1,168 research outputs found
Properties of a magnetic superconductor with weak magnetization - application to
Using a Ginsburg-Landau free energy functional, we study the phase
diagram of a weak magnetic superconductor, where the magnetization from the
magnetic component is marginal in supporting a spontaneous vortex phase in
absence of external magnetic field. In particular, the competition between the
spiral state and spontaneous vortex phase is analysed. Our theory is applied to
understand the magnetic properties of .Comment: 13 pages, 4 postscript figure
Influence of Charge and Energy Imbalances on the Tunneling Current through a Superconductor-Normal Metal Junction
We consider quasiparticle charge and energy imbalances in a thin
superconductor weakly coupled with two normal-metal electrodes via tunnel
junctions at low temperatures. Charge and energy imbalances, which can be
created by injecting quasiparticles at one junction, induce excess tunneling
current at the other junction. We numerically obtain
as a function of the bias voltage across the detection junction.
We show that at the zero bias voltage is purely determined by the
charge imbalance, while the energy imbalance causes a nontrivial -dependence of . The obtained voltage-current characteristics
qualitatively agree with the experimental result by R. Yagi [Phys. Rev. B {\bf
73} (2006) 134507].Comment: 10 pages, 5 figure
Normal metal - insulator - superconductor interferometer
Hybrid normal metal - insulator - superconductor microstructures suitable for
studying an interference of electrons were fabricated. The structures consist
of a superconducting loop connected to a normal metal electrode through a
tunnel barrier . An optical interferometer with a beam splitter can be
considered as a classical analogue for this system. All measurements were
performed at temperatures well below 1 K. The interference can be observed as
periodic oscillations of the tunnel current (voltage) through the junction at
fixed bias voltage (current) as a function of a perpendicular magnetic field.
The magnitude of the oscillations depends on the bias point. It reaches a
maximum at energy which is close to the superconducting gap and decreases
with an increase of temperature. Surprisingly, the period of the oscillations
in units of magnetic flux is equal neither to nor to
, but significantly exceeds these values for larger loop circumferences.
The origin of the phenomena is not clear.Comment: 11 pages and 8 figure
Microscopic model for multiple flux transitions in mesoscopic superconducting loops
A microscopic model is constructed which is able to describe multiple
magnetic flux transitions as observed in recent ultra-low temperature tunnel
experiments on an aluminum superconducting ring with normal metal - insulator -
superconductor junctions [Phys. Rev. B \textbf{70}, 064514 (2004)]. The unusual
multiple flux quantum transitions are explained by the formation of metastable
states with large vorticity. Essential in our description is the modification
of the pairing potential and the superconducting density of states by a
sub-critical value of the persistent current which modulates the measured
tunnel current. We also speculate on the importance of the injected
non-equilibrium quasiparticles on the stability of these metastable states.Comment: 6 pages, 3 figure
U(1) symmetry breaking in one-dimensional Mott insulator studied by the Density Matrix Renormalization Group method
A new type of external fields violating the particle number preservation is
studied in one-dimensional strongly correlated systems by the Density Matrix
Renormalization Group method. Due to the U(1) symmetry breaking, the ground
state has fluctuation of the total particle number, which implies injection of
electrons and holes from out of the chain. This charge fluctuation can be
relevant even at half-filling because the particle-hole symmetry is preserved
with the finite effective field. In addition, we discuss a quantum phase
transition obtained by considering the symmetry-breaking fields as a mean field
of interchain-hopping.Comment: 7 pages, 4 figure
Coupling of Josephson current qubits using a connecting loop
We propose a coupling scheme for the three-Josephson junction qubits which
uses a connecting loop, but not mutual inductance. Present scheme offers the
advantages of a large and tunable level splitting in implementing the
controlled-NOT (CNOT) operation. We calculate the switching probabilities of
the coupled qubits in the CNOT operations and demonstrate that present CNOT
gate can meet the criteria for the fault-tolerant quantum computing. We obtain
the coupling strength as a function of the coupling energy of the Josephson
junction and the length of the connecting loop which varies with selecting two
qubits from the scalable design.Comment: 5 pages with updates, version to appear in Phys. Rev.
