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161.
Abachi S Abbott B Abolins M Acharya BS Adam I Adams DL Adams M Ahn S Aihara H Alitti J Álvarez G Alves GA Amidi E Amos N Anderson EW Aronson SH Astur R Avery RE Balamurali V Balderston J Baldin B Bantly J Bartlett JF Bazizi K Bendich J Beri SB Bertram I Bezzubov VA Bhat PC Bhatnagar V Bhattacharjee M Bischoff A Biswas N Blazey G Blessing S Boehnlein A Bojko NI Borcherding F Borders J Boswell C Brandt A Brock R Bross A Buchholz D Burtovoi VS Butler JM Casey D Castilla-Valdez H Chakraborty D 《Physical review letters》1995,74(14):2632-2637
162.
Abbott B Abolins M Abramov V Acharya BS Adams DL Adams M Ahn S Akimov V Alves GA Amos N Anderson EW Baarmand MM Babintsev VV Babukhadia L Baden A Baldin B Banerjee S Bantly J Barberis E Baringer P Bartlett JF Bassler U Belyaev A Beri SB Bernardi G Bertram I Bezzubov VA Bhat PC Bhatnagar V Bhattacharjee M Blazey G Blessing S Boehnlein A Bojko NI Borcherding F Brandt A Breedon R Briskin G Brock R Brooijmans G Bross A Buchholz D Buescher V Burtovoi VS Butler JM Carvalho W Casey D Casilum Z 《Physical review letters》2000,84(25):5710-5715
We report on a measurement of sigma(pp-->W+X)B(W-->taunu) in pp collisions at sqrt[s]=1.8 TeV at the Fermilab Tevatron. The measurement is based on an integrated luminosity (lum) of 18 pb-1 of data collected with the D0 detector during 1994-1995. We find that sigma(pp-->W+X)B(W-->taunu)=2.22+/-0.09 (stat)+/-0. 10 (syst)+/-0.10 (lum) nb. Lepton universality predicts that the ratio of the tau and electron electroweak charged current couplings to the W boson, gWtau/gWe, be unity. We find gWtau/gWe=0.980+/-0.031, in agreement with lepton universality. 相似文献
163.
Four-term recurrence relations with constant coefficients are derived for a wide class of T chebycheffian B-splines, LB-splines
and complex B-splines. Such a relation exists whenever the differential operator defining the underlying “polynomial” space
can be factored in two essentially different ways. The four lower order B-splines in the recurrence relation appear in two
pairs, each pair corresponding to one of these factorization. It is shown that the two-term recurrence relations for polynomial,
trigonometric and hyperbolic B-splines as well as other known two-term recurrence relations are obtained directly from the
four-term recurrence relations in a unified and systematic way. The above derivation also yields two different two-term recurrence
relations for Green’s functions of these “polynomial” spaces In this context the special examples of exponential functions
and rational functions are analyzed in detail. 相似文献
164.
Stimulated by recent work of Hakopian and Sahakian, polynomial interpolation to data at all the s-dimensional intersections of an arbitrary sequence of hyperplanes in
d is considered, and reduced, by the adjunction of an additional s hyperplanes in general position with respect to the given sequence, to the case s=0 solved much earlier by two of the present authors. In particular, interpolation is from the very same polynomial spaces already used earlier. The difficult question of multiplicity and corresponding matching of derivative information is completely solved, with the number of independent derivative conditions at an intersection exactly equal to that intersection's multiplicity. Also, the consistency requirements placed on the data are minimal in the sense that they need to be checked only at the finitely many 0-dimensional intersections of the hyperplanes involved. The arguments used provide, incidentally, further insights into the two polynomial spaces,
(Ξ) and
(Ξ), of basic interest in box spline theory. 相似文献
165.
