25,312 research outputs found
Remote spectral imaging with simultaneous extraction of 3D topography for historical wall paintings
PRISMS (Portable Remote Imaging System for Multispectral Scanning) is designed for in situ, simultaneous high resolution spectral and 3D topographic imaging of wall paintings and other large surfaces. In particular, it can image at transverse resolutions of tens of microns remotely from distances of tens of metres, making high resolution imaging possible from a fixed position on the ground for areas at heights that is difficult to access. The spectral imaging system is fully automated giving 3D topographic mapping at millimetre accuracy as a by-product of the image focusing process. PRISMS is the first imaging device capable of both 3D mapping and spectral imaging simultaneously without additional distance measuring devices. Examples from applications of PRISMS to wall paintings at a UNESCO site in the Gobi desert are presented to demonstrate the potential of the instrument for large scale 3D spectral imaging, revealing faded writing and material identification
The potential of targeted antiangiogenesis therapies in the treatment of esophageal cancer
published_or_final_versio
Slip energy barriers in aluminum and implications for ductile versus brittle behavior
We conisder the brittle versus ductile behavior of aluminum in the framework
of the Peierls-model analysis of dislocation emission from a crack tip. To this
end, we perform first-principles quantum mechanical calculations for the
unstable stacking energy of aluminum along the Shockley partial
slip route. Our calculations are based on density functional theory and the
local density approximation and include full atomic and volume relaxation. We
find that in aluminum J/m. Within the Peierls-model
analysis, this value would predict a brittle solid which poses an interesting
problem since aluminum is typically considered ductile. The resolution may be
given by one of three possibilites: (a) Aluminum is indeed brittle at zero
temperature, and becomes ductile at a finite temperature due to motion of
pre-existing dislocations which relax the stress concentration at the crack
tip. (b) Dislocation emission at the crack tip is itself a thermally activated
process. (c) Aluminum is actually ductile at all temperatures and the
theoretical model employed needs to be significantly improved in order to
resolve the apparent contradiction.Comment: 4 figures (not included; send requests to [email protected]
Aharonov-Bohm oscillations in a mesoscopic ring with a quantum dot
We present an analysis of the Aharonov-Bohm oscillations for a mesoscopic
ring with a quantum dot inserted in one of its arms. It is shown that
microreversibility demands that the phase of the Aharonov-Bohm oscillations
changes {\it abruptly} when a resonant level crosses the Fermi energy. We use
the Friedel sum rule to discuss the conservation of the parity of the
oscillations at different conductance peaks. Our predictions are illustrated
with the help of a simple one channel model that permits the variation of the
potential landscape along the ring.Comment: 11 pages, Revtex style, 3 figures under request. Submitted to Phys.
Rev. B (rapid communications
Transfer-matrix scaling from disorder-averaged correlation lengths for diluted Ising systems
A transfer matrix scaling technique is developed for randomly diluted
systems, and applied to the site-diluted Ising model on a square lattice in two
dimensions. For each allowed disorder configuration between two adjacent
columns, the contribution of the respective transfer matrix to the decay of
correlations is considered only as far as the ratio of its two largest
eigenvalues, allowing an economical calculation of a configuration-averaged
correlation length. Standard phenomenological-renormalisation procedures are
then used to analyse aspects of the phase boundary which are difficult to
assess accurately by alternative methods. For magnetic site concentration
close to , the extent of exponential behaviour of the curve
is clearly seen for over two decades of variation of . Close to the
pure-system limit, the exactly-known reduced slope is reproduced to a very good
approximation, though with non-monotonic convergence. The averaged correlation
lengths are inserted into the exponent-amplitude relationship predicted by
conformal invariance to hold at criticality. The resulting exponent
remains near the pure value (1/4) for all intermediate concentrations until it
crosses over to the percolation value at the threshold.Comment: RevTeX 3, 11 pages +5 figures, uuencoded, to appear in Phys. Rev. B
(1994), PUC/RJ preprin
The Scaling Behavior of Classical Wave Transport in Mesoscopic Media at the Localization Transition
The propagation of classical wave in disordered media at the Anderson
localization transition is studied. Our results show that the classical waves
may follow a different scaling behavior from that for electrons. For electrons,
the effect of weak localization due to interference of recurrent scattering
paths is limited within a spherical volume because of electron-electron or
electron-phonon scattering, while for classical waves, it is the sample
geometry that determine the amount of recurrent scattering paths that
contribute. It is found that the weak localization effect is weaker in both
cubic and slab geometry than in spherical geometry. As a result, the averaged
static diffusion constant D(L) scales like ln(L)/L in cubic or slab geometry
and the corresponding transmission follows ~ln L/L^2. This is in contrast
to the behavior of D(L)~1/L and ~1/L^2 obtained previously for electrons
or spherical samples. For wave dynamics, we solve the Bethe-Salpeter equation
in a disordered slab with the recurrent scattering incorporated in a
self-consistent manner. All of the static and dynamic transport quantities
studied are found to follow the scaling behavior of D(L). We have also
considered position-dependent weak localization effects by using a plausible
form of position-dependent diffusion constant D(z). The same scaling behavior
is found, i.e., ~ln L/L^2.Comment: 11 pages, 12 figures. Submitted to Phys. Rev. B on 3 May 200
What is the Thouless Energy for Ballistic Systems?
The Thouless energy, \Ec characterizes numerous quantities associated with
sensitivity to boundary conditions in diffusive mesoscopic conductors. What
happens to these quantities if the disorder strength is decreased and a
transition to the ballistic regime takes place? In the present analysis we
refute the intuitively plausible assumption that \Ec loses its meaning as an
inverse diffusion time through the system at hand, and generally disorder
independent scales take over. Instead we find that a variety of (thermodynamic)
observables are still characterized by the Thouless energy.Comment: 4 pages REVTEX, uuencoded file. To appear in Physical Review Letter
- …