724 research outputs found
Specific heat jump at superconducting transition in the presence of Spin-Density-Wave in iron-pnictides
We analyze the magnitude of the specific heat jump \Delta C at the
superconducting transition temperature T_c in the situation when
superconductivity develops in the pre-existing antiferromagnetic phase. We show
that \Delta C/T_c differs from the BCS value and is peaked at the tri-critical
point where this coexistence phase first emerges. Deeper in the magnetic phase,
the onset of coexistence, T_c, drops and \Delta C/T_c decreases, roughly as
\Delta C/T_c \propto T^2_c at intermediate T_c and exponentially at the lowest
T_c, in agreement with the observed behavior of \Delta C/T_c in iron-based
superconductors.Comment: 4+ pages, 3 figure
Spontaneously broken translational symmetry at edges of high-temperature superconductors: thermodynamics in magnetic field
We investigate equilibrium properties, including structure of the order
parameter, superflow patterns, and thermodynamics of low-temperature surface
phases of layered d_{x^2-y^2}-wave superconductors in magnetic field. At zero
external magnetic field, time-reversal symmetry and continuous translational
symmetry along the edge are broken spontaneously in a second order phase
transition at a temperature , where is the
superconducting transition temperature. At the phase transition there is a jump
in the specific heat that scales with the ratio between the edge length and
layer area as , where is
the jump in the specific heat at the d-wave superconducting transition and
is the superconducting coherence length. The phase with broken symmetry
is characterized by a gauge invariant superfluid momentum that
forms a non-trivial planar vector field with a chain of sources and sinks along
the edges with a period of approximately , and saddle point
disclinations in the interior. To find out the relative importance of
time-reversal and translational symmetry breaking we apply an external field
that breaks time-reversal symmetry explicitly. We find that the phase
transition into the state with the non-trivial vector field keeps
its main signatures, and is still of second order. In the external field, the
saddle point disclinations are pushed towards the edges, and thereby a chain of
edge motifs are formed, where each motif contains a source, a sink, and a
saddle point. Due to a competing paramagnetic response at the edges, the phase
transition temperature is slowly suppressed with increasing magnetic
field strength, but the phase with broken symmetry survives into the mixed
state.Comment: 12 pages, 9 figure
Reduced effect of impurities on the universal pairing scale in the cuprates
We consider the effect of non-magnetic impurities on the onset temperature
for the wave pairing in spin-fluctuation scenario for the cuprates.
We analyze intermediate coupling regime when the magnetic correlation length
and the dimensionless coupling is O(1). In the clean limit, in this parameter range, and weakly depends on and
. We found numerically that this universal pairing scale is also quite
robust with respect to impurities: the scattering rate needed to
bring down to zero is about 4 times larger than in weak coupling, in good
quantitative agreement with experiments. We provide analytical reasoning for
this result.Comment: 4 pages, 2 fig, submitted to PR
Pauli-Limited Superconductivity with Classical Magnetic Fluctuations
We examine the effect of classical magnetic fluctuations on the phase diagram
of paramagneticallylimited two-dimensional superconductors under a Zeeman
magnetic field. We derive the free energy expansion in powers of the
superconducting order parameter and analyze the character of the
normalsuperconducting transition. While the transition is of the second order
for all temperatures in the absence of magnetic fluctuations, we find that
proximity to magnetism drives both the transition into the uniform state and
that into the modulated (Fulde-Ferrell-Larkin-Ovchinnikov, FFLO) state to first
order at intermediate temperatures. We compute the thermodynamic signatures of
the normal-superconducting transition along the upper critical field.Comment: 16 pages, 9 figure
Interplay between magnetism and superconductivity in Fe-pnictides
We consider phase transitions and potential co-existence of spin-density-wave
(SDW) magnetic order and extended s-wave () superconducting order within a
two-band itinerant model of iron pnictides, in which SDW magnetism and
superconductivity are competing orders. We show that depending on parameters,
the transition between these two states is either first order, or involves an
intermediate phase in which the two orders co-exist. We demonstrate that such
co-existence is possible when SDW order is incommensurate.Comment: 5 pages, 3 figure
Supercomputer Simulations of Disk Galaxies
The time evolution of models for an isolated disk of highly flattened
galaxies of stars is investigated by direct integration of the Newtonian
equations of motion of N=30,000 identical stars over a time span of many
galactic rotations. Certain astronomical implications of the simulations to
actual disk-shaped (i.e. rapidly rotating) galaxies are explored as well.Comment: 3 pages, 2 figure Aat.sty, Aattable.sty, presented by E. Griv at the
JENAM 2000, S02, Moscow, Russia, 200
Microscopic evidence for field-induced magnetism in CeCoIn
We present NMR data in the normal and superconducting states of CeCoIn
for fields close to T in the plane. Recent
experiments identified a first-order transition from the normal to
superconducting state for T, and a new thermodynamic phase below 290
mK within the superconducting state. We find that the Knight shifts of the
In(1), In(2) and the Co are discontinuous across the first-order transition and
the magnetic linewidths increase dramatically. The broadening differs for the
three sites, unlike the expectation for an Abrikosov vortex lattice, and
suggests the presence of static spin moments in the vortex cores. In the
low-temperature and high-field phase the broad NMR lineshapes suggest ordered
local moments, rather than a long wavelength quasiparticle spin density
modulation expected for an FFLO phase.Comment: 4 pages, 4 figures. to appear in Phys. Rev. Let
Superconductivity and spin-density-waves in multi-band metals
We present a detailed description of two-band quasi-2D metals with s-wave
superconducting (SC) and antiferromagnetic spin-density wave (SDW)
correlations. We present a general approach and use it to investigate the
influence of the difference between the shapes and the areas of the two Fermi
surfaces on the phase diagram. In particular, we determine the conditions for
the co-existence of SC and SDW orders at different temperatures and dopings. We
argue that a conventional s-wave SC order co-exists with SDW order only at very
low and in a very tiny range of parameters. An extended s-wave
superconductivity, for which SC gap changes sign between the two bands,
co-exists with antiferromagnetic SDW over a much wider range of parameters and
temperatures, but even for this SC order the regions of SDW and SC can still be
separated by a first order transition. We show that the co-existence range
becomes larger if SDW order is incommensurate. We apply our results to
iron-based pnictide materials, in some of which co-existence of SDW and SC
orders has been detected.Comment: 18 figures, 22 pages, published version with minor correction
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