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timestamp[s] | authors_parsed
sequence |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
supr-con/9507007 | Kikuo Harigaya | Kikuo Harigaya | Nonlinear optical response in doped conjugated polymers | Accepted for publication in J. Phys.: Condens. Matter | J. Phys.: Condens. Matter 7 (1995) 7529-7534 | 10.1088/0953-8984/7/38/011 | null | supr-con chem-ph cond-mat.supr-con mtrl-th | null | Exciton effects on conjugated polymers are investigated in soliton lattice
states. We use the Su-Schrieffer-Heeger model with long-range Coulomb
interactions. The Hartree-Fock (HF) approximation and the single-excitation
configuration- interaction (single-CI) method are used to obtain optical
absorption spectra. The third-harmonic generation (THG) at off-resonant
frequencies is calculated as functions of the soliton concentration and the
chain length of the polymer. The magnitude of the THG at the 10 percent doping
increases by the factor about 10^2 from that of the neutral system. This is
owing to the accumulation of the oscillator strengths at the lowest exciton
with increasing the soliton concentration. The increase by the order two is
common for several choices of Coulomb interaction strengths.
| [
{
"version": "v1",
"created": "Sun, 30 Jul 1995 15:26:17 GMT"
}
] | 2008-02-03T00:00:00 | [
[
"Harigaya",
"Kikuo",
""
]
] |
supr-con/9508001 | Valerii Vinokur | I. Aranson, B.Ya. Shapiro and V. Vinokur (ANL) | Nucleation and Growth of Normal Phase in Thin Superconducting Strips | 4 pages, Revtex, 2 figures avilable from author via
[email protected] | null | 10.1103/PhysRevLett.76.142 | null | supr-con cond-mat.supr-con | null | We investigate the kinetics of normal phase nucleation and flux line
condensation in the type-II superconductors by numerical study of the
time-dependent Ginzburg-Landau equation. We have shown that under the
sufficient transport current the normal phase nucleates in the superconducting
strips in a form of the macroscopic droplets having the multiple topological
charge. We discuss the stability and the dynamics of the droplets. We found
that pinning suppresses the droplet formation.
| [
{
"version": "v1",
"created": "Thu, 3 Aug 1995 20:10:12 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Aranson",
"I.",
"",
"ANL"
],
[
"Shapiro",
"B. Ya.",
"",
"ANL"
],
[
"Vinokur",
"V.",
"",
"ANL"
]
] |
supr-con/9508002 | Masanori Ichioka | M. Ichioka(Kyoto Univ.), N. Enomoto, N. Hayashi, and K.
Machida(Okayama Univ.) | $s$- and $d_{xy}$-wave components induced around a vortex in
$d_{x^2-y^2}$-wave superconductors | RevTex,9 pages, 6 figures in a uuencoded file | Phys. Rev. B53, 2233 (1996). | 10.1103/PhysRevB.53.2233 | null | supr-con cond-mat.supr-con | null | Vortex structure of $d_{x^2-y^2}$-wave superconductors is microscopically
analyzed in the framework of the quasi-classical Eilenberger equations. If the
pairing interaction contains an $s$-wave ($d_{xy}$-wave) component in addition
to a $d_{x^2-y^2}$-wave component, the $s$-wave ($d_{xy}$-wave) component of
the order parameter is necessarily induced around a vortex in
$d_{x^2-y^2}$-wave superconductors. The spatial distribution of the induced
$s$-wave and $d_{xy}$-wave components is calculated. The $s$-wave component has
opposite winding number around vortex near the $d_{x^2-y^2}$-vortex core and
its amplitude has the shape of a four-lobe clover. The amplitude of
$d_{xy}$-component has the shape of an octofoil. These are consistent with
results based on the GL theory.
| [
{
"version": "v1",
"created": "Sun, 20 Aug 1995 05:46:16 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Ichioka",
"M.",
"",
"Kyoto Univ."
],
[
"Enomoto",
"N.",
"",
"Okayama Univ."
],
[
"Hayashi",
"N.",
"",
"Okayama Univ."
],
[
"Machida",
"K.",
"",
"Okayama Univ."
]
] |
supr-con/9508003 | Asai Yoshihiro | Yoshihiro Asai (ETL, Tsukuba, Japan) | Superconducting, magnetic, and charge correlations in the doped
two-chain Hubbard model | RevTeX 3.0, 11 pages, 5 figs via FAX, Phys.Rev.B to appear | null | 10.1103/PhysRevB.52.10390 | YA#HUB003Y95M01 | supr-con cond-mat.supr-con | null | Superconducting, magnetic, and charge correlation functions and dynamic spin
correlation functions of the doped two-chain Hubbard model is studied with the
projector Quantum Monte carlo method and Lanczos recursion method. Of the three
correlation functions, the interchain singlet superconducting correlation
function is the most long range. Our data is not consistent with the
Luther-Emery picture.
| [
{
"version": "v1",
"created": "Tue, 22 Aug 1995 07:15:09 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Asai",
"Yoshihiro",
"",
"ETL, Tsukuba, Japan"
]
] |
supr-con/9508004 | Steven Spencer | Steven Spencer and Henrik Jeldoft Jensen | The Bean Critical State: Infinitely Unstable | 8 pages including 4 figures. Whole paper in uuencoded postscript file
bean.uu | null | 10.1016/0921-4534(96)00240-7 | null | supr-con cond-mat.supr-con | null | The threshold for creep in the Bean critical state is investigated. We
perturb the Bean state by an energy $\Delta\epsilon$. We find that no matter
how small $\Delta\epsilon$ is it will always be able to induce creep somewhere
on the Bean profile. This finding has important consequences for the
interpretation of low temperature creep phenomena in terms of quantum creep.
| [
{
"version": "v1",
"created": "Thu, 24 Aug 1995 16:22:00 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Spencer",
"Steven",
""
],
[
"Jensen",
"Henrik Jeldoft",
""
]
] |
supr-con/9508005 | Zbigniew J. Koziol | Z. Kozio{\l} and R.A. Dunlap | Nonlinear Flux Diffusion and ac Susceptibility of Superconductors -
Exact Numerical Results | 9 LaTeX pages, 4 Postscript figures, WWW version available at
http://is.dal.ca/~zkoziol/super.html | null | 10.1063/1.361702 | null | supr-con cond-mat.supr-con | null | The ac response of a slab of material with electrodynamic characteristics
$E\sim j^{\kappa+1}$, $\kappa\geq0$, is studied numerically. From the solutions
of the nonlinear diffusion equation, the fundamental and higher-order
components of the harmonic susceptibility are obtained. A large portion of the
data for every $\kappa$ can be scaled by a single parameter, $\xi$
=$t^{1/(\kappa+2)}\cdot H_0^{\kappa/(\kappa+2)}/D$, where $t$ is the period of
the ac field at the surface, $H_0$ is its amplitude and $D$ is the slab
thickness. This is, however, only an approximate scaling property: The field
penetration into a nonlinear medium is a more complex phenomenon than in the
linear case. In particular, the susceptibility values are not uniquely defined
by a set of only two parameters, such as $\kappa$ and $\xi$, while one
parameter, i.e. $t^{1/2}$/D, is sufficient to describe the electrodynamic
response of a linear medium.
| [
{
"version": "v1",
"created": "Tue, 29 Aug 1995 02:38:27 GMT"
}
] | 2022-02-02T00:00:00 | [
[
"Kozioł",
"Z.",
""
],
[
"Dunlap",
"R. A.",
""
]
] |
supr-con/9508006 | Zbigniew J. Koziol | Z. Kozio{\l} and R.A. Dunlap | Magnetostriction of a Superconductor: -Results from the Critical-State
Model | 9 LaTeX pages, 4 Postscript figures, WWW version available at
http://is.dal.ca/~zkoziol/super.html | null | 10.1063/1.361697 | null | supr-con cond-mat.supr-con | null | In many cases, the critical-state theory can be treated as a suffi ciently
accurate approximation for the modelling of the magnetic properties of
superconductors. In the present work, the magnetostrictive hysteresis is
computed for a quite general case of the modified Kim-Anderson model. The
results obtained reproduce many features of the giant magnetostriction
(butterfly-shaped curves) reported in the literature for measurements made on
single-crystal samples of the high-temperature superconductor
$Bi_2Sr_2CaCu_2O_8$. It is shown that addition of a contribution to the
magnetostriction in the superconducting state which is of similar origin as in
the normal state, offers a broader phenomenological interpretation of the
complex magnetostriction hysteresis found in such heavy-fermion compounds as
$UPt_3$, $URu_2Si_2$ or $UBe_{13}$.
