1,525 research outputs found
Weak dipole moment of in collisions with longitudinally polarized electrons
It is pointed out that certain CP-odd momentum correlations in the production
and subsequent decay of tau pairs in collisions get enhanced when the
is longitudinally polarized. Analytic expressions for these correlations
are obtained for the single-pion decay mode of when have
a ``weak" dipole form factor (WDFF) coupling to . For collisions
at the peak, a sensitivity of about 1-5\mbox{ cm} for
the WDFF can be reached using a {\em single} decay
channel, with 's likely to be available at the SLC at Stanford with
polarization of 62\%-75\%.Comment: 9 pages, Latex, PRL-TH-93/17 (Revised
A trait‐based approach to plant species selection to increase functionality of farmland vegetative strips
Farmland vegetative strips are a proven source of support for ecosystem services and are globally used to mitigate effects of agricultural intensification. However, increasing pressures on agricultural land require increases in their functionality, such as supporting multiple ecosystem services concurrently.
The plant species sown in a vegetative strip seed mix determine the establishment, plant community, and ecosystem services that are supported. Currently, there is no clearly defined or structured method to select plant species for multifunctional vegetative strips.
Plant traits determine how plants support ecosystem services. Also, the establishment and persistence of plant communities is influenced by key internal and external factors. We propose a novel, evidence‐informed method of multifunctional vegetative strip design based on these essential traits and factors.
This study had three distinct stages. The first identified plant traits that support water quality protection, pollinators and/or crop pest natural enemies, using existing research evidence. We then identified key factors affecting plant community establishment and persistence. Finally, we applied these standardized methods to design a multifunctional vegetative strip for a specific case study (UK lowland farmland).
Key plant traits identified, included floral display size, flower color, nectar content, leaf surface area, leaf trichome density, percentage fine roots, root length, rooting depth, and root density. Key internal and external establishment factors included life history, native status, distribution, established competitive strategy, associated floristic diversity, flowering time and duration, and preferred soil type and pH. In the United Kingdom case study, we used five different plant traits and all of the identified factors to design a seed mix for a multifunctional vegetative strip.
We present a transferable method of vegetative strip design that can be adapted for other ecosystem services and climates. It provides landowners and advisors with an evidence‐informed approach to increase field margin functionality while supporting farmland biodiversity
Analysis of averaged multichannel delay times
The physical significances and the pros and cons involved in the usage of
different time delay formalisms are discussed. The delay time matrix introduced
by Eisenbud, where only s-waves participate in a reaction, is in general
related to the definition of an angular time delay which is shown not to be
equivalent to the so-called phase time delay of Eisenbud and Wigner even for
single channel scattering. Whereas the expression due to Smith which is derived
from a time delayed radial wave packet is consistent with a lifetime matrix
which is Hermitian, this is not true for any Eisenbud-type lifetime matrix
which violates time reversal invariance. Extending the angular time delay of
Nussenzveig to multiple channels, we show that if one performs an average over
the directions and subtracts the forward angle contribution containing an
interference of the incident and scattered waves, the multichannel angle
dependent average time delay reduces to the one given by Smith. The present
work also rectifies a recently misinterpreted misnomer of the relation due to
Smith.Comment: 15 pages, LaTe
191. Biopsja węzła wartowniczego w operacyjnym raku gruczołu piersiowego – doświadczenia własne
Do chwili obecnej w przypadku raka piersi usunięcie układu chłonnego pachy jest obowiązkowym elementem postępowania chirurgicznego. Zajęcie węzłów chłonnych w przypadku raka piersi jest jednym z czynników rokowniczych jak i wpływa na podjęcie dalszego leczenia uzupełniającego i dlatego usunięcie pachowych węzłów chłonnych jest bardzo ważnym elementem leczenia operacyjnego raka piersi. Technika biopsji węzła wartowniczego (WW) rozwinęła się w przypadkach czerniaka złośliwego skóry i ma na celu precyzyjną ocenę stanu całego dorzecza węzłów chłonnych przy użyciu barwnika Paten Blau V, radioizotopu Tc99 ręcznej sóndy gamma kamery oraz małoinwazyjnej techniki chirurgicznej.Materiał i metodaW okresie od sierpnia 1998 roku do września 2003 roku w I Oddziale Chirurgii Onkologicznej Wielkopolskiego Centrum Onkologii w Poznaniu poddano biopsji WW 400 pacjentek z operacyjnym rakiem piersi. U wszystkich chorych klinicznie nie stwierdzano powiększonych węzłów chłonnych. Wiek pacjentek wahał się od 35 do 70 lat ze średnią wieku 55,2 lat. W przeddzień operacji podawano podskórnie w okolicę guza z czterech wkłuć Nannocoloid znaczony Tc99 w stężeniu 1 mCi zawarty w 4 mililitrach roztworu. Dnia następnego rano wykonywano limfoscyntygrafię celem wykonania mappingu węzła/węzłów wartowniczych. Następnie na sali operacyjnej podawano 1 do 2 mililitrów barwnika Patent Blau V w ten sam sposób, co radiokoloid. Przy użyciu ręcznej sondy gamma kamery identyfikowano miejsce największego wychwytu znacznika w pasze (tzw. Hot, Spot), które zaznaczano. Po odsłonięciu tkanki tłuszczowej pachy uwidaczniano wybarwione drogi chłonne, wzdłuż których dokonywano identyfikację wybarwionego węzła chłonnego. Następnie przy użyciu ręcznej sondy Navigator potwierdzano największy wychwyt promieniowania nad wybarwionym węzłem, w takim przypadku powyższy węzeł chłonny uważany był jako WW i przesyłany do pracowni patologicznej. Po identyfikacji WW chora poddawana była standardowej operacji (mastectomia lub BCT) wraz z limfadenektomią pachową jako nieodłącznym elementem procedury chirurgicznej.WynikiWW udało się zidentyfikować w 97% chorych. W przypadku 7 pacjentek nie udało się odnależć WW. Z pośród chorych z definiowanym WW przerzuty stwierdzono w 20% przypadków, w pozostałej części badanej grupy WW nie zawierał komórek nowotworowych, co stanowi 80% badanej populacji. W badanej grupie chorych stwierdzono 2 przypadki wyniku fałszywie ujemnego. W większoścr przypadków (87,1%) WW występował jako pojedynczy tylko u 2 pacjentów stwierdzono podwójny węzeł chłonny a u jednej chorej WW występował jako potrójny, ogółem mnogie WW wynosiły 2,88% populacji.WnioskiBiopsja WW jest bezpieczną metodą pozwalającą na ocenę dorzecza pachowych węzłów chłonnych w operacyjnym raku piersi. Wyniki nasze potwierdzają w pełni wyniki innych badaczy w Europie i na Świecie
