Doping dependence of the electron–phonon and electron–spin fluctuation interactions in the high-Tc superconductor Bi2Sr2CaCu2O8+δ

Using ultrafast optical techniques, we detect two types of bosons strongly coupled to electrons in the family of Bi _2 Sr _2 CaCu _2 O _8+ _δ (Bi-2212) from the underdoped to overdoped regimes. The different doping dependences of the electron–boson coupling strengths enable us to identify them as ph...

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Main Authors: E E M Chia, D Springer, S K Nair, X Q Zou, S A Cheong, C Panagopoulos, T Tamegai, H Eisaki, S Ishida, S Uchida, A J Taylor, J-X Zhu
Format: Article
Language:English
Published: IOP Publishing 2013-01-01
Series:New Journal of Physics
Online Access:https://doi.org/10.1088/1367-2630/15/10/103027
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author E E M Chia
D Springer
S K Nair
X Q Zou
S A Cheong
C Panagopoulos
T Tamegai
H Eisaki
S Ishida
S Uchida
A J Taylor
J-X Zhu
author_facet E E M Chia
D Springer
S K Nair
X Q Zou
S A Cheong
C Panagopoulos
T Tamegai
H Eisaki
S Ishida
S Uchida
A J Taylor
J-X Zhu
author_sort E E M Chia
collection DOAJ
description Using ultrafast optical techniques, we detect two types of bosons strongly coupled to electrons in the family of Bi _2 Sr _2 CaCu _2 O _8+ _δ (Bi-2212) from the underdoped to overdoped regimes. The different doping dependences of the electron–boson coupling strengths enable us to identify them as phonons and spin fluctuations: electron–phonon coupling ( λ _e−ph ) peaks at optimal doping, while electron–spin fluctuation coupling ( λ _e−sf ) decreases monotonically with doping. This observation is consistent with two facts: (i) superconductivity is in close proximity with antiferromagnetism at low dopings and (ii) a pronounced lattice renormalization effect at larger dopings.
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spelling doaj.art-c763d8c8851a49749d7baf4a0f4993722023-08-08T11:04:11ZengIOP PublishingNew Journal of Physics1367-26302013-01-01151010302710.1088/1367-2630/15/10/103027Doping dependence of the electron–phonon and electron–spin fluctuation interactions in the high-Tc superconductor Bi2Sr2CaCu2O8+δE E M Chia0D Springer1S K Nair2X Q Zou3S A Cheong4C Panagopoulos5T Tamegai6H Eisaki7S Ishida8S Uchida9A J Taylor10J-X Zhu11Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University , Singapore 637371, SingaporeDivision of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University , Singapore 637371, SingaporeDivision of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University , Singapore 637371, SingaporeDivision of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University , Singapore 637371, SingaporeDivision of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University , Singapore 637371, SingaporeDivision of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University , Singapore 637371, Singapore; Department of Physics, University of Crete and FORTH , 71003 Heraklion, GreeceDepartment of Applied Physics, University of Tokyo , Hongo, Bunkyo-ku, Tokyo 113-8656, JapanNational Institute of Advanced Industrial Science and Technology , Tsukuba 305-8568, JapanDepartment of Physics, University of Tokyo , Bunkyo-ku, Tokyo 113-0033, JapanDepartment of Physics, University of Tokyo , Bunkyo-ku, Tokyo 113-0033, JapanMaterials Physics and Applications Division, Los Alamos National Laboratory, Los Alamos, NM 87545, USATheoretical Division and Center for Integrated Nanotechnologies, Los Alamos National Laboratory, Los Alamos, NM 87545, USAUsing ultrafast optical techniques, we detect two types of bosons strongly coupled to electrons in the family of Bi _2 Sr _2 CaCu _2 O _8+ _δ (Bi-2212) from the underdoped to overdoped regimes. The different doping dependences of the electron–boson coupling strengths enable us to identify them as phonons and spin fluctuations: electron–phonon coupling ( λ _e−ph ) peaks at optimal doping, while electron–spin fluctuation coupling ( λ _e−sf ) decreases monotonically with doping. This observation is consistent with two facts: (i) superconductivity is in close proximity with antiferromagnetism at low dopings and (ii) a pronounced lattice renormalization effect at larger dopings.https://doi.org/10.1088/1367-2630/15/10/103027
spellingShingle E E M Chia
D Springer
S K Nair
X Q Zou
S A Cheong
C Panagopoulos
T Tamegai
H Eisaki
S Ishida
S Uchida
A J Taylor
J-X Zhu
Doping dependence of the electron–phonon and electron–spin fluctuation interactions in the high-Tc superconductor Bi2Sr2CaCu2O8+δ
New Journal of Physics
title Doping dependence of the electron–phonon and electron–spin fluctuation interactions in the high-Tc superconductor Bi2Sr2CaCu2O8+δ
title_full Doping dependence of the electron–phonon and electron–spin fluctuation interactions in the high-Tc superconductor Bi2Sr2CaCu2O8+δ
title_fullStr Doping dependence of the electron–phonon and electron–spin fluctuation interactions in the high-Tc superconductor Bi2Sr2CaCu2O8+δ
title_full_unstemmed Doping dependence of the electron–phonon and electron–spin fluctuation interactions in the high-Tc superconductor Bi2Sr2CaCu2O8+δ
title_short Doping dependence of the electron–phonon and electron–spin fluctuation interactions in the high-Tc superconductor Bi2Sr2CaCu2O8+δ
title_sort doping dependence of the electron phonon and electron spin fluctuation interactions in the high tc superconductor bi2sr2cacu2o8 δ
url https://doi.org/10.1088/1367-2630/15/10/103027
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