| [
{
"version": "v1",
"created": "Tue, 29 Aug 1995 16:45:50 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Kozioł",
"Z.",
""
],
[
"Dunlap",
"R. A.",
""
]
] |
supr-con/9509001 | null | Kenneth Holmlund and Petter Minnhagen | Langevin Simulations of Two Dimensional Vortex Fluctuations: Anomalous
Dynamics and a New $IV$-exponent | Submitted to PRB, RevTeX format, 28 pages and 13 figures, figures in
postscript format are available at http://www.tp.umu.se/~holmlund/papers.html | null | 10.1103/PhysRevB.54.523 | null | supr-con cond-mat.supr-con | null | The dynamics of two dimensional (2D) vortex fluctuations are investigated
through simulations of the 2D Coulomb gas model in which vortices are
represented by soft disks with logarithmic interactions. The simulations
trongly support a recent suggestion that 2D vortex fluctuations obey an
intrinsic anomalous dynamics manifested in a long range 1/t-tail in the vortex
correlations. A new non-linear IV-exponent a, which is different from the
commonly used AHNS exponent, a_AHNS and is given by a = 2a_AHNS - 3, is
confirmed by the simulations. The results are discussed in the context of
earlier simulations, experiments and a phenomenological description.
| [
{
"version": "v1",
"created": "Wed, 6 Sep 1995 11:14:33 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Holmlund",
"Kenneth",
""
],
[
"Minnhagen",
"Petter",
""
]
] |
supr-con/9510001 | Vladimir Dzhunushaliev | V.D.Dzhunushaliev | The string model of the Cooper pair in the anisotropic superconductor | final version, Latex, 9p, to be published in Phys. Rev. B | Phys.Rev.B, 54, 10121(1996) | 10.1103/PhysRevB.54.10121 | null | supr-con cond-mat.supr-con hep-th | null | The analogy between the Cooper pair in high temperature superconductor and
the quark-antiquark pair in quantum chromodynamics (QCD) is proposed. In QCD
the nonlinear chromodynamical field between a quark and an antiquark is
confined to a tube. So we assume that there is the strong interaction between
phonons which can confine them to some tube too. This tube is described using
the nonlinear Schr\"odinger equation. We show that it has an infinite spectrum
of axially symmetric (string) solutions with negative finite linear energy
density. The one-dimensional nonlinear Schr\"odinger equation has a finite
spectrum (hence, it has a steady-state) which describes the Cooper pair
squezeed between anisotropy planes in the superconductor. It is shown that in
this model the transition temperature is approximately 45 K.
| [
{
"version": "v1",
"created": "Wed, 11 Oct 1995 10:18:24 GMT"
},
{
"version": "v2",
"created": "Tue, 17 Oct 1995 10:39:16 GMT"
},
{
"version": "v3",
"created": "Thu, 4 Jul 1996 06:35:28 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Dzhunushaliev",
"V. D.",
""
]
] |
supr-con/9510002 | null | P. Calvani, M. Capizzi, S. Lupi, P. Maselli, A. Paolone, (Dipartimento
di Fisica, Universita di Roma ``La Sapienza'', Roma, Italy) and P. Roy
(Laboratoire pour l'Utilization de Rayonnement Electromagnetique, Universite
Paris-Sud, Orsay, France) | Polaronic optical absorption in electron-doped and hole-doped cuprates | File latex, 31 p., submitted to Physical Review B. Figures may be
faxed upon request | null | 10.1103/PhysRevB.53.2756 | null | supr-con cond-mat.supr-con | null | Polaronic features similar to those previously observed in the photoinduced
spectra of cuprates have been detected in the reflectivity spectra of
chemically doped parent compounds of high-critical-temperature superconductors,
both $n$-type and $p$-type. In Nd$_2$CuO$_{4-y}$ these features, whose
intensities depend both on doping and temperature, include local vibrational
modes in the far infrared and a broad band centered at $\sim$ 1000 cm$^{-1}$.
The latter band is produced by the overtones of two (or three) local modes and
is well described in terms of a small-polaron model, with a binding energy of
about 500 cm$^{-1}$. Most of the above infrared features are shown to survive
in the metallic phase of Nd$_{2-x}$Ce$_x$Cu0$_{4-y}$, Bi$_2$Sr$_2$CuO$_6$, and
YBa$_2$Cu$_3$O$_{7-y}$, where they appear as extra-Drude peaks. The occurrence
of polarons is attributed to local modes strongly coupled to carriers, as shown
by a comparison with tunneling results.
| [
{
"version": "v1",
"created": "Fri, 27 Oct 1995 17:52:19 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Calvani",
"P.",
"",
"Laboratoire pour l'Utilization de Rayonnement Electromagnetique, Universite\n Paris-Sud, Orsay, France"
],
[
"Capizzi",
"M.",
"",
"Laboratoire pour l'Utilization de Rayonnement Electromagnetique, Universite\n Paris-Sud, Orsay, France"
],
[
"Lupi",
"S.",
"",
"Laboratoire pour l'Utilization de Rayonnement Electromagnetique, Universite\n Paris-Sud, Orsay, France"
],
[
"Maselli",
"P.",
"",
"Laboratoire pour l'Utilization de Rayonnement Electromagnetique, Universite\n Paris-Sud, Orsay, France"
],
[
"Paolone",
"A.",
"",
"Laboratoire pour l'Utilization de Rayonnement Electromagnetique, Universite\n Paris-Sud, Orsay, France"
],
[
"Roy",
"P.",
"",
"Laboratoire pour l'Utilization de Rayonnement Electromagnetique, Universite\n Paris-Sud, Orsay, France"
]
] |
supr-con/9511001 | null | Dmitry A. Ryndyk (Institute for Physics of Microstructures of Russian
Academy of Sciencies, Nizhny Novgorod, Russia) | Synchronization in one-dimensional array of Josephson coupled thin
layers | REVTeX, 8 pages, no figures | null | null | null | supr-con cond-mat.supr-con | null | We obtain self-consistent macroscopic equations describing interlayer
Josephson effect and intralayer disequilibrium in one-dimensional array of
Josephson coupled layers. We show that ``nonequilibrium coupling'' can lead to
effective spatial and time synchronization and formation of coherent dynamic
resistive state (collective Josephson effect) in Nb-AlO-Nb stacked junctions
and HTSC (intrinsic Josephson effect). We propose it to be the origin of
collective switching phenomena observed in PbBiSrCaCuO.
