1987
DOI: 10.1016/s0022-3093(87)80270-3
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The influence of the structure of different arsenic chalcogenide glasses on the dispersion parameters of a sellmeier and a Lorentz-Lorenz relation

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Cited by 7 publications
(2 citation statements)
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“…The refractive index dispersion in the visible region was expressed by the Lorentz–Lorenz‐type dispersion formula 17 :n2+2n21=3πmc2e2Nf1λ021λ2where, n denotes the refractive index at a wavelength of λ ; m , the electron mass; c , the velocity of light; e , the elementary charge; N , the number of oscillators in a unit volume; f , the average oscillator strength; and λ 0 , the inherent absorption wavelength or average resonance wavelength of the oscillator. Based on this model, the plot of 1/( n 2 − 1) versus 1/ λ 2 was expected to be a straight line with a slope of − πmc 2 / e 2 Nf , and a y ‐axis intercept given by πmc 2 / e 2 Nfλ 0 2 − 1/3.…”
Section: Resultsmentioning
confidence: 99%
“…The refractive index dispersion in the visible region was expressed by the Lorentz–Lorenz‐type dispersion formula 17 :n2+2n21=3πmc2e2Nf1λ021λ2where, n denotes the refractive index at a wavelength of λ ; m , the electron mass; c , the velocity of light; e , the elementary charge; N , the number of oscillators in a unit volume; f , the average oscillator strength; and λ 0 , the inherent absorption wavelength or average resonance wavelength of the oscillator. Based on this model, the plot of 1/( n 2 − 1) versus 1/ λ 2 was expected to be a straight line with a slope of − πmc 2 / e 2 Nf , and a y ‐axis intercept given by πmc 2 / e 2 Nfλ 0 2 − 1/3.…”
Section: Resultsmentioning
confidence: 99%
“…В даному випадку слово «резонанси» взято у лапки тому, що коефіцієнти у формулі (5) визначаються за результатами вимірювань методом підгонки [2,4], а тому обчислені довжини хвиль k l не обов'язково співпадають з будьякими довжинами хвиль атомних або іонних резонансів. Відмітимо, що модель у формі (5) широко використовується у сучасних наукових дослідженнях [17][18][19][20].…”
Section: аналіз літературних джерелunclassified