Predictions for ${\bar \nu} \nu \gamma$ production at LEP

We study predictions for the reaction . The complete one-loop corrections are taken into account and higher order contributions, in particular those for the observed real photons, are added whenever necessary. The event generator MC, a general-purpose Monte Carlo generator for the process based on the method of exclusive exponentiation, is used as the environment. We extend its applicability to the process ,, where the observation of at least a single is required. The exponentiation is implemented in much the same way as for the s-channel process alone. In particular, all photonic effects present in the case of W exchange, which cannot be included in the s-channel exponentiation scheme, are calculated to a finite order only. The real hard photon matrix element is calculated up to . Leading logarithmic contributions of the two-loop corrections and one-loop photonic corrections accompanying real single-photon emission are included. The electroweak corrections are calculated with the DIZET library of the ZFITTER package. Numerical tests and predictions for typical observables are presented. Received: 30 October 2001 / Revised version: 5 March 2002 / Published online: 22 May 2002     

Tau Leptonic Decay τ→lVlVτ in Littlest Higgs Model＊

We consider the τ leptonic decay $\tau\rightarrow l\bar{\nu}_{l}\nu_{\tau}$ in the framework of the littlest Higgs (LH) model and calculate the corrections of new particles to this decay. We find that the contributions of the charged scalars can be safely ignored and the LH model is in perfect agreement with the universality of the couplings of the SU gauge bosons to the leptonic charged currents. The corrections of the LH model to the τ leptonic decay $\tau\rightarrow l\bar{\nu}_{l}\nu_{\tau}$ are not sensitive to the parameter c, but depend strongly on the parameters f and x. The precision measured data about the τ leptonic decay demand that the parameter f approximately equal 3.5 TeV and x>0.1, while agree with the general expectation based on other phenomenological explorations.     

On the polarization of the final nucleon in NC elastic \nu _\mu (\bar \nu _\mu )-N scattering

New short baseline neutrino experiments open new possibilities of high precision study of different neutrino processes. We present here results of the calculation of the polarization of final nucleon in elastic NC $\nu _\mu (\bar \nu _\mu )$ -nucleon scattering. In a numerical analysis the sensitivity to the different choices of the axial and axial strange form factors is examined. Measurements of the polarization of the final proton in elastic e-p scattering drastically changed our knowledge about the electromagnetic form factors of the proton. From measurement of the nucleon polarization in the NC elastic scattering a new additional information about the axial G _A (Q ²) and the strange axial G ^s _A (Q ²) form factors of the nucleon could be inferred.     

Search for $K^{+}\rightarrow \pi ^{+}\nu \bar \nu $ at CERN

The NA62 experiment at CERN SPS was designed to measure the \(BR(K^{+}\rightarrow \pi ^{+}\nu \bar \nu )\) with a decay-in-flight technique. NA62 took data in 2016, 2017 and 2018. Statistics collected in 2016 allowed NA62 to reach the Standard Model sensitivity and to show the proof of principle of the experiment. The preliminary result from the 2016 data set is presented.     

The Semileptonic Decay Modes {\bar{B} \rightarrow D\ell \bar{\nu}} and {\bar{B}_{s} \rightarrow D_{s} \ell \bar{\nu}}: A New Analysis in Potential Model

We consider the Schrödinger equation with a combination of Deng–Fan-type and harmonic terms. To solve the corresponding differential equation, we split the equation to two parts: the parent and the perturbation terms. We use the Nikiforov–Uvarov technique to solve the parent part. For the perturbation part, we apply the series expansion method. Next, using the calculated wave function, we investigate some bottom and charm mesons within the Isgur–Wise function formalism. We present especially semileptonic \({\bar{B} \rightarrow D\ell \bar{\nu}}\) and \({\bar{B}_{s} \rightarrow D_s \ell \bar{\nu }}\) decay widths, branching ratios and \({|V_{cb}|}\) (element of the CKM matrix). Masses of some pseudoscalar mesons are also indicated. Comparisons of our results with experimental values and other approaches are included.     

Self-focusing effects in a nematic liquid crystal at 10.6 $\mathsf{\mu}$m

E7 is a room temperature nematic liquid crystal that presents both a high temperature nematic-to-isotropic transition and a high positive dielectric anisotropy. The optical characteristics of this liquid crystal have been widely investigated in the visible region of the spectrum, while less experiments have been performed in the middle infrared spectral region, where, nevertheless, potential applications are important. We investigate the self-focusing of a middle infrared laser beam when it passes through a film of E7. We also take into account the heating of the liquid crystal film caused by the partial absorption of the laser light by means of a thermographic technique. A theoretical interpretation of the self-focusing phenomenon is given in terms of the reorientation of the molecules with respect to their unperturbed direction and an estimation of the average value of the elastic constants of the liquid crystal is given by fitting the experimental data with the theoretical model.Received: 16 April 2003PACS: 42.70.Df Liquid crystals - 42.65.-k Nonlinear optics - 42.55.Lt Gas lasers including excimer and metal-vapor lasers     

QCD sum rules analysis of the rare B_{c}\rightarrow X\nu\bar{\nu} decays

Taking into account the gluon correction contributions to the correlation function, the form factors relevant to the rare decays are calculated in the framework of the three-point QCD sum rules, where X stands for axial vector particle, AV(D _s1), and vector particles, V(D ^*,D _s ^*). The total decay width as well as the branching ratio of these decays are evaluated using the q ² dependent expressions of the form factors. A comparison of our results with the predictions of the relativistic constituent quark model is presented.     