Amos Uderzo 《Set-Valued and Variational Analysis》2014,22(2):483-501
In the present paper, the Polyak’s principle, concerning convexity of the images of small balls through C1, 1 mappings, is employed in the study of vector optimization problems. This leads to extend to such a context achievements of local programming, an approach to nonlinear optimization, due to B.T. Polyak, which consists in exploiting the benefits of the convex local behaviour of certain nonconvex problems. In doing so, solution existence and optimality conditions are established for localizations of vector optimization problems, whose data satisfy proper assumptions. Such results are subsequently applied in the analysis of welfare economics, in the case of an exchange economy model with infinite-dimensional commodity space. In such a setting, the localization of an economy yields existence of Pareto optimal allocations, which, under certain additional assumptions, lead to competitive equilibria. 相似文献
166.
Karlheinz Grö chenig Amos Ron 《Proceedings of the American Mathematical Society》1998,126(4):1101-1107
Based on Ron and Shen's new method for constructing tight wave-let frames, we show that one can construct, for any dilation matrix, and in any spatial dimension, tight wavelet frames generated by compactly supported functions with arbitrarily high smoothness.
167.
Canton L Pisent G Svenne JP van der Knijff D Amos K Karataglidis S 《Physical review letters》2005,94(12):122503
A multichannel algebraic scattering theory, to find solutions of coupled-channel scattering problems with interactions determined by collective models, has been structured to ensure that the Pauli principle is not violated. By tracking the results in the zero coupling limit, a correct interpretation of the subthreshold and resonant spectra of the compound system can be made. As an example, the neutron-12C system is studied defining properties of 13C to 10 MeV excitation. Accounting for the Pauli principle in collective coupled-channels models is crucial to the outcome. 相似文献
168.
We analyze the situation of an observer coaccelerated relative to a linearly accelerated charge, in order to find whether
he can observe the radiation emitted from the accelerated charge. It is found that the seemingly special situation of the
coaccelerated observer relative to any other observer, is deduced from a wrong use of the retarded coordinate system, when
such a system is inadmissible. It is also found that the coaccelerated observer has no special position other than any other
observer, and hence, he can observe any physical events as any other observer. 相似文献
169.
Direct reaction (p, n) data to the isobaric analogue of the ground state of 90Zr is analysed within a DWA using a complex effective two-nucleon transition interaction, the real part of which has been used in many previous inelastic scattering analyses. Using collective model form factors in the ansatz for the imaginary part of the transition interaction and allowing for virtual resonance excitation, the differential cross sections from the scattering of 18.5–45 MeV protons are well reproduced. The parameters of the required complex interaction have a smooth energy variation similar to that required by a microscopic model analysis of proton inelastic scattering to collective states in nuclei. 相似文献
170.
The differential cross sections for the inelastic scattering of 10 MeV, 19.6 MeV, 30.4 MeV, 40 MeV and 49.35 MeV protons to the 2+ state (1.409 MeV) in 54Fe and of 19.6 MeV protons to the 2+ state (0.846 MeV) in 56Fe are analyzed in conjunction with the available data on the asymmetries and spin-flip probability amplitudes. The scattering amplitudes for both one step (valence plus core polarization) and two step (intermediate resonance) processes are evaluated using an antisymmetrized distorted wave approximation. Collective model representations for both the one step (core polarization) and two step (intermediate resonance) processes are used, and included are the effects of deforming the full Thomas spin-orbit potentials. The one step processes are fixed by the analyses of the scattering of 30.4, 40 and 49.35 MeV protons, with the core polarization contributions being constrained by the B(E2) values for the γ-ray deexcitation of the 2+ states. The analyses of the 19.6 MeV data demonstrates the need for an extra (two step) contribution to the reaction process and are consistent with the virtual formation of an L = 3 giant resonance. The 10 MeV data most certainly demonstrate compound nucleus effects but could also have some strength due to the virtual formation of an intermediate L = 2 giant resonance. The resonance parameters are consistent with recent information concerning the mass variation of giant resonances. 相似文献