排序方式: 共有48条查询结果,搜索用时 46 毫秒
11.
Aihara H Alston-Garnjost M Avery RE Barker AR Bauer DA Bay A Belcinski R Bingham HH Bloom ED Buchanan CD Caldwell DO Chao HY Chun SB Clark AR Cowan GD Crane DA Dahl OI Daoudi M Derby KA Eastman JJ Eberhard PH Edberg TK Eisner AM Erné FC Fairfield KH Fridman A Godfrey G Hauptman JM Ho C Hofmann W Kamae T Kenney RW Khacheryan S Kofler RR Lambert DJ Langeveld WG Layter JG Lin WT Linde FL Loken SC Lu A Lynch GR Lys JE Madaras RJ Magnuson BD Marsiske H Masek GE Mathis LG Maxfield SJ Miller ES 《Physical review D: Particles and fields》1991,43(1):29-33
12.
Aihara H Alston-Garnjost M Avery RE Barbaro-Galtieri A Barker AR Barnett BA Bauer DA Bay A Bobbink GJ Buchanan CD Buijs A Caldwell DO Chao HY Chun SB Clark AR Cowan GD Crane DA Dahl OI Daoudi M Derby KA Eastman JJ Eberhard PH Edberg TK Eisner AM Erné FC Fairfield KH Hauptman JM Hofmann W Hylen J Kamae T Kaye HS Kenney RW Khacheryan S Kofler RR Langeveld WG Layter JG Lin WT Linde FL Loken SC Lu A Lynch GR Madaras RJ Magnuson BD Masek GE Mathis LG Matthews JA Maxfield SJ Miller ES Moses W 《Physical review letters》1990,64(2):172-175
13.
Aihara H Alston-Garnjost M Avery RE Barbaro-Galtieri A Barker AR Barnes AV Barnett BA Bauer DA Bengtsson H Bintinger DL Bobbink GJ Bolognese TS Bross AD Buchanan CD Buijs A Caldwell DO Clark AR Cowan GD Crane DA Dahl OI Derby KA Eastman JJ Eberhard PH Edberg TK Eisner AM Enomoto R Erné FC Fujii T Gary JW Gorn W Hauptman JM Hofmann W Huth JE Hylen J Kamae T Kaye HS Kees KH Kenney RW Kerth LT Ko W Koda RI Kofler RR Kwong KK Lander RL Langeveld WG Layter JG Linde FL Lindsey CS Loken SC Lu A Lu X 《Physical review letters》1986,57(25):3140-3143
14.
Aihara H Alston-Garnjost M Avery RE Barbaro-Galtieri A Barker AR Barnes AV Barnett BA Bauer DA Bengtsson H Bintinger DL Bobbink GJ Bolognese TS Bross AD Buchanan CD Buijs A Caldwell DO Clark AR Cowan GD Crane DA Dahl OI Derby KA Eastman JJ Eberhard PH Edberg TK Eisner AM Enomoto R Erné FC Fujii T Gary JW Gorn W Hauptman JM Hofmann W Huth JE Hylen J Kamae T Kaye HS Kees KH Kenney RW Kerth LT Ko W Koda RI Kofler RR Kwong KK Lander RL Langeveld WG Layter JG Linde FL Lindsey CS Loken SC Lu A Lu XQ 《Physical review letters》1986,57(20):2500-2503
15.
For a family of homogeneous Moran sets, where at each level, subintervals are arranged with in-creasing spaces between neighboring subintervals from left to right, we obtained a formula of the Hausdorff dimensions. 相似文献
16.
Let Ω⊂{0,1}N be a nonempty closed set with N={0,1,2,…}. For N={N0<N1<N2<?}⊂N and ω∈{0,1}N, define ω[N]∈{0,1}N by and
17.
A numeration system Ω is a compactification of the set of real numbers keeping the actions of addition and positive multiplication
in a natural way. That is, Ω is a compact metrizable space with #Ω≥2 to which ℝ acts additively andG acts multiplicatively satisfying the distributive law, whereG is a nontrivial closed multiplicative subgroup of ℝ+. Moreover, the additive action is minimal and uniquely ergodic with 0-topological entropy, while the multiplication by λ
has |log λ|-topological entropy attained uniquely by the unique invariant probability measure under the additive action.
We construct Ω as above as a colored tiling space corresponding to a weighted substitution. This framework contains especially
the substitution dynamical systems and β-transformation systems with periodic expansion of 1, both of which have discreteG. It also contains systems withG=ℝ+. We study α-homogeneous cocycles on it with respect to the addition. They are interesting from the point of view of fractal
functions or sets as well as self-similar processes. We obtain the zeta-functions of Ω with respect to the multiplication. 相似文献
18.
H. Aihara J. Chiba H. Fujii T. Fujii H. Iwasaki T. Kamae K. Nakamura T. Sumiyoshi Y. Takada T. Takeda M. Yamauchi 《Nuclear Physics A》1981,360(2):291-296
Absorption cross sections for antiprotons on C, Al and Cu have been measured by a transmission method at 485 and 597 MeV/c. Nuclei are shown to be black to antiprotons at these momenta. Using the available data up to 280 GeV/c, the momentum dependence of the absorption cross sections is investigated. Empirically, a simple expression σabs = γ(p/p0)−β, with β and γ constants and p0 = 1 GeV/c, gives a good account of the data in a remarkably wide momentum range, 0.5–280 GeV/c. 相似文献
19.
‘Fractal’ functions are formulated as a minimal cocycle on a topological dynamics which admits nontrivial scaling transformations.
In this paper, it is proved that if in addition it admits a continuous family of scaling transformations, then itscapacity is not ino(N
2). We define minimal cocycles with nontrivial scaling transformations coming from substitutions on a finite alphabet which
are proved to have capacityO(N), so that they admit only a discrete family of scaling transformations. We also construct one which has capacityO(N
2) and admit a continuous family of scaling transformations.
Supported by C.N.R.S.(U.R.A 225); Partially supported by the Japan Society for the Promotion of Science. 相似文献
20.
Two theoretical models of γd → pn are developed to study the differential cross-section and'the proton polarization data in a coherent way. The first model is an extension of conventional diagrammatic summations of Born terms and isobar excitation terms. The second model is novel in that the isobar excitation terms are replaced by experimentally determined γN → Nπ helicity amplitudes. The second model allows us to extend to higher energies with the introduction of only one arbitrary parameter. The differential cross-section data are fairly well reproduced in the whole energy range, while the proton polarization data are very far removed from the calculations. 相似文献