Simple test for quantum channel capacity
Basing on states and channels isomorphism we point out that semidefinite
programming can be used as a quick test for nonzero one-way quantum channel
capacity. This can be achieved by search of symmetric extensions of states
isomorphic to a given quantum channel. With this method we provide examples of
quantum channels that can lead to high entanglement transmission but still have
zero one-way capacity, in particular, regions of symmetric extendibility for
isotropic states in arbitrary dimensions are presented. Further we derive {\it
a new entanglement parameter} based on (normalised) relative entropy distance
to the set of states that have symmetric extensions and show explicitly the
symmetric extension of isotropic states being the nearest to singlets in the
set of symmetrically extendible states. The suitable regularisation of the
parameter provides a new upper bound on one-way distillable entanglement.Comment: 6 pages, no figures, RevTeX4. Signifficantly corrected version. Claim
on continuity of channel capacities removed due to flaw in the corresponding
proof. Changes and corrections performed in the part proposing a new upper
bound on one-way distillable etanglement which happens to be not one-way
entanglement monoton
Constraints on R-parity violating couplings from LEP/SLD hadronic observables
We analyze the one loop corrections to hadronic Z decays in an R-parity
violating extension to the Minimal Supersymmetric Standard Model (MSSM).
Performing a global fit to all the hadronic observables at the Z-peak, we
obtain stringent constraints on the R-violating couplings constants lambda' and
lambda''. As a result of the strong constraints from the b asymmetry parameters
A_b and A_FB(b), we find that the couplings lambda'{i31}, lambda'{i32}, and
lambda''{321} are ruled out at the 1 sigma level, and that lambda'{i33} and
lambda''{33i} are ruled out at the 2 sigma level. We also obtain Bayesian
confidence limits for the R-violating couplings.Comment: 30 pages, 19 postscript figures, REVTeX, new section 8 on Bayesian
confidence limits adde
Charged Dual String Vacua from Interacting Rotating Black Holes Via Discrete and Nonlinear Symmetries
Using the stationary formulation of the toroidally compactified heterotic
string theory in terms of a pair of matrix Ernst potentials we consider the
four-dimensional truncation of this theory with no U(1) vector fields excited.
Imposing one time-like Killing vector permits us to express the stationary
effective action as a model in which gravity is coupled to a matrix Ernst
potential which, under certain parametrization, allows us to interpret the
matter sector of this theory as a double Ernst system. We generate a web of
string vacua which are related to each other via a set of discrete symmetries
of the effective action (some of them involve S-duality transformations and
possess non-perturbative character). Some physical implications of these
discrete symmetries are analyzed and we find that, in some particular cases,
they relate rotating black holes coupled to a dilaton with no Kalb--Ramond
field, static black holes with non-trivial dilaton and antisymmetric tensor
fields, and rotating and static naked singularities. Further, by applying a
nonlinear symmetry, namely, the so-called normalized Harrison transformation,
on the seed field configurations corresponding to these neutral backgrounds, we
recover the U(1)^n Abelian vector sector of the four-dimensional action of the
heterotic string, charging in this way the double Ernst system which
corresponds to each one of the neutral string vacua, i.e., the stationary and
the static black holes and the naked singularities.Comment: 19 pages in latex, added referenc
QCD corrections to electroweak l nu_l jj and l^+ l^- jj production
The production of W or Z bosons in association with two jets is an important
background to the Higgs boson search in vector-boson fusion at the LHC. The
purely electroweak component of this background is dominated by vector-boson
fusion, which exhibits kinematic distributions very similar to the Higgs boson
signal. We consider the next-to-leading order QCD corrections to the
electroweak production of l nu_l jj and l^+ l^- jj events at the LHC, within
typical vector-boson fusion cuts. We show that the QCD corrections are modest,
increasing the total cross sections by about 10%. Remaining scale uncertainties
are below 2%. A fully-flexible next-to-leading order partonic Monte Carlo
program allows to demonstrate these features for cross sections within typical
vector-boson-fusion acceptance cuts. Modest corrections are also found for
distributions.Comment: 26 pages, 10 figures. PRD final version. One reference corrected,
introduction expande
On the bound states of the Dirac equation in the extreme Kerr metric
We study the eigenvalues of the angular equation arising after the separation
of the Dirac equation in the extreme Kerr metric. To this purpose a
self-adjoint holomorphic operator family associated to this eigenvalue problem
is considered. We show that the eigenvalues satisfy a first order nonlinear
differential equation with respect to the black hole mass and we solve it.
Finally, we prove that there exist no bound states for the Dirac equation in
the aforementioned metric.Comment: 13 page
- …