scholarly journals Disordering of the vortex lattice through successive destruction of positional and orientational order in a weakly pinned Co0.0075NbSe2 single crystal

2015 ◽  
Vol 5 (1) ◽  
Author(s):  
Somesh Chandra Ganguli ◽  
Harkirat Singh ◽  
Garima Saraswat ◽  
Rini Ganguly ◽  
Vivas Bagwe ◽  
...  

Abstract The vortex lattice in a Type II superconductor provides a versatile model system to investigate the order-disorder transition in a periodic medium in the presence of random pinning. Here, using scanning tunnelling spectroscopy in a weakly pinned Co0.0075NbSe2 single crystal, we show that the vortex lattice in a 3-dimensional superconductor disorders through successive destruction of positional and orientational order, as the magnetic field is increased across the peak effect. At the onset of the peak effect, the equilibrium quasi-long range ordered state transforms into an orientational glass through the proliferation of dislocations. At a higher field, the dislocations dissociate into isolated disclination giving rise to an amorphous vortex glass. We also show the existence of a variety of additional non-equilibrium metastable states, which can be accessed through different thermomagnetic cycling.

2016 ◽  
Vol 6 (1) ◽  
Author(s):  
Somesh Chandra Ganguli ◽  
Harkirat Singh ◽  
Garima Saraswat ◽  
Rini Ganguly ◽  
Vivas Bagwe ◽  
...  

2019 ◽  
Vol 4 (3) ◽  
pp. 74 ◽  
Author(s):  
Mehmet Egilmez ◽  
Isaac Isaac ◽  
Ali S. Alnaser ◽  
Zbigniew Bukowski ◽  
Janusz Karpinski ◽  
...  

We report on the measurements of the remnant magnetization, and hence critical current, in a single crystal of YBa2Cu4O8. A peak in the temperature dependence of the critical current is observed when the external magnetic field is tilted away from the a–b planes. The observed behavior is attributed to a thermally activated instability-driven vortex-lattice splitting or vortex chain formation. The nature of the peak and the possibility of a thermally-activated dimensional crossover have been discussed.


1991 ◽  
Vol 66 (17) ◽  
pp. 2270-2273 ◽  
Author(s):  
D. G. Grier ◽  
C. A. Murray ◽  
C. A. Bolle ◽  
P. L. Gammel ◽  
D. J. Bishop ◽  
...  

2003 ◽  
Vol 91 (16) ◽  
Author(s):  
S. R. Park ◽  
S. M. Choi ◽  
D. C. Dender ◽  
J. W. Lynn ◽  
X. S. Ling

2021 ◽  
Author(s):  
jialu wu ◽  
Bo Li ◽  
Hong Wang ◽  
Ying Zhen Lai ◽  
Yue Ye ◽  
...  

A pair of enantiomers {[Cu(L-pro)(L-tyr)]·2H2O}n (L-1) and {[Cu(D-pro)(D-tyr)]·2H2O}n (D-1) based on the chiral ligands L/D-proline and L/D-tyrosine were synthesized and investigated by single-crystal X-ray structure analysis, IR, thermogravimetric analysis, solid-state...


Crystals ◽  
2018 ◽  
Vol 9 (1) ◽  
pp. 18 ◽  
Author(s):  
Jing Dai ◽  
Boris Kharkov ◽  
Sergey Dvinskikh

We investigate conformational dynamics in the smectic A phase formed by the mesogenic ionic liquid 1-tetradecyl-3-methylimidazolium nitrate. Solid-state high-resolution 13C nuclear magnetic resonance (NMR) spectra are recorded in the sample with the mesophase director aligned in the magnetic field of the NMR spectrometer. The applied NMR method, proton encoded local field spectroscopy, delivers heteronuclear dipolar couplings of each 13C spin to its 1H neighbours. From the analysis of the dipolar couplings, orientational order parameters of the C–H bonds along the hydrocarbon chain were determined. The estimated value of the molecular order parameter S is significantly lower compared to that in smectic phases of conventional non-ionic liquid crystals.


1994 ◽  
Vol 197 (1-4) ◽  
pp. 579-587 ◽  
Author(s):  
W.K. Kwok ◽  
J. Fendrich ◽  
S. Fleshler ◽  
U. Welp ◽  
J. Downey ◽  
...  

1999 ◽  
Vol 13 (29n31) ◽  
pp. 3715-3717 ◽  
Author(s):  
D. G. NAUGLE ◽  
K. D. D. RATHNAYAKA ◽  
K. CLARK ◽  
P. C. CANFIELD

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.


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