4,816 research outputs found
Properties of small HTSC mesa structures: common problems of interlayer tunneling
I analyze common problems of interlayer tunneling in Bi-2212 mesa structures,
such as self-heating and nonuniformity of junctions. Numerical simulations have
shown that self-heating does not mask the temperature dependence of the
superconducting gap. Major problems can be avoided by decreasing mesa sizes.Comment: 3 pages, 4 figures, presentation at EUCAS-2001 (Copenhagen, August
2001) Subm. to Physica
Stacked Josephson junction SQUID
Operation of a Superconducting Quantum Interference Device (SQUID) made of
stacked Josephson junctions is analyzed numerically for a variety of junction
parameters. Due to a magnetic coupling of junctions in the stack, such a SQUID
has certain advantages as compared to an uncoupled multi-junction SQUID.
Namely, metastability of current-flux modulation can be reduced and a
voltage-flux modulation can be improved if junctions in the stack are
phase-locked. Optimum operation of the SQUID is expected for moderately long,
strongly coupled stacked Josephson junctions. A possibility of making a stacked
Josephson junction SQUID based on intrinsic Josephson junctions in high-Tc
superconductor is discussed.Comment: 4 pages, 3 figures, presented at SQUID-2001 (Stenungsbaden September
2001
Intrinsic tunneling spectroscopy: A look from the inside at HTSC
Layered structure of Bi-2212 high superconductor (HTSC), provides a
unique opportunity to probe quasiparticle density of states inside a bulk
single crystal by means of intrinsic (interlayer) tunneling spectroscopy. Here
I present a systematic study of intrinsic tunneling characteristics of Bi-2212
as a function of doping, temperature, magnetic field and intercalation. An
improved resolution made it possible to simultaneously trace the
superconducting gap (SG) and the normal state pseudo-gap (PG) in a close
vicinity of and to analyze closing of the PG at . The obtained
doping phase diagram exhibits a critical doping point for appearance of the PG
and a characteristic crossing of the SG and the PG close to the optimal doping.
All this points towards coexistence of two different and competing order
parameters in Bi-2212.Comment: 4 pages, 5 figures, Presentation at M2S-Rio (May 2003), Subm. to
Physica C. Note: A discussion of magnetic field dependencies is adde
Cosmological perturbations in a family of deformations of general relativity
We study linear cosmological perturbations in a previously introduced family
of deformations of general relativity characterized by the absence of new
degrees of freedom. The homogeneous and isotropic background in this class of
theories is unmodified and is described by the usual Friedmann equations. The
theory of cosmological perturbations is modified and the relevant deformation
parameter has the dimension of length. Gravitational perturbations of the
scalar type can be described by a certain relativistic potential related to the
matter perturbations just as in general relativity. A system of differential
equations describing the evolution of this potential and of the stress-energy
density perturbations is obtained. We find that the evolution of scalar
perturbations proceeds with a modified effective time-dependent speed of sound,
which, contrary to the case of general relativity, does not vanish even at the
matter-dominated stage. In a broad range of values of the length parameter
controlling the deformation, a specific transition from the regime of modified
gravity to the regime of general relativity in the evolution of scalar
perturbations takes place during the radiation domination. In this case, the
resulting power spectrum of perturbations in radiation and dark matter is
suppressed on the comoving spatial scales that enter the Hubble radius before
this transition. We estimate the bounds on the deformation parameter for which
this suppression does not lead to observable consequences. Evolution of scalar
perturbations at the inflationary stage is modified but very slightly and the
primordial spectrum generated during inflation is not noticeably different from
the one obtained in general relativity.Comment: 45 pages, version published in JCAP; minor changes, one section moved
to the appendi
Twistors, CFT and Holography
According to one of many equivalent definitions of twistors a (null) twistor
is a null geodesic in Minkowski spacetime. Null geodesics can intersect at
points (events). The idea of Penrose was to think of a spacetime point as a
derived concept: points are obtained by considering the incidence of twistors.
One needs two twistors to obtain a point. Twistor is thus a ``square root'' of
a point. In the present paper we entertain the idea of quantizing the space of
twistors. Twistors, and thus also spacetime points become operators acting in a
certain Hilbert space. The algebra of functions on spacetime becomes an
operator algebra. We are therefore led to the realm of non-commutative
geometry. This non-commutative geometry turns out to be related to conformal
field theory and holography. Our construction sheds an interesting new light on
bulk/boundary dualities.Comment: 21 pages, figure
GR uniqueness and deformations
In the metric formulation gravitons are described with the parity symmetric
representation of Lorentz group. General Relativity is
then the unique theory of interacting gravitons with second order field
equations. We show that if a chiral representation is used
instead, the uniqueness is lost, and there is an infinite-parametric family of
theories of interacting gravitons with second order field equations. We use the
language of graviton scattering amplitudes, and show how the uniqueness of GR
is avoided using simple dimensional analysis. The resulting distinct from GR
gravity theories are all parity asymmetric, but share the GR MHV amplitudes.
They have new all same helicity graviton scattering amplitudes at every
graviton order. The amplitudes with at least one graviton of opposite helicity
continue to be determinable by the BCFW recursion.Comment: v2: published version, 19 pages, description of the complexified
setting expande
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