| [
{
"version": "v1",
"created": "Tue, 21 Nov 1995 10:28:30 GMT"
}
] | 2008-02-03T00:00:00 | [
[
"Ryndyk",
"Dmitry A.",
"",
"Institute for Physics of Microstructures of Russian\n Academy of Sciencies, Nizhny Novgorod, Russia"
]
] |
supr-con/9511002 | Juan I. Collar | V.Jeudy, J.I.Collar, T.A.Girard, D.Limagne and G.Waysand (G.P.S.,
Univ. Paris 7) | S-35 Beta Irradiation of a Tin Strip in a State of Superconducting
Geometrical Metastability | Compressed PostScript (filename.ps.Z), 9 pages, 2 figures | Nucl.Instrum.Meth. A373 (1996) 65-67 | 10.1016/0168-9002(95)01451-9 | JICUSC-95-8 | supr-con cond-mat.supr-con hep-ex nucl-ex | null | We report the first energy loss spectrum obtained with a geometrically
metastable type I superconducting tin strip irradiated by the beta-emission of
S-35. (Nucl. Instr. Meth. A, in press)
| [
{
"version": "v1",
"created": "Thu, 30 Nov 1995 17:02:06 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Jeudy",
"V.",
"",
"G.P.S.,\n Univ. Paris 7"
],
[
"Collar",
"J. I.",
"",
"G.P.S.,\n Univ. Paris 7"
],
[
"Girard",
"T. A.",
"",
"G.P.S.,\n Univ. Paris 7"
],
[
"Limagne",
"D.",
"",
"G.P.S.,\n Univ. Paris 7"
],
[
"Waysand",
"G.",
"",
"G.P.S.,\n Univ. Paris 7"
]
] |
supr-con/9512001 | Masanori Ichioka | M. Ichioka (Kyoto), N. Hayashi, N. Enomoto and K. Machida (Okayama) | Vortex structure in $d$-wave superconductors | 22 pages, RevTex, 23 figures available upon request | Phys. Rev. B 53, 15316 (1996). | 10.1103/PhysRevB.53.15316 | null | supr-con cond-mat.supr-con | null | Vortex structure of pure $d_{x^2-y^2}$-wave superconductors is
microscopically analyzed in the framework of the quasi-classical Eilenberger
equations. Selfconsistent solution for the $d$-wave pair potential is obtained
for the first time in the case of an isolated vortex. The vortex core
structure, i.e., the pair potential, the supercurrent and the magnetic field,
is found to be fourfold symmetric even in the case that the mixing of $s$-wave
component is absent. The detailed temperature dependences of these quantities
are calculated. The fourfold symmetry becomes clear when temperature is
decreased. The local density of states is calculated for the selfconsistently
obtained pair potential. From the results, we discuss the flow trajectory of
the quasiparticles around a vortex, which is characteristic in the
$d_{x^2-y^2}$-wave superconductors. The experimental relevance of our results
to high temperature superconductors is also given.
| [
{
"version": "v1",
"created": "Sat, 9 Dec 1995 03:20:47 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Ichioka",
"M.",
"",
"Kyoto"
],
[
"Hayashi",
"N.",
"",
"Okayama"
],
[
"Enomoto",
"N.",
"",
"Okayama"
],
[
"Machida",
"K.",
"",
"Okayama"
]
] |
supr-con/9512002 | Juan I. Collar | V.Jeudy, D.Limagne, G.Waysand, J.I.Collar and T.A.Girard (G.P.S.,
Univ. Paris 7) | Beta Irradiation of a Geometrically Metastable Superconducting Strip
Detector with a Magnetic Flux Penetration Read-Out | Compressed PostScript (filename.ps.Z), 8 pages, 2 figures | null | 10.1016/0168-9002(95)01063-7 | JICUSC-95-9 | supr-con cond-mat.supr-con | null | Geometrical metastability, observed in superconducting type I tin flat
strips, has been previously proposed as a principle for particle detection. The
energy deposition of an incoming beta-particle induces the rupture of the
metastability and consequently the penetration of multiquantum flux tubes into
a superconducting tin strip. We present here the first absorption spectra from
two beta sources, which demonstrate the linearity and energy-resolution of
these detectors (presented at the 6th International Workshop on Low Temperature
Detectors for Dark Matter and Neutrinos (LTD-6), Interlaken, Switzerland, Sept.
1995)
| [
{
"version": "v1",
"created": "Sun, 10 Dec 1995 14:42:47 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Jeudy",
"V.",
"",
"G.P.S.,\n Univ. Paris 7"
],
[
"Limagne",
"D.",
"",
"G.P.S.,\n Univ. Paris 7"
],
[
"Waysand",
"G.",
"",
"G.P.S.,\n Univ. Paris 7"
],
[
"Collar",
"J. I.",
"",
"G.P.S.,\n Univ. Paris 7"
],
[
"Girard",
"T. A.",
"",
"G.P.S.,\n Univ. Paris 7"
]
] |
supr-con/9512003 | Eduardo Jagla | E.A.Jagla and C. A. Balseiro | Vortex structure and resistive transitions in high-Tc superconductors | 8 pages + 6 figures | null | 10.1103/PhysRevB.53.15305 | null | supr-con cond-mat.supr-con | null | The nature of the resistive transition for a current applied parallel to the
magnetic field in high-Tc materials is investigated by numerical simulation on
the three dimensional Josephson junction array model. It is shown by using
finite size scaling that for samples with disorder the critical temperature Tp
for the c axis resistivity corresponds to a percolation phase transition of
vortex lines perpendicularly to the applied field. The value of Tp is higher
than the critical temperature for j perpendicular to H, but decreases with the
thickness of the sample and with anisotropy. We predict that critical behavior
around Tp should reflect in experimentally accessible quantities, as the I-V
curves.
| [
{
"version": "v1",
"created": "Thu, 14 Dec 1995 13:30:30 GMT"
}
] | 2009-10-28T00:00:00 | [
[
"Jagla",
"E. A.",
""
],
[
"Balseiro",
"C. A.",
""
]
] |
supr-con/9601001 | Modanese Giovanni | G. Modanese (INFN, Trento) | Updating the theoretical analysis of the weak gravitational shielding
experiment | LaTex, 6 pages. Only formal changes in title and abstract | Proceedings of the 1997 IAF (International Astronautical
Federation) Congress, nr. IAA-97-4.107 | null | UTF-367/96 | supr-con cond-mat.supr-con gr-qc hep-ph | null | The most recent data about the weak gravitational shielding produced recently
through a levitating and rotating HTC superconducting disk show a very weak
dependence of the shielding value ($\sim 1 \%$) on the height above the disk.
We show that whilst this behaviour is incompatible with an intuitive vectorial
picture of the shielding, it is consistently explained by our theoretical
model. The expulsive force observed at the border of the shielded zone is due
to energy conservation.
| [
{
"version": "v1",
"created": "Wed, 17 Jan 1996 20:54:45 GMT"
},
{
"version": "v2",
"created": "Fri, 9 Feb 1996 06:37:54 GMT"
}
] | 2008-02-03T00:00:00 | [
[
"Modanese",
"G.",
"",
"INFN, Trento"
]
] |
supr-con/9602001 | Franco Nori | C. Reichhardt, C. J. Olson, J. Groth, Stuart Field, and Franco Nori | Vortex Plastic Flow, $B(x,y,H(t)), M(H(t)), J_c(B(t))$, Deep in the Bose
Glass and Mott-Insulator Regimes | 4 pages, 4 PostScript Figures | Phys. Rev. B 53 (1996) R8898-R8901 | 10.1103/PhysRevB.53.R8898 | null | supr-con cond-mat.mtrl-sci cond-mat.supr-con | null | We present simulations of flux-gradient-driven superconducting vortices
interacting with strong columnar pinning defects as an external field $H(t)$ is
quasi-statically swept from zero through a matching field $B_{\phi}$. We
analyze several measurable quantities, including the local flux density $
B(x,y,H(t))$, magnetization $M(H(t))$, critical current $J_{c}(B(t))$, and the
individual vortex flow paths. We find a significant change in the behavior of
these quantities as the local flux density crosses $B_{\phi}$, and quantify it
for many microscopic pinning parameters. Further, we find that for a given pin
density $J_c(B)$ can be enhanced by maximizing the distance between the pins
for $ B < B_{\phi} $.
| [
{
"version": "v1",
"created": "Wed, 14 Feb 1996 20:34:48 GMT"
}
] | 2016-09-08T00:00:00 | [
[
"Reichhardt",
"C.",
""
],
[
"Olson",
"C. J.",
""
],
[
"Groth",
"J.",
""
],
[
"Field",
"Stuart",
""
],
[
"Nori",
"Franco",
""
]
] |
supr-con/9602002 | Santi Gilles | G. Santi, T. Jarlborg, M. Peter and M. Weger | s and d-wave symmetries of the solutions of the Eliashberg equations | Uuencoded LaTeX file anf 6 Postscript figures (14 pages). Accepted
for publication in Physica C | null | 10.1016/0921-4534(96)00052-4 | null | supr-con cond-mat.supr-con | null | We examine the different possible symmetries of the superconducting gap
obtained by solving the Eliashberg equations. We consider an electron-phonon
interaction in a strong coupling scenario. The Coulomb pseudopotential plays
the crucial role of providing the repulsion needed to favour the d-wave
symmetry. But the key parameter that allows very anisotropic solutions even
with very strong coupling is the small angular range of the interaction due to
predominantly electron-phonon forward scattering that is found in the high-Tc
superconductors. We find both s and d-wave solutions whose stability depends
mainly on the angular range of the interaction.
