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Photoinduced self-localized structural distortions in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">Y</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Ba</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Cu</mml:mi></mml:mrow><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mrow><mml:mn>7</mml:mn><mml:mo>−</mml:mo><mml:mi>δ</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>

Y. H. KimDepartment of Physics, Institute for Polymers and Organic Solids, University of California, Santa Barbara, Santa Barbara, California 93106Christopher FosterDepartment of Physics, Institute for Polymers and Organic Solids, University of California, Santa Barbara, Santa Barbara, California 93106Alan J. HeegerDepartment of Physics, Institute for Polymers and Organic Solids, University of California, Santa Barbara, Santa Barbara, California 93106S. D. CoxDepartment of Physics, Institute for Polymers and Organic Solids, University of California, Santa Barbara, Santa Barbara, California 93106Galen D. StuckyDepartment of Physics, Institute for Polymers and Organic Solids, University of California, Santa Barbara, Santa Barbara, California 93106
1988lv
ABI

Аннотация

Photoinduced absorption measurements of $\mathrm{Y}{\mathrm{Ba}}_{2}{\mathrm{Cu}}_{3}{\mathrm{O}}_{7\ensuremath{-}\ensuremath{\delta}}$ ($\ensuremath{\delta}=0.75$) from 150 to 4000 ${\mathrm{cm}}^{\ensuremath{-}1}$ are reported. We observed photoinduced infrared-active vibrational modes, associated phonon bleachings, and an electronic transition from a self-localized gap state. The results indicate a local tetragonal to orthorhombic distortion around the charge carriers. The dynamic mass associated with the distortion is smaller in $\mathrm{Y}{\mathrm{Ba}}_{2}{\mathrm{Cu}}_{3}{\mathrm{O}}_{7\ensuremath{-}\ensuremath{\delta}}$ than in ${\mathrm{La}}_{2}$Cu${\mathrm{O}}_{4}$. The photoinduced structural distortion and the associated self-localized gap state demonstrate that the photoexcitations are polarons or bipolarons. Since these photoinduced absorption features are not observed in the isostructural compound ${\mathrm{La}}_{2}$Ni${\mathrm{O}}_{4}$ we conclude that polaron (or bipolaron) formation may play an important role in the high-temperature superconductivity.

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