Model independent calculation of {\cal{B}}({\bar{B}}^0\rightarrow D^{(*)+} \tau^-{\bar{\nu}})/{\cal{B}}({\bar{B}}^0\rightarrow D^{(*)+} e^-{\bar{\nu}})

Using the formulas for the distribution with non-zero lepton mass and experimentally determined form factors, we calculate the spectra and branching fractions for l = e, and . We obtain the results and . Since we used the experimentally measured form factors, these results are independent of theoretical models of the form factors.     

ZnO sensing structure for $\mbox{\sffamily\bfseries NH}_{\hbox{\sffamily\bfseries\fontsize{12}{12}\selectfont 3}}$ detection

Layered structure for the detection and measuring of gaseous ammonia have been presented. The presented sensor structures hale Bern developed on the base of thin ZnO and Au/Cr layers deposited on a glass substrate. The technological as well as optical properties of the elaborated sensing structures have been discussed.     

Biferroic electro – acoustic ceramics with $\mbox{\sffamily\bfseries BiFeO}_{\hbox{\sffamily\bfseries\fontsize{12}{12}\selectfont 3}}$ composition

Bismuth ferrite, one of a few multiferroics, has attracted much attention for many decades since 1960. BiFeO₃ (BFO) belongs to perovskite class of complex oxides. BFO is one of only a few materials in which (anti)ferromagnetism and ferroelectricity coexis in room temperature. Authors prepared BiFeO₃ ceramics by solid state reaction method. The synthesized powders were characterized by X-ray diffraction method. Thermogravimetric and differential thermal analysis were investigated. The microstructure of the BFO ceramics was investigated by means of scanning transmission electron microscopy, and the ferroelectric characteristic of BFO ceramics was demonstrated. BFO is very interesting ceramic material for potential applications in the memory devices, sensors, satellite communications, optical filters and smart devices.     

Double clad aluminosilicate optical fibre doped with $\mbox{\sffamily\bfseries Nd}^{\hbox{\sffamily\bfseries\fontsize{12}{12}\selectfont 3+}}$ ions

Double clad aluminosilicate optical fibre doped with neodymium ions was obtained. Aluminosilicate glasses with low silica (25 mol%) content possess very good optical, thermal and mechanical properties. Simultaneously they are characterized by high solubility of rare earth elements. A set of physical measurements including: DTA, DSC, DL analysis, absorption spectroscopy and thermo-physical properties (thermal stability parameters, refractive index, thermal expansion coefficient, microhardness, density and molar volume) were determined. Double-crucible drawing technique was applied to obtain neodymium doped double clad optical fibre with . Luminescence spectra of aluminosilicate glass and fibre doped with Nd^{3 +} ions are presented.     

70th birthday of Yuri $$\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l}$$ Antonovich Simonov

On the 70th Anniversary of Yurii Antonovich Simonov

70th birthday of Yuri $\overset{\lower0.5em\hbox{$\overset{\lower0.5em\hbox{ Antonovich Simonov     

Investigation of the $B_{c}\rightarrow\chi_{c2} l \overline {\nu} $ transition via QCD sum rules

We study the spectrum of the minimal supersymmetric extension of the Carroll–Field–Jackiw model for Electrodynamics with a topological Chern–Simons-like Lorentz-symmetry violating term. We identify a number of independent background fermion condensates, work out the gaugino dispersion relation and propose a photonic effective action to consider aspects of confinement induced by the SUSY background fermion condensates, which also appear to signal Lorentz-symmetry violation in the photino sector of the action. Our calculations of the static potential are carried out within the framework of the gauge-invariant but path-dependent variables formalism which are alternative to the Wilson loop approach. Our results show that the interaction energy contains a linear term leading to the confinement of static probe charges.     

Gauge invariance, infrared/collinear singularitiesand tree level matrix element for e^ + e^- \to \nu_e \bar{\nu}_e \gamma \gamma

One of the necessary steps in constructing a high-precision option of KKMC, a Monte Carlo program for the high-precision simulation of fermion pair production at LEP and Linear Collider energies, was to make a careful study of the appropriate matrix elements calculated from QED and the complete standard model. In particular, the installation of the double bremsstrahlung matrix element for the process into the scheme of coherent exclusive exponentiation (CEEX) was necessary. In the CEEX scheme one has to define an extrapolation and/or reduction procedure to enable the use of the matrix elements for kinematical configurations with a large number of outgoing particles. The process under study is particularly interesting because of the gauge cancellation of contributions for photon emission from incoming fermion lines and t-channel W. The QED U(1) gauge properties require terms of the triple and quartic gauge couplings to be taken into consideration as well. A natural separation of the complete amplitude into gauge invariant parts was found and is among the main results of the paper. Each part has a well defined physical interpretation, which after partial integration over phase space provides infrared singular, leading-log, next-to-leading-log, and other terms. Contributions related to the triple and quartic gauge coupling of W (extracted with the help of an expansion around the contact W-interaction) have been ordered as well. The separation can be of broader interest; it originates from the rigorous calculation of matrix elements; it visualizes, in the language of spin amplitudes, the properties of factorization necessary for the common multi-process picture. For example, the multiple photon algorithm of PHOTOS, based on the parton shower-like approach, profits from similar considerations. These somewhat speculative aspects of the calculation will be mentioned in the paper as well. Received: 24 April 2005, Revised: 22 July 2005, Published online: 11 October 2005 Supported in part by the EU grant MTKD-CT-2004-510126, in patnership with the CERN Physics department, and Polish State Committee for Scientific Research (KBN) grant 2 P03B 091 27 for years 2004-2006.