| [
{
"version": "v1",
"created": "Fri, 23 Feb 1996 07:25:24 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Santi",
"G.",
""
],
[
"Jarlborg",
"T.",
""
],
[
"Peter",
"M.",
""
],
[
"Weger",
"M.",
""
]
] |
supr-con/9602003 | Durga Prasad Choudhury | S. Oxx, D. P. Choudhury, Balam A. Willemsen, H. Srikanth, S. Sridhar
(Northeastern Univ), B. K. Cho, P. C. Canfield (Ames Lab) | Vortex Response and Critical Fields observed via rf penetration depth
measurements on the superconductor YNi_2B_2C | 6 LaTeX pages with 6 EPS figures, uses RevTeX, multicol and epsf. One
figure bitmapped. Better PS file available at
http://sagar.physics.neu.edu/preprints.html Submitted to Physica C | null | 10.1016/0921-4534(96)00230-4 | null | supr-con cond-mat.supr-con | null | Measurements of the rf penetration depth \lambda(T,H,\theta ) are used to
study the superconducting order parameter, vortex dynamics in the mixed state
and delineate critical fields in the borocarbide superconductor YNi_2B_2C. The
lower critical field has an anomalous T dependence, H_{c1}(T)=1.12[1-(T/T_c)]
kOe, which is however consistent with independent superfluid density
measurements at microwave frequencies. The vortex response is dominated by
viscous flux flow, indicative of extremely weak pinning, and is parametrized by
a field scale H_{c2,eff}. The angular dependence of the vortex contribution
\lambda(\theta) is in good agreement with the Coffey-Clem model. Structure is
seen in the depairing transition in the vicinity of the upper critical field,
with the existence of well-defined critical fields H_{c2a}, H_{c2b} and
H_{c2c}, with the vortex field scale H_{c2,eff} closest to H_{c2b}. Overall the
measurements indicate that YNi_2B_2C has a rich and unusual field dependence of
its transport parameters.
| [
{
"version": "v1",
"created": "Mon, 26 Feb 1996 20:11:10 GMT"
},
{
"version": "v2",
"created": "Tue, 27 Feb 1996 21:35:05 GMT"
}
] | 2015-06-26T00:00:00 | [
[
"Oxx",
"S.",
"",
"Northeastern Univ"
],
[
"Choudhury",
"D. P.",
"",
"Northeastern Univ"
],
[
"Willemsen",
"Balam A.",
"",
"Northeastern Univ"
],
[
"Srikanth",
"H.",
"",
"Northeastern Univ"
],
[
"Sridhar",
"S.",
"",
"Northeastern Univ"
],
[
"Cho",
"B. K.",
"",
"Ames Lab"
],
[
"Canfield",
"P. C.",
"",
"Ames Lab"
]
] |
supr-con/9604001 | null | Alexey V. Samokhvalov (Institute for physics of microstructures,
Nizhny Novgorod, Russia) | Vortex loops entry into type--II superconductors | LaTeX file ( 22 pages & 7 figures ); the required TeX style file
"bezier.sty" is attached; accepted for publication in Physica C | Physica C 259 (1996) 337 | 10.1016/0921-4534(96)00003-2 | null | supr-con cond-mat.supr-con | null | The magnetic field distribution, the magnetic flux, and the free energy of an
Abrikosov vortex loop near a flat surface of type--II superconductors are
calculated in the London approximation. The shape of such a vortex line is a
semicircle of arbitrary radius. The interaction of the vortex half--ring and an
external homogeneous magnetic field applied along the surface is studied. The
magnitude of the energy barrier against the vortex expansion into
superconductor is found. The possibilities of formation of an equilibrium
vortex line determined by the structure of the applied magnetic field by
creating the expanding vortex loops near the surface of type--II superconductor
are discussed.
| [
{
"version": "v1",
"created": "Mon, 8 Apr 1996 12:43:47 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Samokhvalov",
"Alexey V.",
"",
"Institute for physics of microstructures,\n Nizhny Novgorod, Russia"
]
] |
supr-con/9604002 | Kamran Behnia | K. Behnia(1), H. Aubin(1), L. Taillefer(2), R. Gagnon(2) ((1)
Universit\'e Paris-Sud (2) McGill University) | Low temperature thermal conductivity of Zn-doped YBCO: evidence for
impurity-induced electronic bound states | 8 pages, 3 Encapsulated Postscript figures | null | null | KB-96-1 | supr-con cond-mat.supr-con | null | The thermal conductivity of Zn-doped YBCO crystals was studied at low
temperature (0.15 < T < 0.8 K) for different concentrations of Zn impurities. A
small amount of Zn induces a dramatic decrease in the non-linear component of
the low-temperature thermal conductivity. Moreover, the magnitude of the linear
component (obtained by extrapolating the data to T=0) is found to depend on Zn
concentration. After an initial decrease, this linear term, associated with the
electronic contribution to the conductivity, increases with increasing Zn
dopage. Such an increase is consistent with the introduction of low-energy
excitations by Zn impurities as expected for a $d_{x^2-y^2}$ superconducting
state in contrast to an anisotropic s-wave gap. The results are compared to
quantitative predictions of available theoretical models.
| [
{
"version": "v1",
"created": "Mon, 22 Apr 1996 16:25:41 GMT"
}
] | 2008-02-03T00:00:00 | [
[
"Behnia",
"K.",
""
],
[
"Aubin",
"H.",
""
],
[
"Taillefer",
"L.",
""
],
[
"Gagnon",
"R.",
""
]
] |
supr-con/9605001 | Prozorov Ruslan | R. Prozorov, A. Poddar, E. Sheriff, A. Shaulov, Y. Yeshurun (Institute
for Superconductivity, Physics Department, Bar-Ilan University, Ramat-Gan,
Israel) | Irreversible magnetization in thin YBCO films rotated in external
magnetic field | 14 pages, 7 PostScript figures | null | 10.1016/0921-4534(96)00266-3 | null | supr-con cond-mat.supr-con | null | The magnetization M of a thin YBaCuO film is measured as a function of the
angle $\theta $ between the applied field H and the c-axis. For fields above
the first critical field, but below the Bean's field for first penetration H*,
M is symmetric with respect to $\theta =\pi $ and the magnetization curves for
forward and backward rotation coincide. For H>H* the curves are asymmetric and
they do not coincide. These phenomena have a simple explanation in the
framework of the Bean critical state model.
| [
{
"version": "v1",
"created": "Thu, 2 May 1996 12:51:14 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Prozorov",
"R.",
"",
"Institute\n for Superconductivity, Physics Department, Bar-Ilan University, Ramat-Gan,\n Israel"
],
[
"Poddar",
"A.",
"",
"Institute\n for Superconductivity, Physics Department, Bar-Ilan University, Ramat-Gan,\n Israel"
],
[
"Sheriff",
"E.",
"",
"Institute\n for Superconductivity, Physics Department, Bar-Ilan University, Ramat-Gan,\n Israel"
],
[
"Shaulov",
"A.",
"",
"Institute\n for Superconductivity, Physics Department, Bar-Ilan University, Ramat-Gan,\n Israel"
],
[
"Yeshurun",
"Y.",
"",
"Institute\n for Superconductivity, Physics Department, Bar-Ilan University, Ramat-Gan,\n Israel"
]
] |
supr-con/9605002 | R. D. Parmentier | C. Soriano, G. Costabile, R. D. Parmentier (INFM & Dept. Physics,
Univ. Salerno) | Coupling of Josephson flux-flow oscillators to an external RC load | uuencoded, gzipped tar archive containing 11 pages of REVTeX text + 4
PostScript figures. To appear in Supercond. Sci. Technol | null | 10.1088/0953-2048/9/7/011 | null | supr-con cond-mat.supr-con | null | We investigate by numerical simulations the behavior of the power dissipated
in a resistive load capacitively coupled to a Josephson flux flow oscillator
and compare the results to those obtained for a d.c. coupled purely resistive
load. Assuming realistic values for the parameters R and C, both in the high-
and in the low-Tc case the power is large enough to allow the operation of such
a device in applications.
