Systematic Raman study of optical phonons in $R$Ba$_2$Cu$_3$O$_{6+\delta}$ ($R$ = Y, Dy, Gd, Sm, Nd): Antiferromagnetic coupling strength versus lattice parameters
Physical Review B 99, 094525 (2019) We present a systematic study of the interplay between lattice parameters and the energy of the optical phonons as well as the antiferromagnetic coupling strength, $J$, in the high-$T_{\text{c}}$ superconducting cuprate $R$Ba$_2$Cu$_3$O$_{6+\delta}$ (\mbox{R-123},...
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Abstract | Physical Review B 99, 094525 (2019) We present a systematic study of the interplay between lattice parameters and
the energy of the optical phonons as well as the antiferromagnetic coupling
strength, $J$, in the high-$T_{\text{c}}$ superconducting cuprate
$R$Ba$_2$Cu$_3$O$_{6+\delta}$ (\mbox{R-123}, $R =$ Y, Dy, Gd, Sm, Nd) with
hole-doping $p$ ($0.00<p \lesssim 0.04$). The energy of the $B_{1g}$-mode at
$\nu_{B1g}\approx~335$ cm$^{-1}$ has been found to relate systematically to the
inverse of the lattice parameter $a$. Our results confirm the temperature
dependent phonon splitting for Nd-123 at low doping, which has been reported
for optimally-doped Nd-123. Surprisingly, $J$ is independent of $a$ for the
first four $R$ families, and a general consistency between
$T_{\text{c}}^{\text{max}}$ and $J$, as suggested in a previous investigation,
could not be confirmed. |
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AbstractList | Physical Review B 99, 094525 (2019) We present a systematic study of the interplay between lattice parameters and
the energy of the optical phonons as well as the antiferromagnetic coupling
strength, $J$, in the high-$T_{\text{c}}$ superconducting cuprate
$R$Ba$_2$Cu$_3$O$_{6+\delta}$ (\mbox{R-123}, $R =$ Y, Dy, Gd, Sm, Nd) with
hole-doping $p$ ($0.00<p \lesssim 0.04$). The energy of the $B_{1g}$-mode at
$\nu_{B1g}\approx~335$ cm$^{-1}$ has been found to relate systematically to the
inverse of the lattice parameter $a$. Our results confirm the temperature
dependent phonon splitting for Nd-123 at low doping, which has been reported
for optimally-doped Nd-123. Surprisingly, $J$ is independent of $a$ for the
first four $R$ families, and a general consistency between
$T_{\text{c}}^{\text{max}}$ and $J$, as suggested in a previous investigation,
could not be confirmed. |
Author | Mallett, Benjamin P. P Müllner, Silvia Keren, Amit Crump, Wayne Lemmens, Peter Tallon, Jeffery L Wulferding, Dirk |
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BackLink | https://doi.org/10.1103/PhysRevB.99.094525$$DView published paper (Access to full text may be restricted) https://doi.org/10.48550/arXiv.1904.04909$$DView paper in arXiv |
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Snippet | Physical Review B 99, 094525 (2019) We present a systematic study of the interplay between lattice parameters and
the energy of the optical phonons as well as... |
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Title | Systematic Raman study of optical phonons in $R$Ba$_2$Cu$_3$O$_{6+\delta}$ ($R$ = Y, Dy, Gd, Sm, Nd): Antiferromagnetic coupling strength versus lattice parameters |
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