Upper critical field and peak effect in (Li0.8Fe0.2)OHFeSe single crystal

2021 ◽  
pp. 162454
Author(s):  
Yuxian Wu ◽  
Zhiwei Wen ◽  
Yong Li ◽  
Yajing Cui ◽  
Yongliang Chen ◽  
...  
Keyword(s):  
Single Crystal ◽  
Critical Field ◽  
Upper Critical Field ◽  
Peak Effect

dHvA oscillations, upper critical field and the peak effect studies in a single crystal of LuNi2B2C

2005 ◽  
Vol 359-361 ◽  
pp. 476-478 ◽  
Author(s):  
D. Jaiswal-Nagar ◽  
A.D. Thakur ◽  
M.R. Eskildsen ◽  
P.C. Canfield ◽  
S.M. Yusuf ◽  
...  
Keyword(s):  
Single Crystal ◽  
Critical Field ◽  
Upper Critical Field ◽  
Peak Effect

CRITICAL FIELD AND MAGNETORESISTANCE OF SINGLE CRYSTAL TmNi2B2C

1999 ◽  
Vol 13 (29n31) ◽  
pp. 3715-3717 ◽  
Author(s):  
D. G. NAUGLE ◽  
K. D. D. RATHNAYAKA ◽  
K. CLARK ◽  
P. C. CANFIELD
Keyword(s):  
Magnetic Field ◽  
Transition Temperature ◽  
Single Crystal ◽  
Critical Field ◽  
Superconducting Transition Temperature ◽  
Magnetic Transition ◽  
Upper Critical Field ◽  
Superconducting Transition ◽  
Large Anisotropy ◽  
The Magnetic Field

In-plane resistance as a function of magnitude and direction of the magnetic field and the temperature has been measured for TmNi2B2C from above the superconducting transition temperature at 10.7 K to below the magnetic transition TN=1.5 K. The superconducting upper critical field HC2(T) exhibits a large anisotropy and structure in the vicinity of TN. The magnetoresistance above TC is large and changes sign as the direction of the magnetic field is rotated from in-plane to parallel with the c-axis.

Anisotropic Upper Critical Field of Single Crystal RNi2B2C (R = Y, Lu)

1998 ◽  
Vol 12 (29n31) ◽  
pp. 3264-3266 ◽  
Author(s):  
A. C. Du Mar ◽  
K. D. D. Rathnayaka ◽  
D. G. Naugle ◽  
P. C. Canfield
Keyword(s):  
Low Temperature ◽  
Single Crystal ◽  
Critical Field ◽  
Upper Critical Field ◽  
Critical Fields ◽  
Linear Behavior ◽  
Upward Curvature

Measurements of the anisotropic upper critical field curves have been extended for YNi 2B2C and LuNi2B2C (T c = 15.6 K and 16.1 K, respectively). Measurements of R(T, H) were taken along the crystallographic directions of <100> and <110>. The resulting critical fields show an upward curvature near T c and a linear behavior at low temperature, which continues to below 2 K with little, if any, sign of saturation.

Orientational anisotropy of the upper critical field in single-crystal YBa2Cu3O7andBi2.2CaSr1.9Cu2O8+x

1988 ◽  
Vol 38 (13) ◽  
pp. 9280-9283 ◽  
Author(s):  
M. J. Naughton ◽  
R. C. Yu ◽  
P. K. Davies ◽  
J. E. Fischer ◽  
R. V. Chamberlin ◽  
...  
Keyword(s):  
Single Crystal ◽  
Critical Field ◽  
Upper Critical Field

scholarly journals Anisotropy of upper critical field near TC and magnetic gap of superconducting URu2Si2 single crystal.

1991 ◽  
Vol 185-189 ◽  
pp. 2623-2624
Author(s):  
F.G. Aliev ◽  
V.V. Moshchalkov ◽  
V.V. Pryadun ◽  
N. Agrait ◽  
S. Vieira ◽  
...  
Keyword(s):  
Single Crystal ◽  
Critical Field ◽  
Upper Critical Field

Upper Critical Field Measurements on a Single Crystal YBa2Cu3Oxup to 38 T

1987 ◽  
Vol 26 (Part 2, No. 11) ◽  
pp. L1892-L1894 ◽  
Author(s):  
Toshiro Sakakibara ◽  
Tsuneaki Goto ◽  
Yasuhiro Iye ◽  
Noboru Miura ◽  
Hiroyuki Takeya ◽  
...  
Keyword(s):  
Single Crystal ◽  
Critical Field ◽  
Upper Critical Field ◽  
Field Measurements

The Anisotropic Upper Critical Field of Single Crystal YBa2Cu3Ox

1987 ◽  
Vol 26 (Part 2, No. 6) ◽  
pp. L1057-L1059 ◽  
Author(s):  
Yasuhiro Iye ◽  
Tsuyoshi Tamegai ◽  
Hiroyuki Takeya ◽  
Humihiko Takei
Keyword(s):  
Single Crystal ◽  
Critical Field ◽  
Upper Critical Field

scholarly journals Determination of the Upper Critical Field of a Single Crystal LiFeAs: The Magnetic Torque Study up to 35 Tesla

2011 ◽  
Vol 80 (1) ◽  
pp. 013706 ◽  
Author(s):  
Nobuyuki Kurita ◽  
Kentaro Kitagawa ◽  
Kazuyuki Matsubayashi ◽  
Ade Kismarahardja ◽  
Eun-Sang Choi ◽  
...  
Keyword(s):  
Single Crystal ◽  
Critical Field ◽  
Upper Critical Field ◽  
Magnetic Torque

Transport Properties and Upper Critical Field of Single Crystal Non-Magnetic LuxY1-xNi2B2C and Magnetic LuxGd1-xNi2B2C

2003 ◽  
Vol 17 (18n20) ◽  
pp. 3493-3495 ◽  
Author(s):  
K. D. D. Rathnayaka ◽  
D. G. Naugle ◽  
A. C. Dumar ◽  
M. P. Anatska ◽  
P. C. Canfield
Keyword(s):  
Magnetic Field ◽  
Thermal Conductivity ◽  
Low Temperature ◽  
Single Crystal ◽  
Critical Field ◽  
Magnetic Impurity ◽  
Positive Curvature ◽  
Upper Critical Field ◽  
Magnetic Impurities ◽  
The Magnetic Field

The in-plane resistance of single crystal non-magnetic Lu x Y 1-x Ni 2 B 2 C and magnetic Lu x Gd 1-x Ni 2 B 2 C samples as a function of the magnitude and direction of the magnetic field and temperature have been measured. The superconducting upper critical field Hc2(T) is anisotropic for both. A positive curvature in Hc2(T) near Tc(x) is clearly observed only for the non-magnetic impurity. At low temperature Hc2(T) for the sample with magnetic impurities is strongly reduced. Thermopower, thermal conductivity and resistivity as a function of temperature are also reported for Lu x Gd 1-x Ni 2 B 2 C .

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