| [
{
"version": "v1",
"created": "Sat, 11 May 1996 11:31:51 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Soriano",
"C.",
"",
"INFM & Dept. Physics,\n Univ. Salerno"
],
[
"Costabile",
"G.",
"",
"INFM & Dept. Physics,\n Univ. Salerno"
],
[
"Parmentier",
"R. D.",
"",
"INFM & Dept. Physics,\n Univ. Salerno"
]
] |
supr-con/9606001 | Hagen Kleinert | Hagen Kleinert and Adriaan Schakel | New Universality Class in the Superconductive Phase Transition | Invited talk presented by A. Schakel at the 10'th International
Conference on Problems of Quantum Field Theory, Alushta, Ukraine, May 13-17,
1996. Author Information under
http://www.physik.fu-berlin.de/~kleinert/institution.html; HTML version and
PostScript version of paper available at
http://www.physik.fu-berlin.de/~kleinert/kleiner_re247/preprint.html | null | null | null | supr-con cond-mat.supr-con | null | The superconductive phase transition in the Ginzburg-Landau theory (or
Coulomb-Higgs phase transition of scalar QED in 3D) is discussed in a dual
formulation which focuses on the magnetic rather than the electric excitations
of the system. Renormalization group analysis of the dual formulation reveals
the transition to be of second order and of a new universality class. Whereas
coherence length and specific heat have XY-model exponents, the magnetic
penetration depth shows mean-field behavior. Experimental evidence for these
predictions is discussed.
| [
{
"version": "v1",
"created": "Fri, 14 Jun 1996 05:08:29 GMT"
}
] | 2008-02-03T00:00:00 | [
[
"Kleinert",
"Hagen",
""
],
[
"Schakel",
"Adriaan",
""
]
] |
supr-con/9606002 | Nobuhiko Hayashi | N. Hayashi, M. Ichioka, K. Machida (Okayama Univ.) | Star-shaped Local Density of States around Vortices in a Type II
Superconductor | 4 pages, REVTeX, 3 figures available upon request | Phys. Rev. Lett. 77, 4074 (1996). | 10.1103/PhysRevLett.77.4074 | null | supr-con cond-mat.supr-con | null | The electronic structure of vortices in a type II superconductor is analyzed
within the quasi-classical Eilenberger framework. The possible origin of a
sixfold ``star'' shape of the local density of states, observed by scanning
tunneling microscope experiments on NbSe$_2$, is examined in the light of the
three effects; the anisotropic pairing, the vortex lattice, and the anisotropic
density of states at the Fermi surface. Outstanding features of split parallel
rays of this star are well explained in terms of an anisotropic $s$-wave
pairing. This reveals a rich internal electronic structure associated with a
vortex core.
| [
{
"version": "v1",
"created": "Fri, 21 Jun 1996 09:34:10 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Hayashi",
"N.",
"",
"Okayama Univ."
],
[
"Ichioka",
"M.",
"",
"Okayama Univ."
],
[
"Machida",
"K.",
"",
"Okayama Univ."
]
] |
supr-con/9606003 | Prozorov Ruslan | Y. Abulafia, A. Shaulov, Y. Wolfus, R. Prozorov, L. Burlachkov, and Y.
Yeshurun, D. Majer E. Zeldov, H. W\"uhl, V.B. Geshkenbein, V.M. Vinokur | Plastic vortex-creep in YBa$_2$Cu$_3$O$_{7-x}$ crystals | 10 pages, RevTeX type, 4 PS figures | null | 10.1103/PhysRevLett.77.1596 | null | supr-con cond-mat.supr-con | null | Local magnetic relaxation measurements in YBa$_2$Cu$_3$O$_{7-x}$ crystals
show evidence for plastic vortex-creep associated with the motion of
dislocations in the vortex lattice. This creep mechanism governs the vortex
dynamics in a wide range of temperatures and fields below the melting line and
above the field corresponding to the peak in the ''fishtail'' magnetization. In
this range the activation energy $U_{pl}$, which decreases with field, drops
below the elastic (collective) creep activation energy, $U_{el}$, which
increases with field. A crossover in flux dynamics from elastic to plastic
creep is shown to be the origin of the fishtail in YBa$_2$Cu$_3$O$_{7-x}$.
| [
{
"version": "v1",
"created": "Sat, 22 Jun 1996 23:11:39 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Abulafia",
"Y.",
""
],
[
"Shaulov",
"A.",
""
],
[
"Wolfus",
"Y.",
""
],
[
"Prozorov",
"R.",
""
],
[
"Burlachkov",
"L.",
""
],
[
"Yeshurun",
"Y.",
""
],
[
"Zeldov",
"D. Majer E.",
""
],
[
"Wühl",
"H.",
""
],
[
"Geshkenbein",
"V. B.",
""
],
[
"Vinokur",
"V. M.",
""
]
] |
supr-con/9607001 | Michael Simkin | M.V.Simkin (Brown University) | On Mean-Field Theory of Quantum Phase Transition in Granular
Superconductors | null | Physica C 267 (1996) 161 | 10.1016/0921-4534(96)00376-0 | null | supr-con cond-mat.supr-con | null | In previous work on quantum phase transition in granular superconductors,
where mean-field theory was used, an assumption was made that the order
parameter as a function of the mean field is a convex up function. Though this
is not always the case in phase transitions, this assumption must be verified,
what is done in this article.
| [
{
"version": "v1",
"created": "Sat, 6 Jul 1996 22:27:10 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Simkin",
"M. V.",
"",
"Brown University"
]
] |
supr-con/9607002 | null | J.J. Betouras, R. Joynt, Z.-W. Dong, T. Venkatesan, P. Hadley | Ginzburg-Landau Theory of Josephson Field Effect Transistors | REVTEX, 4 figures upon request, submitted to Appl. Phys. Lett | null | 10.1063/1.117661 | null | supr-con cond-mat.supr-con | null | A theoretical model of high-T_c Josephson Field Effect Transistors (JoFETs)
based on a Ginzburg-Landau free energy expression whose parameters are field-
and spatially- dependent is developed. This model is used to explain
experimental data on JoFETs made by the hole-overdoped Ca-SBCO bicrystal
junctions (three terminal devices). The measurements showed a large modulation
of the critical current as a function of the applied voltage due to charge
modulation in the bicrystal junction. The experimental data agree with the
solutions of the theoretical model. This provides an explanation of the large
field effect, based on the strong suppresion of the carrier density near the
grain boundary junction in the absence of applied field and the subsequent
modulation of the density by the field.
| [
{
"version": "v1",
"created": "Thu, 11 Jul 1996 19:37:23 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Betouras",
"J. J.",
""
],
[
"Joynt",
"R.",
""
],
[
"Dong",
"Z. -W.",
""
],
[
"Venkatesan",
"T.",
""
],
[
"Hadley",
"P.",
""
]
] |
supr-con/9607003 | null | J. I. Martin, M. Velez, F. Guinea and J. L. Vicent | Flux flow resistivity and vortex viscosity of high-Tc films | 3 pages. 4 figures upon request | null | 10.1103/PhysRevB.55.5659 | null | supr-con cond-mat.supr-con | null | The flux flow regime of high-T$_{\rm c}$ samples of different normal state
resistivities is studied in the temperature range where the sign of the Hall
effect is reversed. The scaling of the vortex viscosity with normal state
resistivity is consistent with the Bardeen-Stephen theory. Estimates of the
influence of possible mechanisms suggested for the sign reversal of the Hall
effect are also given.
| [
{
"version": "v1",
"created": "Fri, 12 Jul 1996 15:29:37 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Martin",
"J. I.",
""
],
[
"Velez",
"M.",
""
],
[
"Guinea",
"F.",
""
],
[
"Vicent",
"J. L.",
""
]
] |
supr-con/9607004 | Durga P. Choudhury | S. Sridhar, S. Oxx, B.A. Willemsen, H. Srikanth, and D.P. Choudhury
(Physics Department, Northeastern University) | Comments on "Vortex Glass and Lattice Melting Transitions in a YNi_2B_2C
Single Crystal" | 1 page, LaTeX type, 1 PostScript figure, Uses PRABIB.STY file, 600
dpi PS file available at http://sagar.physics.neu.edu/preprints.html To
appear in Physical Review Letters | null | 10.1103/PhysRevLett.77.2145 | null | supr-con cond-mat.supr-con | null | Recently, Mun et.al. (Phys. Rev. Lett., 76, 2790 (1996)) have published their
results on single crystal YNi_2B_2C, claiming that their experimental
observations can be explained in terms of formation of Vortex Glass and Lattice
melting. Our experiments, carried out on samples obtained from the SAME source,
reveal a much richer phase diagram and span wider regions of experimental
parameter space than Mun et. al. that encompasses most of their observations.
