10,794 research outputs found
Generic Misalignment Aberration Patterns in Wide-Field Telescopes
Axially symmetric telescopes produce well known "Seidel" off-axis third-order
aberration patterns: coma, astigmatism, curvature of field and distortion. When
axial symmetry is broken by the small misalignments of optical elements,
additional third-order aberration patterns arise: one each for coma,
astigmatism and curvature of field and two for distortion. Each of these
misalignment patterns is characterized by an associated two-dimensional vector,
each of which in turn is a linear combination of the tilt and decenter vectors
of the individual optical elements. For an N-mirror telescope, 2(N-1) patterns
must be measured to keep the telescope aligned. Alignment of the focal plane
may require two additional patterns. For N = 3, as in a three mirror
anastigmat, there is a two-dimensional "subspace of benign misalignment" over
which the misalignment patterns for third-order coma, astigmatism and curvature
of field are identically zero. One would need to measure at least one of the
two distortion patterns to keep the telescope aligned. Alternatively, one might
measure one of the fifth-order misalignment patterns, which are derived herein.
But the fifth-order patterns are rather insensitive to misalignments, even with
moderately wide fields, rendering them of relatively little use in telescope
alignment. Another alternative would be to use telescope pointing as part of
the alignment solution.Comment: 50 pages, 13 figures, Accepted for Publication in PAS
Giant isotope effect in the incoherent tunneling specific heat of the molecular nanomagnet Fe8
Time-dependent specific heat experiments on the molecular nanomagnet Fe8 and
the isotopic enriched analogue 57Fe8 are presented. The inclusion of the 57Fe
nuclear spins leads to a huge enhancement of the specific heat below 1 K,
ascribed to a strong increase in the spin-lattice relaxation rate Gamma arising
from incoherent, nuclear-spin-mediated magnetic quantum tunneling in the
ground-doublet. Since Gamma is found comparable to the expected tunneling rate,
the latter process has to be inelastic. A model for the coupling of the
tunneling levels to the lattice is presented. Under transverse field, a
crossover from nuclear-spin-mediated to phonon-induced tunneling is observed.Comment: Replaced with version accepted for publication in Physical Review
Letter
Quantum dot dephasing by edge states
We calculate the dephasing rate of an electron state in a pinched quantum
dot, due to Coulomb interactions between the electron in the dot and electrons
in a nearby voltage biased ballistic nanostructure. The dephasing is caused by
nonequilibrium time fluctuations of the electron density in the nanostructure,
which create random electric fields in the dot. As a result, the electron level
in the dot fluctuates in time, and the coherent part of the resonant
transmission through the dot is suppressed
Acoustoelectric current and pumping in a ballistic quantum point contact
The acoustoelectric current induced by a surface acoustic wave (SAW) in a
ballistic quantum point contact is considered using a quantum approach. We find
that the current is of the "pumping" type and is not related to drag, i.e. to
the momentum transfer from the wave to the electron gas. At gate voltages
corresponding to the plateaus of the quantized conductance the current is
small. It is peaked at the conductance step voltages. The peak current
oscillates and decays with increasing SAW wavenumber for short wavelengths.
These results contradict previous calculations, based on the classical
Boltzmann equation.Comment: 4 pages, 1 figur
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