sufficiently removed from reissuance segment I can be introduced in such a manner that…”
Section: 2 Mmentioning
confidence: 97%
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“…An exact solution of this problem is hopeless; therefore, system [4] is solved approximately. 3 The absolute value of the polarization a in accordance with [5] reaches the order of magnitude of the cube of the wavelength of light X only in the immediate vicinity of precise resonance (co = co 0 ); for distances co -co 0 greater than the real line width modulus a is smaller than X 3 and then decreases rapidly. Therefore, for frequencies of incident light which are sufficiently removed from reissuance segment I can be introduced in such a manner that…”
Section: 2 Mmentioning
confidence: 97%
“…It is pointed out that in the approximate computation of integrals terms of the order of magnitude of (l/X) 3 are neglected in relation to the ones taken into account. Taking [5] into account, [24] can be expressed in the following terms to a sufficient degree of accuracy:…”
Section: Qj = A(a Z E-ikr » + Q Z T Zz E~i Kr )mentioning
confidence: 99%
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