1,057 research outputs found
Elliptic Quantum Billiard
The exact and semiclassical quantum mechanics of the elliptic billiard is
investigated. The classical system is integrable and exhibits a separatrix,
dividing the phasespace into regions of oscillatory and rotational motion. The
classical separability carries over to quantum mechanics, and the Schr\"odinger
equation is shown to be equivalent to the spheroidal wave equation. The quantum
eigenvalues show a clear pattern when transformed into the classical action
space. The implication of the separatrix on the wave functions is illustrated.
A uniform WKB quantization taking into account complex orbits is shown to be
adequate for the semiclassical quantization in the presence of a separatrix.
The pattern of states in classical action space is nicely explained by this
quantization procedure. We extract an effective Maslov phase varying smoothly
on the energy surface, which is used to modify the Berry-Tabor trace formula,
resulting in a summation over non-periodic orbits. This modified trace formula
produces the correct number of states, even close to the separatrix. The
Fourier transform of the density of states is explained in terms of classical
orbits, and the amplitude and form of the different kinds of peaks is
analytically calculated.Comment: 33 pages, Latex2e, 19 figures,macros: epsfig, amssymb, amstext,
submitted to Annals of Physic
Inertial waves in a rotating spherical shell: attractors and asymptotic spectrum
We investigate the asymptotic properties of inertial modes confined in a
spherical shell when viscosity tends to zero. We first consider the mapping
made by the characteristics of the hyperbolic equation (Poincar\'e's equation)
satisfied by inviscid solutions. Characteristics are straight lines in a
meridional section of the shell, and the mapping shows that, generically, these
lines converge towards a periodic orbit which acts like an attractor.
We then examine the relation between this characteristic path and
eigensolutions of the inviscid problem and show that in a purely
two-dimensional problem, convergence towards an attractor means that the
associated velocity field is not square-integrable. We give arguments which
generalize this result to three dimensions. We then consider the viscous
problem and show how viscosity transforms singularities into internal shear
layers which in general betray an attractor expected at the eigenfrequency of
the mode. We find that there are nested layers, the thinnest and most internal
layer scaling with -scale, being the Ekman number. Using an
inertial wave packet traveling around an attractor, we give a lower bound on
the thickness of shear layers and show how eigenfrequencies can be computed in
principle. Finally, we show that as viscosity decreases, eigenfrequencies tend
towards a set of values which is not dense in , contrary to the
case of the full sphere ( is the angular velocity of the system).
Hence, our geometrical approach opens the possibility of describing the
eigenmodes and eigenvalues for astrophysical/geophysical Ekman numbers
(), which are out of reach numerically, and this for a wide
class of containers.Comment: 42 pages, 20 figures, abstract shortene
Bottlenecks to vibrational energy flow in OCS: Structures and mechanisms
Finding the causes for the nonstatistical vibrational energy relaxation in
the planar carbonyl sulfide (OCS) molecule is a longstanding problem in
chemical physics: Not only is the relaxation incomplete long past the predicted
statistical relaxation time, but it also consists of a sequence of abrupt
transitions between long-lived regions of localized energy modes. We report on
the phase space bottlenecks responsible for this slow and uneven vibrational
energy flow in this Hamiltonian system with three degrees of freedom. They
belong to a particular class of two-dimensional invariant tori which are
organized around elliptic periodic orbits. We relate the trapping and
transition mechanisms with the linear stability of these structures.Comment: 13 pages, 13 figure
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