We speculate that this material has anomalous intrinsic properties and the
results cannot be explained by simple models about the flux lattice.
| [
{
"version": "v1",
"created": "Sat, 20 Jul 1996 00:50:25 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Sridhar",
"S.",
"",
"Physics Department, Northeastern University"
],
[
"Oxx",
"S.",
"",
"Physics Department, Northeastern University"
],
[
"Willemsen",
"B. A.",
"",
"Physics Department, Northeastern University"
],
[
"Srikanth",
"H.",
"",
"Physics Department, Northeastern University"
],
[
"Choudhury",
"D. P.",
"",
"Physics Department, Northeastern University"
]
] |
supr-con/9607005 | Franco Nori | C. Reichhardt, J. Groth, C. J. Olson, Stuart Field, Franco Nori | Spatio-temporal dynamics and plastic flow of vortices in superconductors
with periodic arrays of pinning sites | null | Phys. Rev. B 54 (1996) 16108-16115 | 10.1103/PhysRevB.54.16108 | null | supr-con cond-mat.mtrl-sci cond-mat.supr-con nlin.PS patt-sol | null | We present simulations of flux-gradient-driven superconducting rigid vortices
interacting with square and triangular arrays of columnar pinning sites in an
increasing external magnetic field. These simulations allow us to
quantitatively relate spatio-temporal microscopic information of the vortex
lattice with typically measured macroscopic quantities, such as the
magnetization $M(H)$. The flux lattice does not become completely commensurate
with the pinning sites throughout the sample at the magnetization matching
peaks, but forms a commensurate lattice in a region close to the edge of the
sample. Matching fields related to unstable vortex configurations do not
produce peaks in $M(H)$. We observe a variety of evolving complex flux
profiles, including flat terraces or plateaus separated by winding
current-carrying strings and, near the peaks in $M(H)$, plateaus only in
certain regions, which move through the sample as the field increases.
| [
{
"version": "v1",
"created": "Wed, 24 Jul 1996 20:52:19 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Reichhardt",
"C.",
""
],
[
"Groth",
"J.",
""
],
[
"Olson",
"C. J.",
""
],
[
"Field",
"Stuart",
""
],
[
"Nori",
"Franco",
""
]
] |
supr-con/9607006 | Andreas Schoenenberger | A. Sch\"onenberger, A. Larkin, E. Heeb, V. Geshkenbein, G. Blatter | Strong Pinning and Plastic Deformations of the Vortex Lattice | 12 pages, TeX type, Postscript figures | null | 10.1103/PhysRevLett.77.4636 | null | supr-con cond-mat.supr-con | null | We investigate numerically the dynamically generated plastic deformations of
a 3D vortex lattice (VL) driven through a disorder potential with isolated,
strong pinning centers (point-like or extended along the field direction). We
find that the VL exhibits a very peculiar dynamical behavior in the plastic
flow regime, in particular, topological excitations consisting of three or four
entangled vortices are formed. We determine the critical current density $j_c$
and the activation energy for depinning $U_c$ in the presence of a finite
density of strong pinning centers.
| [
{
"version": "v1",
"created": "Fri, 26 Jul 1996 14:13:11 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Schönenberger",
"A.",
""
],
[
"Larkin",
"A.",
""
],
[
"Heeb",
"E.",
""
],
[
"Geshkenbein",
"V.",
""
],
[
"Blatter",
"G.",
""
]
] |
supr-con/9607007 | Frithjof Anders | F. B. Anders and K. Gloos | Towards a Microscopic Theory for Metallic Heavy-Fermion Point Contacts | 3 pages, TeX type, 1 eps figure include, SCES96 Z\"urich | Physica B, 230-232, 437 (1997) | 10.1016/S0921-4526(96)00604-7 | null | supr-con cond-mat.supr-con | null | The bias-dependent resistance R(V) of NS-junctions is calculated using the
Keldysh formalism in all orders of the transfer matrix element. We present a
compact and simple formula for the Andreev current, that results from the
coupling of electrons and holes on the normal side via the anomalous Green's
function on the superconducting side. Using simple BCS Nambu-Green's functions
the well known Blonder-Tinkam-Klapwijk theory can be recovered. Incorporating
the energy-dependent quasi-particle lifetime of the heavy fermions strongly
reduces the Andreev-reflection signal.
| [
{
"version": "v1",
"created": "Fri, 26 Jul 1996 21:05:38 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Anders",
"F. B.",
""
],
[
"Gloos",
"K.",
""
]
] |
supr-con/9608001 | null | Jorge Berger and Jacob Rubinstein (Technion) | Topology and Phase Transitions in the Little-Parks Experiment | Latex, 26 pages, 5 figs upon request | SIAM J Appl Math {\bf 58} (1998) 103--121 | null | null | supr-con cond-mat.supr-con quant-ph | null | This is an analytic study of the problem of transitions between normal and
superconducting phases for a sample which encloses a magnetic flux. A
preliminary study of this problem, based on numerical minimization of the free
energy for a particular form of the thickness of the sample, was published in
Phys. Rev. Lett. {\bf 75}, 320 (1995). For a sample of uniform thickness the
order parameter is uniform, but even infinitesimal deviations from uniform
thickness give rise to a singly connected state in which the order parameter
vanishes at a suitable layer, so that the superconducting part does not enclose
the magnetic field. The stability domain of this singly connected state is a
line segment in the magnetic field-temperature plane, delimited by two critical
points. The phase diagram contains several bifurcation lines, which are
systematically analyzed.
| [
{
"version": "v1",
"created": "Thu, 8 Aug 1996 04:57:12 GMT"
}
] | 2008-02-03T00:00:00 | [
[
"Berger",
"Jorge",
"",
"Technion"
],
[
"Rubinstein",
"Jacob",
"",
"Technion"
]
] |
supr-con/9608002 | Sean M. Quinlan | P. J. Hirschfeld, S. M. Quinlan, and D. J. Scalapino | c-Axis Infrared Conductivity of a d_{x^2-y^2}-Wave Superconductor with
Impurity and Spin-Fluctuation Scattering | 18 pages, 8 Postscript figures, REVTeX 3.0 with psfig macros | null | 10.1103/PhysRevB.55.12742 | null | supr-con cond-mat.supr-con | null | Results of a calculation of the c-axis infrared conductivity sigma_c for a
d_{x^2-y^2}-wave superconductor which include both elastic impurity and
inelastic spin-fluctuation scattering are presented and compared with the
ab-plane conductivity sigma_{ab} in the same model. In this model,the
interlayer c-axis coupling is taken to be weak and diffusive. While in clean
systems, inelastic scattering leads to a peak at omega = 4*Delta_0 in
sigma_{ab} for T < T_c, it has little effect on the corresponding sigma_c,
which exhibits structure only at omega = 2*Delta_0 and is directly related to
the single-particle density of states N(omega). The c-axis penetration depth
lambda_c in the same model is predicted to vary as T^3 at low temperatures in
clean samples. We discuss recent optical experiments on the cuprates and
compare with these predictions.
| [
{
"version": "v1",
"created": "Fri, 9 Aug 1996 23:44:28 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Hirschfeld",
"P. J.",
""
],
[
"Quinlan",
"S. M.",
""
],
[
"Scalapino",
"D. J.",
""
]
] |
supr-con/9608003 | Oleg Tchernyshyov | A. S. Blaer (1), H. C. Ren (2), and O. Tchernyshyov (1) ((1) Columbia
University, (2) Rockefeller University) | Extended bound states and resonances of two fermions on a periodic
lattice | 21 pages, RevTeX, 4 Postscript figures, arithmetic errors corrected.
