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Chiral discrimination in optical binding
The laser-induced intermolecular force that exists between two or more particles in the presence of an electromagnetic field is commonly termed “optical binding.” Distinct from the single-particle forces that are at play in optical trapping at the molecular level, the phenomenon of optical binding is a manifestation of the coupling between optically induced dipole moments in neutral particles. In other, more widely known areas of optics, there are many examples of chiral discrimination—signifying the different response a chiral material has to the handedness of an optical input. In the present analysis, extending previous work on chiral discrimination in optical binding, a mechanism is identified using a quantum electrodynamical approach. It is shown that the optical binding force between a pair of chiral molecules can be significantly discriminatory in nature, depending upon both the handedness of the interacting particles and the polarization of the incident light, and it is typically several orders of magnitude larger than previously reported
DMRG evaluation of the Kubo formula -- Conductance of strongly interacting quantum systems
In this paper we present a novel approach combining linear response theory
(Kubo) for the conductance and the Density Matrix Renormalization Group (DMRG).
The system considered is one-dimensional and consists of non-interacting tight
binding leads coupled to an interacting nanostructure via weak links. Electrons
are treated as spinless fermions and two different correlation functions are
used to evaluate the conductance.
Exact diagonalization calculations in the non-interacting limit serve as a
benchmark for our combined Kubo and DMRG approach in this limit. Including both
weak and strong interaction we present DMRG results for an extended
nanostructure consisting of seven sites. For the strongly interacting structure
a simple explanation of the position of the resonances is given in terms of
hard-core particles moving freely on a lattice of reduced size.Comment: 7 pages, 2 figures. Minor typos correcte
Scaling of in heavy ion collisions
We interpret the scaling of the corrected elliptic flow parameter w.r.t. the
corrected multiplicity, observed to hold in heavy ion collisions for a wide
variety of energies and system sizes. We use dimensional analysis and
power-counting arguments to place constraints on the changes of initial
conditions in systems with different center of mass energy .
Specifically, we show that a large class of changes in the (initial) equation
of state, mean free path, and longitudinal geometry over the observed
are likely to spoil the scaling in observed experimentally. We
therefore argue that the system produced at most Super Proton Synchrotron (SPS)
and Relativistic Heavy Ion Collider (RHIC) energies is fundamentally the same
as far as the soft and approximately thermalized degrees of freedom are
considered. The ``sQGP'' (Strongly interacting Quark-Gluon Plasma) phase, if it
is there, is therefore not exclusive to RHIC. We suggest, as a goal for further
low-energy heavy ion experiments, to search for a ``transition''
where the observed scaling breaks.Comment: Accepted for publication by Phys. Rev. C Based on presentation in
mini-symposium on QGP collective properties, Frankfurt. Discussion expanded,
results adde
Comment on "Off-diagonal Long-range Order in Bose Liquids: Irrotational Flow and Quantization of Circulation"
In the context of an application to superfluidity, it is elaborated how to do
quantum mechanics of a system with a rotational velocity. Especially, in both
the laboratory frame and the non-inertial co-rotating frame, the canonical
momentum, which corresponds to the quantum mechanical momentum operator,
contains a part due to the rotational velocity.Comment: 2 page, comment on cond-mat/010435
Elasticity of an interfacial particle raft
We study the collective behaviour of a close packed monolayer of non-Brownian
particles at a fluid-liquid interface. Such a particle raft forms a
two-dimensional elastic solid and can support anisotropic stresses and strains,
e.g. it buckles in uniaxial compression and cracks in tension. We characterise
this solid in terms of a Young's modulus and Poisson ratio derived from simple
theoretical considerations and show the validity of these estimates by using an
experimental buckling assay to deduce the Young's modulus.Comment: 7 pages, 5 figure
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