We report on magnetization measurements performed on a single crystal of
Bi2+xSr2-xCuO6+\delta with Tc\sim7 K for H||c-axis. The isofield M(T)
curves show a large reversible region, with a pronounced rounding effect as M
approaches zero which prevents the determination of Tc(H). Deviations from the
linear behavior of magnetisation near Tc(H) are studied through the asymptotic
behavior of $-M(T)\sim(T-Ta)^m$, where m is an exponent and Ta an
apparent temperature transition. Values of m deviates from the expected mean
field value, 1/2, suggesting the importance of phase fluctuations. Resulting
values of Ta, interpreted as the onset of phase correlations, decrease as field
increases showing an upward curvature. Values of Tc(H) are obtained through a
two-dimensional critical scaling analysis obeyed by many M(T) curves. The
resulting phase diagram do not show upward curvature and lies below the Ta(H)
line. The value of Hc2(0) estimated from the initial slope $H_c2/dT is
twice the value suggested by the phase diagram. Amplitude fluctuations above
Ta(H) are explained in terms of a Ginzburg-Landau approach extended to high
reduced temperatures and magnetic fields by the introduction of a total-energy
cutoff in the fluctuation spectrum.
Description
Magnetic phase diagram of the layered superconductor
Bi{2+x}Sr{2-x}CuO{6+\delta} (Bi2201) with Tc~7 K
%0 Generic
%1 salemsuguijr2012magnetic
%A Salem-Sugui Jr, S.
%A Alvarenga, A. D.
%A Mosqueira, J.
%A Dancausa, J. D.
%A Mejia, C. Salazar
%A Sinnecker, E.
%A Luo, Huiqian
%A Wen, Hai-Hu
%D 2012
%K BKT highTc magnetisation_above_Tc
%R 10.1088/0953-2048/25/10/105004
%T Magnetic phase diagram of the layered superconductor
Bi2+xSr2-xCuO6+\delta (Bi2201) with Tc~7 K
%U http://arxiv.org/abs/1208.2605
%X We report on magnetization measurements performed on a single crystal of
Bi2+xSr2-xCuO6+\delta with Tc\sim7 K for H||c-axis. The isofield M(T)
curves show a large reversible region, with a pronounced rounding effect as M
approaches zero which prevents the determination of Tc(H). Deviations from the
linear behavior of magnetisation near Tc(H) are studied through the asymptotic
behavior of $-M(T)\sim(T-Ta)^m$, where m is an exponent and Ta an
apparent temperature transition. Values of m deviates from the expected mean
field value, 1/2, suggesting the importance of phase fluctuations. Resulting
values of Ta, interpreted as the onset of phase correlations, decrease as field
increases showing an upward curvature. Values of Tc(H) are obtained through a
two-dimensional critical scaling analysis obeyed by many M(T) curves. The
resulting phase diagram do not show upward curvature and lies below the Ta(H)
line. The value of Hc2(0) estimated from the initial slope $H_c2/dT is
twice the value suggested by the phase diagram. Amplitude fluctuations above
Ta(H) are explained in terms of a Ginzburg-Landau approach extended to high
reduced temperatures and magnetic fields by the introduction of a total-energy
cutoff in the fluctuation spectrum.
@misc{salemsuguijr2012magnetic,
abstract = {We report on magnetization measurements performed on a single crystal of
Bi{2+x}Sr{2-x}CuO{6+\delta} with Tc\sim7 K for H||c-axis. The isofield M(T)
curves show a large reversible region, with a pronounced rounding effect as M
approaches zero which prevents the determination of Tc(H). Deviations from the
linear behavior of magnetisation near Tc(H) are studied through the asymptotic
behavior of $\sqrt{-M(T)}\sim(T-Ta)^m$, where m is an exponent and Ta an
apparent temperature transition. Values of m deviates from the expected mean
field value, 1/2, suggesting the importance of phase fluctuations. Resulting
values of Ta, interpreted as the onset of phase correlations, decrease as field
increases showing an upward curvature. Values of Tc(H) are obtained through a
two-dimensional critical scaling analysis obeyed by many M(T) curves. The
resulting phase diagram do not show upward curvature and lies below the Ta(H)
line. The value of H{c2}(0) estimated from the initial slope $H_{c2}/dT is
twice the value suggested by the phase diagram. Amplitude fluctuations above
Ta(H) are explained in terms of a Ginzburg-Landau approach extended to high
reduced temperatures and magnetic fields by the introduction of a total-energy
cutoff in the fluctuation spectrum.},
added-at = {2012-08-15T17:25:22.000+0200},
author = {Salem-Sugui Jr, S. and Alvarenga, A. D. and Mosqueira, J. and Dancausa, J. D. and Mejia, C. Salazar and Sinnecker, E. and Luo, Huiqian and Wen, Hai-Hu},
biburl = {https://www.bibsonomy.org/bibtex/2a619d202cbc93737033dd052b43724d4/vakaryuk},
description = {Magnetic phase diagram of the layered superconductor
Bi{2+x}Sr{2-x}CuO{6+\delta} (Bi2201) with Tc~7 K},
doi = {10.1088/0953-2048/25/10/105004},
interhash = {96136dcbeead299fa776d21657f71d2a},
intrahash = {a619d202cbc93737033dd052b43724d4},
keywords = {BKT highTc magnetisation_above_Tc},
note = {cite arxiv:1208.2605 Comment: 6 pages, 4 figures},
timestamp = {2012-08-15T17:25:22.000+0200},
title = {Magnetic phase diagram of the layered superconductor
Bi{2+x}Sr{2-x}CuO{6+\delta} (Bi2201) with Tc~7 K},
url = {http://arxiv.org/abs/1208.2605},
year = 2012
}