An abbreviated version (no appendix) appeared in PRB on March 1, 1997 | Phys. Rev. B 55, 6035 (1997) | 10.1103/PhysRevB.55.6035 | CU-TP-771, RU-96-6B | supr-con cond-mat.supr-con | null | The high-$T_c$ cuprates are possible candidates for d-wave superconductivity,
with the Cooper pair wave function belonging to a non-trivial irreducible
representation of the lattice point group. We argue that this d-wave symmetry
is related to a special form of the fermionic kinetic energy and does not
require any novel pairing mechanism. In this context, we present a detailed
study of the bound states and resonances formed by two lattice fermions
interacting via a non-retarded potential that is attractive for nearest
neighbors but repulsive for other relative positions. In the case of strong
binding, a pair formed by fermions on adjacent lattice sites can have a small
effective mass, thereby implying a high condensation temperature. For a weakly
bound state, a pair with non-trivial symmetry tends to be smaller in size than
an s-wave pair. These and other findings are discussed in connection with the
properties of high-$T_c$ cuprate superconductors.
| [
{
"version": "v1",
"created": "Mon, 12 Aug 1996 16:00:41 GMT"
},
{
"version": "v2",
"created": "Thu, 13 Mar 1997 13:59:10 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Blaer",
"A. S.",
""
],
[
"Ren",
"H. C.",
""
],
[
"Tchernyshyov",
"O.",
""
]
] |
supr-con/9608004 | Georg Bruun | G. M. Bruun, V. N. Nicopoulos, N. F. Johnson | Ginzburg-Landau-Gor'kov Theory of Magnetic oscillations in a type-II
2-dimensional Superconductor | 39 pages, 8 figures. This is a replacement of supr-con/9608004.
Several sections changed or added, including a section on the effect of spin
and the effect of a conserved number of particles. To be published in Phys.
Rev. B | PHYS REV B 56: (2) 809-825 JUL 1 1997 | 10.1103/PhysRevB.56.809 | null | supr-con cond-mat.supr-con | null | We investigate de Haas-van Alphen (dHvA) oscillations in the mixed state of a
type-II two-dimensional superconductor within a self-consistent Gor'kov
perturbation scheme. Assuming that the order parameter forms a vortex lattice
we can calculate the expansion coefficients exactly to any order. We have
tested the results of the perturbation theory to fourth and eight order against
an exact numerical solution of the corresponding Bogoliubov-de Gennes
equations. The perturbation theory is found to describe the onset of
superconductivity well close to the transition point $H_{c2}$. Contrary to
earlier calculations by other authors we do not find that the perturbative
scheme predicts any maximum of the dHvA-oscillations below $H_{c2}$. Instead we
obtain a substantial damping of the magnetic oscillations in the mixed state as
compared to the normal state. We have examined the effect of an oscillatory
chemical potential due to particle conservation and the effect of a finite
Zeeman splitting. Furthermore we have investigated the recently debated issue
of a possibility of a sign change of the fundamental harmonic of the magnetic
oscillations. Our theory is compared with experiment and we have found good
agreement.
| [
{
"version": "v1",
"created": "Wed, 14 Aug 1996 16:35:44 GMT"
},
{
"version": "v2",
"created": "Mon, 19 Aug 1996 14:07:39 GMT"
},
{
"version": "v3",
"created": "Fri, 11 Apr 1997 22:08:12 GMT"
}
] | 2016-09-08T00:00:00 | [
[
"Bruun",
"G. M.",
""
],
[
"Nicopoulos",
"V. N.",
""
],
[
"Johnson",
"N. F.",
""
]
] |
supr-con/9608005 | Robert B. Laughlin | R. B. Laughlin (Stanford) | Evidence for Quasiparticle Decay in Photoemission from Underdoped
Cuprates | 4 pages of ReVTeX, 3 eps figures | Phys. Rev. Lett. 79, 1726 (1997) | 10.1103/PhysRevLett.79.1726 | p01jul96 | supr-con cond-mat.supr-con | null | I argue that the ``gap'' recently observed at the Brillouin zone face of
cuprate superconductors in photoemission by Marshall et al [Phys. Rev. Lett.
76, 4841 (1996)] and Ding et al [Nature 382, 54 (1996)] is evidence for the
decay of the injected hole into a spinon-holon pair.
| [
{
"version": "v1",
"created": "Thu, 15 Aug 1996 01:08:36 GMT"
},
{
"version": "v2",
"created": "Sun, 8 Feb 1998 19:42:41 GMT"
},
{
"version": "v3",
"created": "Tue, 17 Feb 1998 17:28:22 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Laughlin",
"R. B.",
"",
"Stanford"
]
] |
supr-con/9608006 | Bozidar Mitrovic | B. Mitrovic and M. Castle (Brock University, Canada) | Strong coupling theory of the interlayer tunneling model for high
temperature superconductors | 23 pages, 7 Postscript figures, REVTeX 3.0 with epsf macros | null | 10.1088/0953-8984/9/42/015 | null | supr-con cond-mat.supr-con | null | The interlayer pair tunneling model of Anderson et al. is generalized to
include the strong coupling effects associated with in-plane interactions. The
equations for the superconducting transition temperature T_{c} are solved
numerically for several models of electron-optical phonon coupling. The
nonmagnetic in-plane impurity scattering suppresses T_{c} in all cases
considered, and it is possible to obtain a fair agreement with experiments for
a reasonable choice of parameters. For the anisotropic electron-phonon coupling
proposed by Song and Annett we find that the interlayer pair tunneling can
stabilize the d_{x^2-y^2}-wave superconducting state with a high T_{c}.
Moreover, in this case there is a possibility of an impurity induced crossover
from the d$_{x^2-y^2}$-wave state stabilized by the interlayer tunneling to the
s-wave state at a low impurity concentration. We also calculate the isotope
effect associated with the in-plane oxygen optic mode and its dependence on the
strength of the interlayer pair tunneling. Small positive values of the isotope
exponent are obtained for strengths of pair tunneling that give high transition
temperatures.
| [
{
"version": "v1",
"created": "Thu, 15 Aug 1996 17:16:38 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Mitrovic",
"B.",
"",
"Brock University, Canada"
],
[
"Castle",
"M.",
"",
"Brock University, Canada"
]
] |
supr-con/9608007 | null | Francesca Federici, Andrei A. Varlamov | The Fluctuation Induced Pseudogap in the Infrared Optical Conductivity
of High Temperature Superconductors | 8 pages, 4 eps figures, Submitted to Phys. Rev. B | null | 10.1103/PhysRevB.55.6070 | null | supr-con cond-mat.supr-con | null | We study the effect of fluctuations on the {\bf ac} conductivity of a layered
superconductor both for $c$-axis and $ab$-plane electromagnetic wave
polarizations. The fluctuation contributions of different physical nature and
signs (paraconductivity, Maki-Thompson anomalous contribution, one-electron
density of states renormalization) are found to be suppressed by the external
field at different characterisitic frequencies ($ \omega_{\rm AL}\sim T-T_{\rm
c}$, $\omega_{\rm MT} \sim \max\{ T-T_{\rm c}, \tau_{\varphi}^{-1}\}$, $
\omega_{\rm DOS} \sim \min\{T,\tau ^{-1}\}$ for the $2D$ case). As a result the
appearance of the nonmonotonic frequency dependence (pseudogap) in the infrared
optical conductivity of HTS film is predicted. The effect has to be especially
pronounced in the case of the electromagnetic field polarization along
$c$-axis.
| [
{
"version": "v1",
"created": "Fri, 23 Aug 1996 09:39:49 GMT"
},
{
"version": "v2",
"created": "Wed, 28 Aug 1996 11:54:46 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Federici",
"Francesca",
""
],
[
"Varlamov",
"Andrei A.",
""
]
] |
supr-con/9608008 | Ruslan Prozorov | R. Prozorov, M. Konczykowski, B. Schmidt, Y. Yeshurun, A. Shaulov, C.
