1,067 research outputs found
The strange quark condensate in the nucleon in 2+1 flavor QCD
We calculate the "strange quark content of the nucleon", ,
which is important for interpreting the results of some dark matter detection
experiments. The method is to evaluate quark-line disconnected correlations on
the MILC lattice ensembles, which include the effects of dynamical strange
quarks. After continuum and chiral extrapolations, the result is <N |s s_bar
|N> = 0.69 +- 0.07(statistical) +- 0.09(systematic), in the modified minimal
subtraction scheme (2 GeV), or for the renormalization scheme invariant form,
m_s partial{M_N}/partial{m_s} = 59(6)(8) MeV.Comment: Added figures and references, especially for fit range choice. Other
changes for clarity. Version to appear in publicatio
Determination of B*B pi coupling in unquenched QCD
The coupling is a fundamental parameter of chiral effective
Lagrangian with heavy-light mesons and can constrain the chiral behavior of
, and the form factor in the soft pion limit. We
compute the coupling with the static heavy quark and the
-improved Wilson light quark. Simulations are carried out with
unquenched lattices at and
lattices at generated by CP-PACS collaboration. To improve the
statistical accuracy, we employ the all-to-all propagator technique and the
static quark action with smeared temporal link variables following the quenched
study by Negishi {\it et al.}. These methods successfully work also on
unquenched lattices, and determine the coupling with 1--2%
statistical accuracy on each lattice spacing.Comment: 19pages,26figure
The intrinsic strangeness and charm of the nucleon using improved staggered fermions
We calculate the intrinsic strangeness of the nucleon, - ,
using the MILC library of improved staggered gauge configurations using the
Asqtad and HISQ actions. Additionally, we present a preliminary calculation of
the intrinsic charm of the nucleon using the HISQ action with dynamical charm.
The calculation is done with a method which incorporates features of both
commonly-used methods, the direct evaluation of the three-point function and
the application of the Feynman- Hellman theorem. We present an improvement on
this method that further reduces the statistical error, and check the result
from this hybrid method against the other two methods and find that they are
consistent. The values for and found here, together with
perturbative results for heavy quarks, show that dark matter scattering through
Higgs-like exchange receives roughly equal contributions from all heavy quark
flavors.Comment: 17 pages, 14 figure
Quantum reservoir computing with a single nonlinear oscillator
Realizing the promise of quantum information processing remains a daunting
task, given the omnipresence of noise and error. Adapting noise-resilient
classical computing modalities to quantum mechanics may be a viable path
towards near-term applications in the noisy intermediate-scale quantum era.
Here, we propose continuous variable quantum reservoir computing in a single
nonlinear oscillator. Through numerical simulation of our model we demonstrate
quantum-classical performance improvement, and identify its likely source: the
nonlinearity of quantum measurement. Beyond quantum reservoir computing, this
result may impact the interpretation of results across quantum machine
learning. We study how the performance of our quantum reservoir depends on
Hilbert space dimension, how it is impacted by injected noise, and briefly
comment on its experimental implementation. Our results show that quantum
reservoir computing in a single nonlinear oscillator is an attractive modality
for quantum computing on near-term hardware.Comment: 9 pages, 5 figure
A new scheme for the running coupling constant in gauge theories using Wilson loops
We propose a new renormalization scheme of the running coupling constant in
general gauge theories using the Wilson loops. The renormalized coupling
constant is obtained from the Creutz ratio in lattice simulations and the
corresponding perturbative coefficient at the leading order. The latter can be
calculated by adopting the zeta-function resummation techniques. We perform a
benchmark test of our scheme in quenched QCD with the plaquette gauge action.
The running of the coupling constant is determined by applying the step-scaling
procedure. Using several methods to improve the statistical accuracy, we show
that the running coupling constant can be determined in a wide range of energy
scales with relatively small number of gauge configurations.Comment: 30pages, figs and comments added,reference added(v3
PHOTOCHEMISTRY OF PHYCOBILIPROTEINS
Native PEC from the cyanobacterium, Mastigocladus laminosus, and its isolated α-subunit show photoreversibly photochromic reactions with difference-maxima around 502 and 570 nm in the spectral region of the α-84 phycoviolobilin chromophore. (b) Native PEC and its β-subunit show little if any reversible photochemistry in the 600–620 nm region, where the phycocyanobilin chromophores on the β-subunit absorb maximally, (c) Reversible photochemistry is retained in ureadenatured PEC at pH = 7.0 or pH ≤ 3. The difference maxima are shifted to 510 and 600 nm, and the amplitudes are decreased. An irreversible absorbance increase occurs around 670 nm (pH ≤ 3). (d) The amplitude of the reversible photoreaction difference spectrum is maximum in the presence of 4–5 M urea or 1 M KSCN, conditions known to dissociate phycobiliprotein aggregates into monomers. At the same time, the phycocyanobilin chromophore(s) are bleached irreversibly, (e) The amplitude becomes very small in high aggregates, e.g. in phycobilisomes. (f) In a reciprocal manner, the phototransformation of native PEC leads to a reversible shift of its aggregation equilibrium between trimer and monomer. The latter is favored by orange, the former by green light, (g) It is concluded that the phycoviolobilin chromophore of PEC is responsible for reversible photochemistry in PEC, and that there is not only an influence of aggregation state on photochemistry, but also vice versa an effect of the status of the chromophore on aggregation state. This could constitute a primary signal in the putative function as sensory pigment, either directly, or indirectly via the release of other polypeptides, via photodynamic effects, or the like
Principal series of finite subgroups of SU(3)
We attempt to give a complete description of the "exceptional" finite
subgroups Sigma(36x3), Sigma(72x3) and Sigma(216x3) of SU(3), with the aim to
make them amenable to model building for fermion masses and mixing. The
information on these groups which we derive contains conjugacy classes, proper
normal subgroups, irreducible representations, character tables and tensor
products of their three-dimensional irreducible representations. We show that,
for these three exceptional groups, usage of their principal series, i.e.
ascending chains of normal subgroups, greatly facilitates the computations and
illuminates the relationship between the groups. As a preparation and testing
ground for the usage of principal series, we study first the dihedral-like
groups Delta(27) and Delta(54) because both are members of the principal series
of the three groups discussed in the paper.Comment: 43 pages, no figures; typos corrected, clarifications and references
added, version matches publication in J. Phys.
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