5,643 research outputs found
Determining the Nonperturbative Collins-Soper Kernel From Lattice QCD
At small transverse momentum , transverse-momentum dependent parton
distribution functions (TMDPDFs) arise as genuinely nonperturbative objects
that describe Drell-Yan like processes in hadron collisions as well as
semi-inclusive deep-inelastic scattering. TMDPDFs naturally depend on the
hadron momentum, and the associated evolution is determined by the
Collins-Soper equation. For the corresponding
evolution kernel (or anomalous dimension) is nonperturbative and must be
determined as an independent ingredient in order to relate TMDPDFs at different
scales. We propose a method to extract this kernel using lattice QCD and the
Large-Momentum Effective Theory, where the physical TMD correlation involving
light-like paths is approximated by a quasi TMDPDF, defined using equal-time
correlation functions with a large-momentum hadron state. The kernel is
determined from a ratio of quasi TMDPDFs extracted at different hadron momenta.Comment: 9 pages, 2 figures; v2: extended the review of TMDPDF commonalities,
version submitted to PRD; v3: minor changes, journal versio
The diffusion coefficient of propagating fronts with multiplicative noise
Recent studies have shown that in the presence of noise both fronts
propagating into a metastable state and so-called pushed fronts propagating
into an unstable state, exhibit diffusive wandering about the average position.
In this paper we derive an expression for the effective diffusion coefficient
of such fronts, which was motivated before on the basis of a multiple scale
ansatz. Our systematic derivation is based on the decomposition of the
fluctuating front into a suitably positioned average profile plus fluctuating
eigenmodes of the stability operator. While the fluctuations of the front
position in this particular decomposition are a Wiener process on all time
scales, the fluctuations about the time averaged front profile relax
exponentially.Comment: 4 page
A diquark model for baryons containing one heavy quark
We present a phenomenological ansatz for coupling a heavy quark with two
light quarks to form a heavy baryon. The heavy quark is treated in the heavy
mass limit, and the light quark dynamics is approximated by propagating scalar
and axial vector 'diquarks'. The resulting effective lagrangian, which
incorporates heavy quark and chiral symmetry, describes interactions of heavy
baryons with Goldstone bosons in the low energy region. As an application, the
Isgur--Wise form factors are estimated.Comment: 9 pages + 8 figures, both as uuencoded PS, discussion of Bjorken
limit (1 par + 1 fig) added, to appear in Z.Phys.
Rare radiative B decays to orbitally excited K mesons
The exclusive rare radiative B meson decays to orbitally excited axial-vector
mesons K_1^*(1270), K_1(1400) and to the tensor meson K_2^*(1430) are
investigated in the framework of the relativistic quark model based on the
quasipotential approach in quantum field theory. These decays are considered
without employing the heavy quark expansion for the s quark. Instead the s
quark is treated to be light and the expansion in inverse powers of the large
recoil momentum of the final K^{**} meson is used to simplify calculations. It
is found that the ratio of the branching fractions of rare radiative B decays
to axial vector K^*_1(1270) and K_1(1400) mesons is significantly influenced by
relativistic effects. The obtained results for B decays to the tensor meson
K_2^*(1430) agree with recent experimental data from CLEO.Comment: 17 pages, revte
Masses of tetraquarks with two heavy quarks in the relativistic quark model
Masses of tetraquarks with two heavy quarks and open charm and bottom are
calculated in the framework of the diquark-antidiquark picture in the
relativistic quark model. All model parameters were regarded as fixed by
previous considerations of various properties of mesons and baryons. The light
quarks and diquarks are treated completely relativistically. The c quark is
assumed to be heavy enough to make the diquark configurations dominating. The
diquarks are considered not to be point-like but to have an internal structure
which is taken into account by the calculated diquark form factor entering the
diquark-gluon interaction. It is found that all the (cc)(\bar q\bar q')
tetraquarks have masses above the thresholds for decays into open charm mesons.
Only the I(J^P)=0(1^+) state of (bb)(\bar u\bar d) lies below the BB* threshold
and is predicted to be narrow.Comment: 12 pages; version to be published in Phys.Rev.
Statistics at the tip of a branching random walk and the delay of traveling waves
We study the limiting distribution of particles at the frontier of a
branching random walk. The positions of these particles can be viewed as the
lowest energies of a directed polymer in a random medium in the mean-field
case. We show that the average distances between these leading particles can be
computed as the delay of a traveling wave evolving according to the Fisher-KPP
front equation. These average distances exhibit universal behaviors, different
from those of the probability cascades studied recently in the context of mean
field spin-glasses.Comment: 4 pages, 2 figure
Quark and pion condensation in a chromomagnetic background field
The general features of quark and pion condensation in dense quark matter
with flavor asymmetry have been considered at finite temperature in the
presence of a chromomagnetic background field modelling the gluon condensate.
In particular, pion condensation in the case of a constant abelian
chromomagnetic field and zero temperature has been studied both analytically
and numerically. Under the influence of the chromomagnetic background field the
effective potential of the system is found to have a global minimum for a
finite pion condensate even for small values of the effective quark coupling
constant. In the strong field limit, an effective dimensional reduction has
been found to take place.Comment: 17 pages, 6 figure
Exploiting jet binning to identify the initial state of high-mass resonances
If a new high-mass resonance is discovered at the Large Hadron Collider,
model-independent techniques to identify the production mechanism will be
crucial to understand its nature and effective couplings to Standard Model
particles. We present a powerful and model-independent method to infer the
initial state in the production of any high-mass color-singlet system by using
a tight veto on accompanying hadronic jets to divide the data into two mutually
exclusive event samples (jet bins). For a resonance of several hundred GeV, the
jet binning cut needed to discriminate quark and gluon initial states is in the
experimentally accessible range of several tens of GeV. It also yields
comparable cross sections for both bins, making this method viable already with
the small event samples available shortly after a discovery. Theoretically, the
method is made feasible by utilizing an effective field theory setup to compute
the jet cut dependence precisely and model independently and to systematically
control all sources of theoretical uncertainties in the jet binning, as well as
their correlations. We use a 750 GeV scalar resonance as an example to
demonstrate the viability of our method.Comment: 6 pages, 2 figures, v2: journal versio
J Fluorescence
The scope of this paper is to illustrate the need for an improved quality assurance in fluorometry. For this purpose, instrumental sources of error and their influences on the reliability and comparability of fluorescence data are highlighted for frequently used photoluminescence techniques ranging from conventional macro- and microfluorometry over fluorescence microscopy and flow cytometry to microarray technology as well as in vivo fluorescence imaging. Particularly, the need for and requirements on fluorescence standards for the characterization and performance validation of fluorescence instruments, to enhance the comparability of fluorescence data, and to enable quantitative fluorescence analysis are discussed. Special emphasis is dedicated to spectral fluorescence standards and fluorescence intensity standards
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