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961.
Aubert B Bona M Boutigny D Karyotakis Y Lees JP Poireau V Prudent X Tisserand V Zghiche A Garra Tico J Grauges E Lopez L Palano A Pappagallo M Eigen G Stugu B Sun L Abrams GS Battaglia M Brown DN Button-Shafer J Cahn RN Groysman Y Jacobsen RG Kadyk JA Kerth LT Kolomensky YG Kukartsev G Lopes Pegna D Lynch G Mir LM Orimoto TJ Osipenkov IL Ronan MT Tackmann K Tanabe T Wenzel WA Del Amo Sanchez P Hawkes CM Watson AT Koch H Schroeder T Walker D Asgeirsson DJ Cuhadar-Donszelmann T Fulsom BG Hearty C 《Physical review letters》2008,100(13):131802
We report results of a search for CPT and Lorentz violation in B(0)-B[over ](0) oscillations using inclusive dilepton events from 232 x 10(6) Upsilon(4S)-->BB[over ] decays recorded by the BABAR detector at the PEP-II B Factory at SLAC. We find 2.8sigma significance, compatible with no signal, for variations in the complex CPT violation parameter z at the Earth's sidereal frequency and extract values for the quantities Deltaa(micro) in the general Lorentz-violating standard-model extension. The spectral powers for variations in z over the frequency range 0.26 yr(-1) to 2.1 solar day(-1) are also compatible with no signal. 相似文献
962.
S.David Chappell David J. Cole-Hamilton Anita M.R. Galas Michael B. Hursthouse Nigel P.C. Walker 《Polyhedron》1985,4(1):121-125
Reaction of [RhCl(PPh3)3] with [o-MeC6H4CH2MgBr] affords high yields of the non-fluxional complex, [Rh(CH2C6H4Me)(PPh3)2] which has been shown crystallographically to contain a 1-3-η-benzyl group bound through the phenyl carbon atom that is not substituted with the methyl group. Crystals of this compound are triclinic, space group P, with a = 10.561(6). b = 17.705(3), c = 10.934(4) Å, α = 80.69(3), β = 116.86(4), γ = 102.30(4)° and Z = 2. The structure was solved via the heavy-atom method and refined to R = 0.032 using 5379 diffractometer data with I > 1.56(I). Attempts to prepare π-bonded xylylene complexes from this compound by reaction with base have been unsuccessful, but protonation followed by recrystallisation from acetone gives [Rh{(CH3)2CO}2(PPh3)2]BF4. 相似文献
963.
On Backtracking Failure in Newton–GMRES Methods with a Demonstration for the Navier–Stokes Equations
Raymond S. Tuminaro Homer F. Walker John N. Shadid 《Journal of computational physics》2002,180(2):549
In an earlier study of inexact Newton methods, we pointed out that certain counterintuitive behavior may occur when applying residual backtracking to the Navier–Stokes equations with heat and mass transport. Specifically, it was observed that a Newton–GMRES method globalized by backtracking (linesearch, damping) may be less robust when high accuracy is required of each linear solve in the Newton sequence than when less accuracy is required. In this brief discussion, we offer a possible explanation for this phenomenon, together with an illustrative numerical experiment involving the Navier–Stokes equations. 相似文献
964.
965.
The thermoreflectance spectrum of CuI in the 4–7 eV region is reported. New structure in the region has been assigned to the spin-orbit split triplet between the first valence band and the second conduction band at k=0. The magnitude of the splitting indicates an inverted order in the second conduction band and a large d-state mixture in the valence band. 相似文献
966.
Using a separable fixed scatterer pion-nucleon interaction and the distorted wave impulse approximation we have made predictions for medium energy pion inelastic scattering from 16O and (π?, π0) charge exchange from 48Ca. An optical potential based on the pion-nucleon interaction adopted in this work has been shown previously to provide good fits to pion-nucleus elastic scattering. After a discussion of the basic formulae, we present results of calculations for pion inelastic scattering from 16O for initial pion lab kinetic energies of 70 and 180 MeV. Because of the strong energy dependence of the pion-nucleon interaction there are qualitative differences between the predictions for the nuclear response in the momentum transfer, energy loss plane for Tπlab = 70 and 180 MeV. At these energies, states not prominently excited by other probes are predicted to be observable. In particular, Jπ = 3? and 4?, T = 0 states appear prominently in the excitation spectrum region at large momentum transfer. A comparison of π? and π+ scattering showing the effects of the Coulomb interaction is presented. The predictions for pion single-charge exchange on 48Ca indicate that this interaction would be useful for studying the location of the T> states arising from the splitting of the giant dipole resonance in T ≠ 0 nuclei. 相似文献
967.
968.
969.
M.E. Binkley J.R. Elliott L.R. Fortney J.S. Loos W.J. Robertson C.M. Rose W.D. Walker W.M. Yeager G.W. Meisner R.B. Muir 《Physics letters. [Part B]》1973,45(3):295-298
Measurement of the π0 multiplicity cross sections are reported for n0 ? 6, where n0 is the number of produced π0 particles, and for N ? 8, where N is the number of charged particles. The inclusive π0 cross section is 29 ± 3 mb. Values for the correlation parameters, 〈n0〉 and 〈n0(n0 ? 1)〉2, are also presented. 相似文献
970.
John Walker 《The Journal of the Operational Research Society》1978,29(9):915-922
In this paper, a man-machine interactive method is presented as an aid in solving the bicriterion mathematical programming problem. It is assumed that the two objective functions are real-valued functions of the decision variables which are themselves constrained to some compact and nonempty set. The overall utility function is assumed to be unknown explicitly to the decision-maker but is assumed to be a real-valued function defined on the pairs of feasible values of the objective functions and monotone non-decreasing in each argument. The decision-maker is required only to provide yes or no answers to questions regarding the desirability of increase or decrease in objective function values of solutions that he will not accept as optimal. Convergence of the method is indicated and a numerical example is presented in order to demonstrate its applicability. 相似文献