2,887 research outputs found
Global hyperon polarization at local thermodynamic equilibrium with vorticity, magnetic field and feed-down
The system created in ultrarelativistic nuclear collisions is known to behave
as an almost ideal liquid. In non-central collisions, due to the large orbital
momentum, such a system might be the fluid with the highest vorticity ever
created under laboratory conditions. Particles emerging from such a highly
vorticous fluid are expected to be globally polarized with their spins on
average pointing along the system angular momentum. Vorticity-induced
polarization is the same for particles and antiparticles, but the intense
magnetic field generated in these collisions may lead to the splitting in
polarization. In this paper we outline the thermal approach to the calculation
of the global polarization phenomenon for particles with spin and we discuss
the details of the experimental study of this phenomenon, estimating the effect
of feed-down. A general formula is derived for the polarization transfer in
two-body decays and, particularly, for strong and electromagnetic decays. We
find that accounting for such effects is crucial when extracting vorticity and
magnetic field from the experimental data.Comment: 14 pages, 1 figure. Final version published in PRC with one more
formula and slightly revised tex
Aspects Of Heavy Quark Theory
Recent achievements in the heavy quark theory are critically reviewed. The
emphasis is put on those aspects which either did not attract enough attention
or cause heated debates in the current literature. Among other topics we
discuss (i) basic parameters of the heavy quark theory; (ii) a class of exact
QCD inequalities; (iii) new heavy quark sum rules; (iv) virial theorem; (v)
applications (|V_cb| from the total semileptonic width and from the B->D*
transition at zero recoil). In some instances new derivations of the previously
known results are given, or new aspects addressed. In particular, we dwell on
the exact QCD inequalities. Furthermore, a toy model is considered that may
shed light on the controversy regarding the value of the kinetic energy of
heavy quarks obtained by different methods.Comment: 67 pages, 6 Figures; plain LaTeX. Changes: Some equations in Sect.4
related to spin-nonsinglet sum rules are corrected. The references are
updated
"Unusual" critical states in type-II superconductors
We give a theoretical description of the general critical states in which the
critical currents in type-II superconductors are not perpendicular to the local
magnetic induction. Such states frequently occur in real situations, e.g., when
the sample shape is not sufficiently symmetric or the direction of the external
magnetic field changes in some complex way. Our study is restricted to the
states in which flux-line cutting does not occur. The properties of such
general critical states can essentially differ from the well-known properties
of the usual Bean critical states. To illustrate our approach, we analyze
several examples. In particular, we consider the critical states in a slab
placed in a uniform perpendicular magnetic field and to which two components of
the in-plane magnetic field are then applied successively. We also analyze the
critical states in a long thin strip placed in a perpendicular magnetic field
which then is tilted towards the axis of the strip.Comment: 15 pages including 11 figure
On the and as Bound States and Approximate Nambu-Goldstone Bosons
We reconsider the two different facets of and mesons as
bound states and approximate Nambu-Goldstone bosons. We address several topics,
including masses, mass splittings between and and between and
, meson wavefunctions, charge radii, and the wavefunction overlap.Comment: 15 pages, late
Precision Studies of Duality in the 't Hooft Model
We address numerical aspects of local quark-hadron duality using the example
of the exactly solvable 't Hooft model, two-dimensional QCD with N_c -->
infinity. The primary focus of these studies is total semileptonic decay widths
relevant for extracting |V_{cb}| and |V_{ub}|. We compare the exact
channel-by-channel sum of exclusive modes to the corresponding rates obtained
in the standard 1/m_Q expansion arising from the Operator Product Expansion. An
impressive agreement sets in unexpectedly early, immediately after the
threshold for the first hadronic excitation in the final state. Yet even at
higher energy release it is possible to discern the seeds of duality-violating
oscillations. We find the ``Small Velocity'' sum rules to be exceptionally well
saturated already by the first excited state. We also obtain a convincing
degree of duality in the differential distributions and in an analogue of
R_{e^+e^-}(s). Finally, we discuss possible lessons for semileptonic decays of
actual heavy quarks in QCD.Comment: 45 pages, 16 eps figures include
The Lambda_b lifetime in the light front quark model
The enhancement of the Lambda_b decay width relative to B decay one due to
the difference of Fermi motion effects in Lambda_b and B is calculated in the
light--front quark model with the simplifying assumption that Lambda_b consists
of the heavy quark and light scalar diquark. In order to explain the large
deviation from unity in the experimental result for tau(Lambda_b)/tau(B), it is
necessary that diquark be light and the ratio of the squares of the Lambda_b
and B wave functions at the origin be \le 1.Comment: final journal version to appear in JETP Letter
Decay of metastable current states in one-dimensional resonant tunneling devices
Current switching in a double-barrier resonant tunneling structure is studied
in the regime where the current-voltage characteristic exhibits intrinsic
bistability, so that in a certain range of bias two different steady states of
current are possible. Near the upper boundary V_{th} of the bistable region the
upper current state is metastable, and because of the shot noise it eventually
decays to the stable lower current state. We find the time of this switching
process in strip-shaped devices, with the width small compared to the length.
As the bias V is tuned away from the boundary value V_{th} of the bistable
region, the mean switching time \tau increases exponentially. We show that in
long strips \ln\tau \propto (V_{th} -V)^{5/4}, whereas in short strips \ln\tau
\propto (V_{th} -V)^{3/2}. The one-dimensional geometry of the problem enables
us to obtain analytically exact expressions for both the exponential and the
prefactor of \tau. Furthermore, we show that, depending on the parameters of
the system, the switching can be initiated either inside the strip, or at its
ends.Comment: 12 pages, 5 figures, update to published versio
Quenched disorder induced magnetization jumps in (Sm,Sr)MnO
Magnetic field induced step-like changes in magnetization and resistivity of
SmSr manganites were studied. A strong dependence of these features on the
cooling rate was observed. Magnetostriction, however, does not show the
presence of large strain in our samples. From all these features we can rule
out the conventional explanation of magnetization jumps as a consequence of
martensitic transition. We propose instead that quenched by fast cooling
disorder leads to the formation of an inhomogeneous metastable state and to
subsequent magnetization jumps.Comment: 4 pages, 4 figures, to be published in PRB Brief
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