1,046 research outputs found
Strongly correlated fermions on a kagome lattice
We study a model of strongly correlated spinless fermions on a kagome lattice
at 1/3 filling, with interactions described by an extended Hubbard Hamiltonian.
An effective Hamiltonian in the desired strong correlation regime is derived,
from which the spectral functions are calculated by means of exact
diagonalization techniques. We present our numerical results with a view to
discussion of possible signatures of confinement/deconfinement of fractional
charges.Comment: 10 pages, 10 figure
Complete phase diagram of the spin-1/2 -- model (with ) on the honeycomb lattice
We use the coupled cluster method to investigate the ground-state (GS)
properties of the frustrated spin-1/2 -- model on the
honeycomb lattice, with nearest-neighbor exchange coupling plus
next-nearest-neighbor () and next-next-nearest-neighbor () exchanges
of equal strength. In particular we find a direct first-order phase transition
between the N\'eel-ordered antiferromagnetic phase and the ferromagnetic phase
at a value when , compared to the
corresponding classical value of -1. We find no evidence for any intermediate
phase. From this and our previous CCM studies of the model we present its full
zero-temperature GS phase diagram.Comment: 4 pages, 4 figure
On confined fractional charges: a simple model
We address the question whether features known from quantum chromodynamics
(QCD) can possibly also show up in solid-state physics. It is shown that
spinless fermions of charge on a checkerboard lattice with nearest-neighbor
repulsion provide for a simple model of confined fractional charges. After
defining a proper vacuum the system supports excitations with charges
attached to the ends of strings. There is a constant confining force acting
between the fractional charges. It results from a reduction of vacuum
fluctuations and a polarization of the vacuum in the vicinity of the connecting
strings.Comment: 5 pages, 3 figure
Charge degrees in the quarter-filled checkerboard lattice
For a systematic study of charge degrees of freedom in lattices with
geometric frustration, we consider spinless fermions on the checkerboard
lattice with nearest-neighbor hopping and nearest-neighbor repulsion at
quarter-filling. An effective Hamiltonian for the limit is given to
lowest non-vanishing order by the ring exchange (). We show
that the system can equivalently be described by hard-core bosons and map the
model to a confining U(1) lattice gauge theory.Comment: Proceedings of ICM200
Semiclassical ordering in the large-N pyrochlore antiferromagnet
We study the semiclassical limit of the generalization of the
pyrochlore lattice Heisenberg antiferromagnet by expanding about the saddlepoint in powers of a generalized inverse spin. To leading order,
we write down an effective Hamiltonian as a series in loops on the lattice.
Using this as a formula for calculating the energy of any classical ground
state, we perform Monte-Carlo simulations and find a unique collinear ground
state. This state is not a ground state of linear spin-wave theory, and can
therefore not be a physical (N=1) semiclassical ground state.Comment: 4 pages, 4 eps figures; published versio
Frustrated ferromagnetic spin-1/2 chain in a magnetic field: The phase diagram and thermodynamic properties
The frustrated ferromagnetic spin-1/2 Heisenberg chain is studied by means of
a low-energy field theory as well as the density-matrix renormalization group
and exact diagonalization methods. Firstly, we study the ground-state phase
diagram in a magnetic field and find an `even-odd' (EO) phase characterized by
bound pairs of magnons in the region of two weakly coupled antiferromagnetic
chains. A jump in the magnetization curves signals a first-order transition at
the boundary of the EO phase, but otherwise the curves are smooth. Secondly, we
discuss thermodynamic properties at zero field, where we confirm a double-peak
structure in the specific heat for moderate frustrating next-nearest neighbor
interactions.Comment: 4 pages RevTex4, 4 figures. Minor changes, title modified. Additional
material is available here:
http://www.theorie.physik.uni-goettingen.de/~honecker/j1j2-td
DNA binding kinetics of two response regulators, PlnC and PlnD, from the bacteriocin regulon of Lactobacillus plantarum C11
<p>Abstract</p> <p>Background</p> <p>Bacteriocin production in the lactic acid bacterium <it>Lactobacillus plantarum </it>C11 is regulated through a quorum sensing based pathway involving two highly homologous response regulators (59% identity and 76% similarity), PlnC as a transcriptional activator and PlnD as a repressor. Previous <it>in vitro </it>studies have shown that both regulators bind, as homodimers, to the same DNA regulatory repeats to exert their regulatory functions. As the genes for these two proteins are located on the same auto-regulatory operon, hence being co-expressed upon gene activation, it is plausible that their opposite functions must somehow be differentially regulated, either in terms of timing and/or binding kinetics, so that their activities do not impair each other in an uncontrolled manner. To understand the nature behind this potential differentiation, we have studied the binding kinetics of the two regulators on five target promoters (P<sub><it>plnA</it></sub>, P<sub><it>plnM</it></sub>, P<sub><it>plnJ</it></sub>, P<sub><it>plnE </it></sub>and P<sub><it>plnG</it></sub>) from the bacteriocin regulon of <it>L. plantarum </it>C11.</p> <p>Results</p> <p>By using surface plasmon resonance spectroscopy we obtained parameters such as association rates, dissociation rates and dissociation constants, showing that the two regulators indeed differ greatly from each other in terms of cooperative binding and binding strength to the different promoters. For instance, cooperativity is very strong for PlnC binding to the promoter of the regulatory operon (P<sub><it>plnA</it></sub>), but not to the promoter of the transport operon (P<sub><it>plnG</it></sub>), while the opposite is seen for PlnD binding to these two promoters. The estimated affinity constants indicate that PlnC can bind to P<sub><it>plnA </it></sub>to activate transcription of the key regulatory operon <it>plnABCD </it>without much interference from PlnD, and that the repressive function of PlnD might act through a different mechanism than repression of the regulatory operon.</p> <p>Conclusion</p> <p>We have characterised the DNA binding kinetics of the two regulators PlnC and PlnD from the bacteriocin locus in <it>L. plantarum </it>C11. Our data show that PlnC and PlnD, despite their strong homology to each other, differ greatly from each other in terms of binding affinity and cooperativity to the different promoters of the <it>pln </it>regulon.</p
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