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Optical Properties of the Cu-O Plane in the Bi2Sr2-xLaxCuO6 Family (Articolo in rivista)
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- Optical Properties of the Cu-O Plane in the Bi2Sr2-xLaxCuO6 Family (Articolo in rivista) (literal)
- Anno
- 2013-01-01T00:00:00+01:00 (literal)
- Http://www.cnr.it/ontology/cnr/pubblicazioni.owl#doi
- 10.1007/s10948-012-2055-6 (literal)
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- D. Nicoletti (1) P. Calvani (1) P. Di Pietro (1) O. Limaj (2) U. Schade (3) S. Ono (4)Yoichi Ando (5) S. Lupi (2) (literal)
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- 1. CNR-SPIN and Dipartimento di Fisica, Università di Roma La Sapienza, Piazzale A. Moro 2, 00185, Rome, Italy
2. CNR-IOM and Dipartimento di Fisica, Università di Roma La Sapienza, Piazzale A. Moro 2, 00185, Rome, Italy
3. Elektronenspeicherring BESSY 2, Helmholtz Zentrum Berlin Mat & Energie GmbH, 12489, Berlin, Germany
4. Central Research Institute of Electric Power Industry, Komae, Tokyo, 201-8511, Japan
5. Institute of Scientific and Industrial Research, Osaka University, Ibaraki, Osaka, 567-0047, Japan (literal)
- Titolo
- Optical Properties of the Cu-O Plane in the Bi2Sr2-xLaxCuO6 Family (literal)
- Abstract
- The ab-plane optical conductivity of seven single crystals, belonging to the family Bi2Sr2-x La x CuO6, has been measured for hole concentrations per Cu site 0.03<=p<=0.18, and for 6 K<=T<=300 K (500 K for p=0.16). At low doping, ten phonon lines are detected, which are due to the removal of the degeneracy of five E u modes (out of the predicted six). They are superimposed to a far-infrared band, which as doping increases, closes the insulating gap thus building up the Drude term. The insulator-to-metal transition occurs between p=0.7 and p=0.10 consistently with a Mott mechanism. In the metallic phase, a multiband analysis identifies a Drude term plus a mid-infrared band, which weakly depends on temperature and softens as p increases, like in other cuprates. The optical response of the crystal at optimum doping has been analyzed also in the superconducting phase. The Ferrel-Glover-Tinkham sum rule requires an integration up to ?>>6? and the penetration depth is 290 nm. The bosonic spectral function includes a strong peak around 50 meV, which survives up to 500 K and, therefore, might be assigned to an electron-phonon interaction. (literal)
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