2,807 research outputs found
Iowa in War Times
This history of Iowa\u27s involvement in the Civil War was published in 1888. The author, Samuel Hawkins Marshall Byers, was a member of the Fifth Iowa Infantry during the Civil War, having enlisted in 1861. Byers was eventually captured and spent well over a year in several Confederate prison camps. Following his escape, Byers joined Gen. William Tecumseh Sherman\u27s staff until the war\u27s end. In 1869 he was appointed United States Consul to Zurich, Switzerland, and later held the same position in Rome. Byers many works include The Song of Iowa the official state song of Iowa.https://scholarworks.uni.edu/iowabooks/1016/thumbnail.jp
Re-parameterization Invariance in Fractional Flux Periodicity
We analyze a common feature of a nontrivial fractional flux periodicity in
two-dimensional systems. We demonstrate that an addition of fractional flux can
be absorbed into re-parameterization of quantum numbers. For an exact
fractional periodicity, all the electronic states undergo the
re-parameterization, whereas for an approximate periodicity valid in a large
system, only the states near the Fermi level are involved in the
re-parameterization.Comment: 4 pages, 1 figure, minor changes, final version to appear in J. Phys.
Soc. Jp
Quantum shot-noise at local tunneling contacts on mesoscopic multiprobe conductors
New experiments that measure the low-frequency shot-noise spectrum at local
tunneling contacts on mesoscopic structures are proposed. The current
fluctuation spectrum at a single tunneling tip is determined by local partial
densities of states. The current-correlation spectrum between two tunneling
tips is sensitive to non-diagonal density of states elements which are
expressed in terms of products of scattering states of the conductor. Thus such
an experiment permits to investigate correlations of electronic wave functions.
We present specific results for a clean wire with a single barrier and for
metallic diffusive conductors.Comment: 4 pages REVTeX, 2 figure
Persistent current of two-chain Hubbard model with impurities
The interplay between impurities and interactions is studied in the gapless
phase of two-chain Hubbard model in order to see how the screening of impurity
potentials due to repulsive interactions in single-chain model will be changed
by increasing the number of channels. Renormalization group calculations show
that charge stiffness, and hence persistent current, of the two-chain model are
less enhanced by interactions than single chain case.Comment: 4 Pages, RevTeX, No figures, Submitted to PR
Spin diffusion in doped semiconductors
The behavior of spin diffusion in doped semiconductors is shown to be
qualitatively different than in undoped (intrinsic) ones. Whereas a spin packet
in an intrinsic semiconductor must be a multiple-band disturbance, involving
inhomogeneous distributions of both electrons and holes, in a doped
semiconductor a single-band disturbance is possible. For n-doped nonmagnetic
semiconductors the enhancement of diffusion due to a degenerate electron sea in
the conduction band is much larger for these single-band spin packets than for
charge packets, and can exceed an order of magnitude at low temperatures even
for equilibrium dopings as small as 10^16 cm^-3. In n-doped ferromagnetic and
semimagnetic semiconductors the motion of spin packets polarized antiparallel
to the equilibrium carrier spin polarization is predicted to be an order of
magnitude faster than for parallel polarized spin packets. These results are
reversed for p-doped semiconductors.Comment: 8 pages, 4 figure
Topological quenching of the tunnel splitting for a particle in a double-well potential on a planar loop
The motion of a particle along a one-dimensional closed curve in a plane is considered. The only restriction on the shape of the loop is that it must be invariant under a twofold rotation about an axis perpendicular to the plane of motion. Along the curve a symmetric double-well potential is present leading to a twofold degeneracy of the classical ground state. In quantum mechanics, this degeneracy is lifted: the energies of the ground state and the first excited state are separated from each other by a slight difference ¿E, the tunnel splitting. Although a magnetic field perpendicular to the plane of the loop does not influence the classical motion of the charged particle, the quantum-mechanical separation of levels turns out to be a function of its strength B. The dependence of ¿E on the field B is oscillatory: for specific discrete values Bn the splitting drops to zero, indicating a twofold degeneracy of the ground state. This result is obtained within the path-integral formulation of quantum mechanics; in particular, the semiclassical instanton method is used. The origin of the quenched splitting is intuitively obvious: it is due to the fact that the configuration space of the system is not simply connected, thus allowing for destructive interference of quantum-mechanical amplitudes. From an abstract point of view this phenomenon can be traced back to the existence of a topological term in the Lagrangian and a nonsimply connected configuration space. In principle, it should be possible to observe the splitting in appropriately fabricated mesoscopic rings consisting of normally conducting metal
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