Spectroscopic distinction between the normal state pseudogap and the superconducting gap of cuprate high T_{c} superconductors

arxiv: 0705.0111 · v1 · pith:3WFGD5J2new · submitted 2007-05-01 · ❄️ cond-mat.supr-con · cond-mat.str-el

Spectroscopic distinction between the normal state pseudogap and the superconducting gap of cuprate high T_(c) superconductors

Li Yu , D. Munzar , A.V. Boris , P. Yordanov , J. Chaloupka , Th. Wolf , C.T. Lin , B. Keimer

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C. Bernhard

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classification ❄️ cond-mat.supr-con cond-mat.str-el

keywords statedifferentnormalpseudogapsuperconductingaccountbroad-bandc-axis

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We report on broad-band infrared ellipsometry measurements of the c-axis conductivity of underdoped RBa_{2}Cu_{3}O_{7-d} (R=Y, Nd, and La) single crystals. Our data provide a detailed account of the spectral weight (SW) redistributions due to the normal state pseudogap (PG) and the superconducting (SC) gap. They show that these phenomena involve different energy scales, exhibit distinct doping dependencies and thus are likely of different origin. In particular, the SW redistribution in the PG state closely resembles the one of a conventional charge- or spin density wave (CDW or SDW) system.

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Spectroscopic distinction between the normal state pseudogap and the superconducting gap of cuprate high T_(c) superconductors

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