32,860 research outputs found
Determining the strange and antistrange quark distributions of the nucleon
The difference between the strange and antistrange quark distributions,
\delta s(x)=s(x)-\sbar(x), and the combination of light quark sea and strange
quark sea, \Delta (x)=\dbar(x)+\ubar(x)-s(x)-\sbar(x), are originated from
non-perturbative processes, and can be calculated using non-perturbative models
of the nucleon. We report calculations of and using
the meson cloud model. Combining our calculations of with
relatively well known light antiquark distributions obtained from global
analysis of available experimental data, we estimate the total strange sea
distributions of the nucleon.Comment: 4 pages, 3 figures; talk given by F.-G. at QNP0
Charge Ordered RVB States in the Doped Cuprates
We study charge ordered d-wave resonating valence bond states (dRVB) in the
doped cuprates, and estimate the energies of these states in a generalized model by using a renormalized mean field theory. The long range Coulomb
potential tends to modulate the charge density in favor of the charge ordered
RVB state. The possible relevance to the recently observed
checkerboard patterns in tunnelling conductance in high cuprates is
discussed.Comment: 4 pages, 4 figures, 3 table
Entanglement and Quantum Phases in the Anisotropic Ferromagnetic Heisenberg Chain in the Presence of Domain Walls
We discuss entanglement in the spin-1/2 anisotropic ferromagnetic Heisenberg
chain in the presence of a boundary magnetic field generating domain walls. By
increasing the magnetic field, the model undergoes a first-order quantum phase
transition from a ferromagnetic to a kink-type phase, which is associated to a
jump in the content of entanglement available in the system. Above the critical
point, pairwise entanglement is shown to be non-vanishing and independent of
the boundary magnetic field for large chains. Based on this result, we provide
an analytical expression for the entanglement between arbitrary spins. Moreover
the effects of the quantum domains on the gapless region and for
antiferromagnetic anisotropy are numerically analysed. Finally multiparticle
entanglement properties are considered, from which we establish a
characterization of the critical anisotropy separating the gapless regime from
the kink-type phase.Comment: v3: 7 pages, including 4 figures and 1 table. Published version. v2:
One section (V) added and references update
L-functions of Symmetric Products of the Kloosterman Sheaf over Z
The classical -variable Kloosterman sums over the finite field
give rise to a lisse -sheaf on , which we call the Kloosterman
sheaf. Let be the
-function of the -fold symmetric product of . We
construct an explicit virtual scheme of finite type over such that the -Euler factor of the zeta function of coincides with
. We also prove
similar results for and .Comment: 16 page
Using Moran's I and GIS to study the spatial pattern of forest litter carbon density in a subtropical region of southeastern China
Spatial pattern information of carbon density in forest ecosystem including
forest litter carbon (FLC) plays an important role in evaluating carbon
sequestration potentials. The spatial variation of FLC
density in the typical subtropical forests in southeastern China was
investigated using Moran's I, geostatistics and a geographical information
system (GIS). A total of 839 forest litter samples were collected based on a
12 km (south–north) × 6 km (east–west) grid system in Zhejiang
province. Forest litter carbon density values were very variable, ranging
from 10.2 kg ha<sup>−1</sup> to 8841.3 kg ha<sup>−1</sup>, with an average of
1786.7 kg ha<sup>−1</sup>. The aboveground biomass had the strongest positive correlation
with FLC density, followed by forest age and elevation. Global Moran's I
revealed that FLC density had significant positive spatial autocorrelation.
Clear spatial patterns were observed using local Moran's I. A spherical
model was chosen to fit the experimental semivariogram. The moderate
"nugget-to-sill" (0.536) value revealed that both natural and
anthropogenic factors played a key role in spatial heterogeneity of FLC
density. High FLC density values were mainly distributed in northwestern and
western part of Zhejiang province, which were related to adopting long-term
policy of forest conservation in these areas, while Hang-Jia-Hu (HJH) Plain,
Jin-Qu (JQ) Basin and coastal areas had low FLC density due to low forest
coverage and intensive management of economic forests. These spatial
patterns were in line with the spatial-cluster map described by local
Moran's I. Therefore, Moran's I, combined with geostatistics and GIS, could
be used to study spatial patterns of environmental variables related to
forest ecosystem
Scale dependence of the beta diversity-scale relationship
Alpha, beta, and gamma diversity are three fundamental biodiversity components in ecology, but most studies focus only on the scale issues of the alpha or gamma diversity component. The beta diversity component, which incorporates both alpha and gamma diversity components, is ideal for studying scale issues of diversity. We explore the scale dependency of beta diversity and scale relationship, both theoretically as well as by application to actual data sets. Our results showed that a power law exists for beta diversity-area (spatial grain or spatial extent) relationships, and that the parameters of the power law are dependent on the grain and extent for which the data are defined. Coarse grain size generates a steeper slope (scaling exponent z) with lower values of intercept (c), while a larger extent results in a reverse trend in both parameters. We also found that, for a given grain (with varying extent) or a given extent (with varying grain) the two parameters are themselves related by power laws. These findings are important because they are the first to simultaneously relate the various components of scale and diversity in a unified manner
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