21,627 research outputs found
Intersection numbers for normal functions
We expand the notion of a normal function for a Hodge class on an
even-dimensional complex projective manifold to the notion of a 'topological
normal function' associated to any primitive integral cohomology class. The
definition of the intersection number of two topological normal functions is
the analogue of that given by Griffiths and Green for classical normal
functions. We give a simple proof that the intersection number of the normal
functions is the same as the intersection number of their corresponding
cohomology classes.Comment: 7 page
Collisional invariants for the phonon Boltzmann equation
For the phonon Boltzmann equation with only pair collisions we characterize
the set of all collisional invariants under some mild conditions on the
dispersion relation
The Geometry of Niggli Reduction I: The Boundary Polytopes of the Niggli Cone
Correct identification of the Bravais lattice of a crystal is an important
step in structure solution. Niggli reduction is a commonly used technique. We
investigate the boundary polytopes of the Niggli-reduced cone in the
six-dimensional space G6 by algebraic analysis and organized random probing of
regions near 1- through 8-fold boundary polytope intersections. We limit
consideration of boundary polytopes to those avoiding the mathematically
interesting but crystallographically impossible cases of 0 length cell edges.
Combinations of boundary polytopes without a valid intersection in the closure
of the Niggli cone or with an intersection that would force a cell edge to 0 or
without neighboring probe points are eliminated. 216 boundary polytopes are
found: 15 5-D boundary polytopes of the full G6 Niggli cone, 53 4-D boundary
polytopes resulting from intersections of pairs of the 15 5-D boundary
polytopes, 79 3-D boundary polytopes resulting from 2-fold, 3-fold and 4-fold
intersections of the 15 5-D boundary polytopes, 55 2-D boundary polytopes
resulting from 2-fold, 3-fold, 4-fold and higher intersections of the 15 5-D
boundary polytopes, 14 1-D boundary polytopes resulting from 3-fold and higher
intersections of the 15 5-D boundary polytopes. All primitive lattice types can
be represented as combinations of the 15 5-D boundary polytopes. All
non-primitive lattice types can be represented as combinations of the 15 5-D
boundary polytopes and of the 7 special-position subspaces of the 5-D boundary
polytopes. This study provides a new, simpler and arguably more intuitive basis
set for the classification of lattice characters and helps to illuminate some
of the complexities in Bravais lattice identification. The classification is
intended to help in organizing database searches and in understanding which
lattice symmetries are "close" to a given experimentally determined cell
Aharonov-Bohm oscillations and resonant tunneling in strongly correlated quantum dots
We investigate Aharonov-Bohm oscillations of the current through a strongly
correlated quantum dot embedded in an arbitrary scattering geometry.
Resonant-tunneling processes lead to a flux-dependent renormalization of the
dot level. As a consequence we obtain a fine structure of the current
oscillations which is controlled by quantum fluctuations. Strong Coulomb
repulsion leads to a continuous bias voltage dependent phase shift and, in the
nonlinear response regime, destroys the symmetry of the differential
conductance under a sign change of the external flux.Comment: RevTex, 5 pages, 3 PostScript figures. Accepted for publication in
Phys. Rev. Let
The Geometry of Niggli Reduction II: BGAOL -- Embedding Niggli Reduction
Niggli reduction can be viewed as a series of operations in a six-dimensional
space derived from the metric tensor. An implicit embedding of the space of
Niggli-reduced cells in a higher dimensional space to facilitate calculation of
distances between cells is described. This distance metric is used to create a
program, BGAOL, for Bravais lattice determination. Results from BGAOL are
compared to the results from other metric-based Bravais lattice determination
algorithms
Experience with advanced instrumentation in a hot section cascade
The Lewis Research Center gas turbine Hot Section Test Facility was developed to provide a real engine environment with known boundary conditions for the aerothermal performance evaluation and verification of computer design codes. This verification process requires experimental measurements in a hostile environment. The research instruments used in this facility are presented, and their characteristics and how they perform in this environment are discussed. The research instrumentation consisted of conventional pressure and temperature sensors, as well as thin-film thermocouples and heat flux gages. The hot gas temperature was measured by an aspirated temperature probe and by a dual-element, fast-response temperature probe. The data acquisition mode was both steady state and time dependent. These experiments were conducted over a wide range of gas Reynolds numbers, exit gas Mach numbers, and heat flux levels. This facility was capable of testing at temperatures up to 1600 K, and at pressures up to 18 atm. These corresponded to an airfoil exit Reynolds number range of 0.5 x 10(6) to 2.5 x 10(6) based on the airfoil chord of 5.55 cm. The results characterize the performance capability and the durability of the instrumentation. The challenge of making measurements in hostile environments is also discussed. The instruments exhibited more than adequate durability to achieve the measurement profile. About 70 percent of the thin-film thermocouples and the dual-element temperature probe survived several hundred thermal cycles and more than 35 hr at gas temperatures up to 1600 K. Within the experimental uncertainty, the steady-state and transient heat flux measurements were comparable and consistent over the range of Reynolds numbers tested
- …