1969
DOI: 10.1016/0038-1098(69)90681-4
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The influence of phonons and polarons on the infrared absorption of cadmium oxide

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1971
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Cited by 45 publications
(20 citation statements)
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“…, in good agreement with the calculated [19] value of 267 cm À1 and with the experimental [20] one of 262 cm…”
supporting
confidence: 88%
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“…, in good agreement with the calculated [19] value of 267 cm À1 and with the experimental [20] one of 262 cm…”
supporting
confidence: 88%
“…, in good agreement with the calculated [19] value of 431 cm À1 , but lower than the experimental value of 523 cm À1 derived from the infrared measurements [20]. The PPDOS is characterized by four well-separated regions that are distinguished corresponding to transverse acoustic (TA), longitudinal acoustic (LA), TO, and longitudinal optic (LO) modes.…”
supporting
confidence: 60%
“…This plasmon-phonon peak shifts to higher frequencies with increasing density, such that a double peak structure can appear in the 3D many-polaron optical absorption spectrum, consistent with the observed bimodal polaronic band in cadmium oxide. 38 As a first application of the method presented here, we chose to investigate the optical absorption of the interacting polaron gas in the RPA framework. For Nd 2 CuO 4Ϫ␦ (␦ Ͻ0.004), similarities were observed ͑see Fig.…”
Section: Discussionmentioning
confidence: 99%
“…Using a band edge effective mass of m * = 0.24m 0 and ε(∞) = 5.4 [13,32], a plasmon energy of E p = 245 meV for the annealed sample gives a carrier density of n = 5.9 × 10 19 cm −3 , whereas E p = 460 meV for the asgrown sample gives n = 2.5 × 10 20 cm −3 . The agreement with Hall measurement is excellent for the high carrier concentration sample, illustrating HAXPES bulk sensitivity, and suggests there is no significant contribution of extra carrier density from an electron accumulation layer.…”
Section: Core Levelsmentioning
confidence: 99%