1,842 research outputs found
The interaction-strength interpolation method for main-group chemistry: benchmarking, limitations, and perspectives
We have tested the original interaction-strength-interpolation (ISI)
exchange-correlation functional for main group chemistry. The ISI functional is
based on an interpolation between the weak and strong coupling limits and
includes exact-exchange as well as the G\"orling-Levy second-order energy. We
have analyzed in detail the basis-set dependence of the ISI functional, its
dependence on the ground-state orbitals, and the influence of the
size-consistency problem. We show and explain some of the expected limitations
of the ISI functional (i.e. for atomization energies), but also unexpected
results, such as the good performance for the interaction energy of
dispersion-bonded complexes when the ISI correlation is used as a correction to
Hartree-Fock.Comment: 20 pages, 20 figure
Strictly correlated uniform electron droplets
We study the energetic properties of finite but internally homogeneous
D-dimensional electron droplets in the strict-correlation limit. The indirect
Coulomb interaction is found to increase as a function of the electron number,
approaching the tighter forms of the Lieb-Oxford bound recently proposed by
Rasanen et al. [Phys. Rev. Lett. 102, 206406 (2009)]. The bound is satisfied in
three-, two-, and one-dimensional droplets, and in the latter case it is
reached exactly - regardless of the type of interaction considered. Our results
provide useful reference data for delocalized strongly correlated systems, and
they can be used in the development and testing of exchange-correlation density
functionals in the framework of density-functional theory
Cognitive function and cholinergic transmission in patients with subcortical vascular dementia and microbleeds: a TMS study
Irradiation of Materials with Short, Intense Ion pulses at NDCX-II
We present an overview of the performance of the Neutralized Drift
Compression Experiment-II (NDCX-II) accelerator at Berkeley Lab, and report on
recent target experiments on beam driven melting and transmission ion energy
loss measurements with nanosecond and millimeter-scale ion beam pulses and thin
tin foils. Bunches with around 10^11 ions, 1-mm radius, and 2-30 ns FWHM
duration have been created with corresponding fluences in the range of 0.1 to
0.7 J/cm^2. To achieve these short pulse durations and mm-scale focal spot
radii, the 1.1 MeV He+ ion beam is neutralized in a drift compression section,
which removes the space charge defocusing effect during final compression and
focusing. The beam space charge and drift compression techniques resemble
necessary beam conditions and manipulations in heavy ion inertial fusion
accelerators. Quantitative comparison of detailed particle-in-cell simulations
with the experiment play an important role in optimizing accelerator
performance.Comment: 15 pages, 7 figures. revised manuscript submitted to Laser and
Particle Beam
Unpaired and spin-singlet paired states of a two-dimensional electron gas in a perpendicular magnetic field
We present a variational study of both unpaired and spin-singlet paired
states induced in a two-dimensional electron gas at low density by a
perpendicular magnetic field. It is based on an improved circular-cell
approximation which leads to a number of closed analytical results. The
ground-state energy of the Wigner crystal containing a single electron per cell
in the lowest Landau level is obtained as a function of the filling factor
: the results are in good agreement with those of earlier approaches and
predict for the upper filling factor at which the
solid-liquid transition occurs. A novel localized state of spin-singlet
electron pairs is examined and found to be a competitor of the unpaired state
for filling factor . The corresponding phase boundary is quantitatively
displayed in the magnetic field-electron density plane.Comment: 19 pages, 8 figures, submitted to Phys. Rev. B on 7th April 2001. to
appear in Phys. Rev.
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Electron Cloud Effects in Intense, Ion Beam Linacs: Theory and Experimental Planning for Heavy-Ion Fusion
Heavy-ion accelerators for HIF will operate at high aperture-fill factors with high beam current and long pulses. This will lead to beam ions impacting walls: liberating gas molecules and secondary electrons. Without special preparation a large fractional electron population ({approx}>1%) is predicted in the High-Current Experiment (HCX), but wall conditioning and other mitigation techniques should result in substantial reduction. Theory and particle-in-cell simulations suggest that electrons, from ionization of residual and desorbed gas and secondary electrons from vacuum walls, will be radially trapped in the {approx}4 kV ion beam potential. Trapped electrons can modify the beam space charge, vacuum pressure, ion transport dynamics, and halo generation, and can potentially cause ion-electron instabilities. Within quadrupole (and dipole) magnets, the longitudinal electron flow is limited to drift velocities (E x B and {del}B) and the electron density can vary azimuthally, radially, and longitudinally. These variations can cause centroid misalignment, emittance growth and halo growth. Diagnostics are being developed to measure the energy and flux of electrons and gas evolved from walls, and the net charge and gas density within magnetic quadrupoles, as well as the their effect on the ion beam
Measurement of Strange Quark Contributions to the Nucleon's Form Factors at Q^2=0.230 (GeV/c)^2
We report on a measurement of the parity-violating asymmetry in the
scattering of longitudinally polarized electrons on unpolarized protons at a
of 0.230 (GeV/c)^2 and a scattering angle of \theta_e = 30^o - 40^o.
Using a large acceptance fast PbF_2 calorimeter with a solid angle of
\Delta\Omega = 0.62 sr the A4 experiment is the first parity violation
experiment to count individual scattering events. The measured asymmetry is
A_{phys} =(-5.44 +- 0.54_{stat} +- 0.27_{\rm sys}) 10^{-6}. The Standard Model
expectation assuming no strangeness contributions to the vector form factors is
. The difference is a direct measurement of the
strangeness contribution to the vector form factors of the proton. The
extracted value is G^s_E + 0.225 G^s_M = 0.039 +- 0.034 or F^s_1 + 0.130 F^s_2
= 0.032 +- 0.028.Comment: 5 pages, 3 figures, submitted to Phys. Rev. Letters on Dec 11, 200
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