Villard, G. Koren | On the origin of the irreversibility line in thin YBaCuO7 films with and
without columnar defects | 19 pages, LaTex, 6 PostScript figures; Author's Homepage:
http://www.biu.ac.il:80/~prozorr | null | 10.1103/PhysRevB.54.15530 | null | supr-con cond-mat.supr-con | null | We report on measurements of the angular dependence of the irreversibility
temperature $T_{irr}(\theta) $ in $YBa_2Cu_3O_{7-\delta }$ thin films, defined
by the onset of a third harmonic signal and measured by a miniature Hall probe.
From the functional form of $T_{irr}(\theta)$ we conclude that the origin of
the irreversibility line in unirradiated films is a dynamic crossover from an
unpinned to a pinned vortex liquid. In irradiated films the irreversibility
temperature is determined by the trapping angle.
| [
{
"version": "v1",
"created": "Mon, 26 Aug 1996 15:08:35 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Prozorov",
"R.",
""
],
[
"Konczykowski",
"M.",
""
],
[
"Schmidt",
"B.",
""
],
[
"Yeshurun",
"Y.",
""
],
[
"Shaulov",
"A.",
""
],
[
"Villard",
"C.",
""
],
[
"Koren",
"G.",
""
]
] |
supr-con/9609001 | Durga P. Choudhury | Durga P. Choudhury, Balam A. Willemsen, John S. Derov and S. Sridhar
(Physics Department, Northeastern University and Rome Laboratory, Hanscom
AFB.) | Nonlinear Response of HTSC Thin Film Microwave Resonators in an Applied
DC Magnetic Field | 4 pages, LaTeX type, Uses IEEE style files, 600 dpi PostScript file
with color figures available at http://sagar.physics.neu.edu/preprints.html
Submitted to IEEE Transactions on Applied Superconductivity | null | 10.1109/77.620744 | null | supr-con cond-mat.supr-con | null | The non-linear microwave surface impedance of patterned YBCO thin films, was
measured using a suspended line resonator in the presence of a perpendicular DC
magnetic field of magnitude comparable to that of the microwave field.
Signature of the virgin state was found to be absent even for relatively low
microwave power levels. The microwave loss was initially found to decrease for
small applied DC field before increasing again. Also, non-linearities inherent
in the sample were found to be substantially suppressed at low powers at these
applied fields. These two features together can lead to significant improvement
in device performance.
| [
{
"version": "v1",
"created": "Sat, 31 Aug 1996 17:34:38 GMT"
}
] | 2016-11-18T00:00:00 | [
[
"Choudhury",
"Durga P.",
"",
"Physics Department, Northeastern University and Rome Laboratory, Hanscom\n AFB."
],
[
"Willemsen",
"Balam A.",
"",
"Physics Department, Northeastern University and Rome Laboratory, Hanscom\n AFB."
],
[
"Derov",
"John S.",
"",
"Physics Department, Northeastern University and Rome Laboratory, Hanscom\n AFB."
],
[
"Sridhar",
"S.",
"",
"Physics Department, Northeastern University and Rome Laboratory, Hanscom\n AFB."
]
] |
supr-con/9609002 | Durga P. Choudhury | Balam A. Willemsen, J. S. Derov and S.Sridhar (Physics Department,
Northeastern University and Rome Laboratory, Hanscom AFB) | Critical State Flux Penetration and Linear Microwave Vortex Response in
YBa_2Cu_3O_{7-x} Films | 20 pages, LaTeX type, Uses REVTeX style files, Submitted to Physical
Review B, 600 dpi PostScript file with high resolution figures available at
http://sagar.physics.neu.edu/preprints.html | null | 10.1103/PhysRevB.56.11989 | null | supr-con cond-mat.supr-con | null | The vortex contribution to the dc field (H) dependent microwave surface
impedance Z_s = R_s+iX_s of YBa_2Cu_3O_{7-x} thin films was measured using
suspended patterned resonators. Z_s(H) is shown to be a direct measure of the
flux density B(H) enabling a very precise test of models of flux penetration.
Three regimes of field-dependent behavior were observed: (1) Initial flux
penetration occurs on very low field scales H_i(4.2K) 100Oe, (2) At moderate
fields the flux penetration into the virgin state is in excellent agreement
with calculations based upon the field-induced Bean critical state for thin
film geometry, parametrized by a field scale H_s(4.2K) J_c*d 0.5T, (3) for very
high fields H >>H_s, the flux density is uniform and the measurements enable
direct determination of vortex parameters such as pinning force constants
\alpha_p and vortex viscosity \eta. However hysteresis loops are in
disagreement with the thin film Bean model, and instead are governed by the low
field scale H_i, rather than by H_s. Geometric barriers are insufficient to
account for the observed results.
| [
{
"version": "v1",
"created": "Tue, 3 Sep 1996 14:08:26 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Willemsen",
"Balam A.",
"",
"Physics Department,\n Northeastern University and Rome Laboratory, Hanscom AFB"
],
[
"Derov",
"J. S.",
"",
"Physics Department,\n Northeastern University and Rome Laboratory, Hanscom AFB"
],
[
"Sridhar",
"S.",
"",
"Physics Department,\n Northeastern University and Rome Laboratory, Hanscom AFB"
]
] |
supr-con/9609003 | Hasegawa Yasumasa | Yasumasa Hasegawa (Himeji Institute of Technology) | Density of States and NMR Relaxation Rate in Anisotropic
Superconductivity with Intersecting Line Nodes | 7 pages, 4 PostScript Figures, LaTeX, to appear in J. Phys. Soc. Jpn | null | 10.1143/JPSJ.65.3131 | null | supr-con cond-mat.supr-con | null | We show that the density of states in an anisotropic superconductor with
intersecting line nodes in the gap function is proportional to $E log (\alpha
\Delta_0 /E)$ for $|E| << \Delta_0$, where $\Delta_0$ is the maximum value of
the gap function and $\alpha$ is constant, while it is proportional to $E$ if
the line nodes do not intersect. As a result, a logarithmic correction appears
in the temperature dependence of the NMR relaxation rate and the specific heat,
which can be observed experimentally. By comparing with those for the heavy
fermion superconductors, we can obtain information about the symmetry of the
gap function.
| [
{
"version": "v1",
"created": "Wed, 18 Sep 1996 07:57:29 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Hasegawa",
"Yasumasa",
"",
"Himeji Institute of Technology"
]
] |
supr-con/9609004 | Masanori Ichioka | Naoki Enomoto, Masanori Ichioka and Kazushige Machida (Okayama Univ.) | Ginzburg Landau theory for d-wave pairing and fourfold symmetric vortex
core structure | 12 pages including 8 eps figs, LaTeX with jpsj.sty & epsfig | J. Phys. Soc. Jpn. 66, 204 (1997). | 10.1143/JPSJ.66.204 | null | supr-con cond-mat.supr-con | null | The Ginzburg Landau theory for d_{x^2-y^2}-wave superconductors is
constructed, by starting from the Gor'kov equation with including correction
terms up to the next order of ln(T_c/T). Some of the non-local correction terms
are found to break the cylindrical symmetry and lead to the fourfold symmetric
core structure, reflecting the internal degree of freedom in the pair
potential. Using this extended Ginzburg Landau theory, we investigate the
fourfold symmetric structure of the pair potential, current and magnetic field
around an isolated single vortex, and clarify concretely how the vortex core
structure deviates from the cylindrical symmetry in the d_{x^2-y^2}-wave
superconductors.
| [
{
"version": "v1",
"created": "Wed, 25 Sep 1996 14:17:09 GMT"
}
] | 2009-10-30T00:00:00 | [
[
"Enomoto",
"Naoki",
"",
"Okayama Univ."
],
[
"Ichioka",
"Masanori",
"",
"Okayama Univ."
],
[
"Machida",
"Kazushige",
"",
"Okayama Univ."
]
] |