Broadening of the Beresinkii-Kosterlitz-Thouless superconducting transition by inhomogeneity and finite-size effects
We discuss the crucial role played by finite-size effects and inhomogeneity
on the Beresinkii-Kosterlitz-Thouless (BKT) transition in two-dimensional
superconductors. In particular, we focus on the temperature dependence of the
resistivity, that is dominated by superconducting fluctuations above the BKT
transition temperature and by inhomogeneity below it. By means of a
renormalization-group approach we establish a direct correspondence between the
parameter values used to describe the BKT fluctuation regime and the distance
between and the mean-field Ginzburg-Landau transition temperature.
Below a resistive tail arises due to finite-size effect and
inhomogeneity, that reflects also on the temperature dependence of the
superfluid density. We apply our results to recent experimental data in
superconducting LaAlO/SrTiO heterostructures, and we extract several
informations on the microscopic properties of the system from our BKT fitting
parameters. Finally, we compare our approach to recent data analysis presented
in the literature, where the physical meaning of the parameter values in the
BKT formulas has been often overlooked.Comment: 11 pages, 9 figures, final versio
Magnetization vector in the reversible region of a highly anisotropic cuprate superconductor: anisotropy factor and the role of 2D vortex fluctuations
By using a high quality Tl2Ba2Ca2Cu3O10 (Tl-2223) single crystal as an
example, the magnetization vector was probed in the reversible region of highly
anisotropic cuprate superconductors. For that, we have measured its components
along and transverse to the applied magnetic field for different crystal
orientations. The analysis shows that the angular dependence of the
perpendicular component of the magnetization vector follows the one predicted
by a London-like approach which includes a contribution associated with the
thermal fluctuations of the 2D vortex positions. For the Tl-2223 crystal
studied here, a lower bound for the anisotropy factor was estimated to be about
190.Comment: 6 pages, 3 figure
Hole-trapping by Ni, Kondo effect and electronic phase diagram in non-superconducting Ni-substituted La2-xSrxCu1-yNiyO4
In order to investigate the electronic state in the normal state of high-Tc
cuprates in a wide range of temperature and hole-concentration, specific-heat,
electrical-resistivity, magnetization and muon-spin-relaxation (muSR)
measurements have been performed in non-superconducting Ni-substituted
La2-xSrxCu1-yNiyO4 where the superconductivity is suppressed through the
partial substitution of Ni for Cu without disturbing the Cu-spin correlation in
the CuO2 plane so much. In the underdoped regime, it has been found that there
exist both weakly localized holes around Ni and itinerant holes at high
temperatures. With decreasing temperature, all holes tend to be localized,
followed by the occurrence of variable-range hopping conduction at low
temperatures. Finally, in the ground state, it has been found that each Ni2+
ion traps a hole strongly and that a magnetically ordered state appears. In the
overdoped regime, on the other hand, it has been found that a Kondo-like state
is formed around each Ni2+ spin at low temperatures. In conclusion, the ground
state of non-superconducting La2-xSrxCu1-yNiyO4 changes upon hole doping from a
magnetically ordered state with the strong hole-trapping by Ni2+ to a metallic
state with Kondo-like behavior due to Ni2+ spins, and the quantum phase
transition is crossover-like due to the phase separation into short-range
magnetically ordered and metallic regions.Comment: 9 pages, 8 figures, accepted for publication in Phys. Rev.
Coherent Topological Charge Structure in Models and QCD
In an effort to clarify the significance of the recent observation of
long-range topological charge coherence in QCD gauge configurations, we study
the local topological charge distributions in two-dimensional sigma
models, using the overlap Dirac operator to construct the lattice topological
charge. We find long-range sign coherence of topological charge along extended
one-dimensional structures in two-dimensional spacetime. We discuss the
connection between the long range topological structure found in and
the observed sign coherence along three-dimensional sheets in four-dimensional
QCD gauge configurations. In both cases, coherent regions of topological charge
form along membrane-like surfaces of codimension one. We show that the Monte
Carlo results, for both two-dimensional and four-dimensional gauge theory,
support a view of topological charge fluctuations suggested by Luscher and
Witten. In this framework, the observed membranes are associated with
boundaries between ``k-vacua,'' characterized by an effective local value of
which jumps by across the boundary.Comment: 26 page
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