A. Stevens
Brookhaven National Laboratory
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Physical Review Letters | 1997
Stephen L. Adler; A. Stevens; S. H. Kettell; A. Konaka; James MacDonald; J. S. Haggerty; C. Witzig; S. Sugimoto; Y. Kuno; A. J. S. Smith; L. S. Littenberg; D. A. Bryman; P. Kitching; T. Shinkawa; Masato Aoki; M. M. Ito; J. S. Frank; R. Soluk; C. Ng; Andre Spence Turcot; F. C. Shoemaker; Y. Yoshimura; Y. Kishi; R. C. Strand; J.R. Stone; Robert McPherson; M. V. Diwan; T. F. Kycia; J.-M. Poutissou; M. Kuriki
An event consistent with the signature expected for the rare kaon decay K+ --> pi+ nu anti-nu has been observed. In the pion momentum region examined, 211 pi+ nu anti-nu, the branching ratio is (4.2 +9.7/-3.5) x E-10.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2003
H. Hahn; E. Forsyth; H. Foelsche; M. Harrison; J. Kewisch; G. Parzen; S. Peggs; E. Raka; Alessandro G. Ruggiero; A. Stevens; S. Tepikian; P. Thieberger; Dejan Trbojevic; J. Wei; E. Willen; S. Ozaki; S.Y. Lee
The salient performance objectives for the Relativistic Heavy Ion Collider (RHIC) are presented and the rationale for the design choices of the major collider systems is conveyed. RHIC provides collisions of heavy ions covering the entire mass range from protons to gold. For the prototypical case of Au-on-Au, one obtains energies up to 100 GeV/n per beam and luminosities of B2 � 10 26 cm � 2 s � 1 , averaged over a 10-h storage time. Operation with polarized protons is also possible. The overall accelerator complex used for gold ions consists of the Tandem Van de Graaff, the Booster, the AGS, and the Collider itself, and the scenario for the beam transfer between machines is described. The two separate collider rings cross at six interaction points, where the lattice design provides low-beta insertions for maximum luminosity. The interaction diamond length of o20 cm rms is achieved by bunched beam operation and holding the 56 bunches in a 197 MHz radio-frequency (RF) system after their acceleration in a 28 MHz RF system. The rings are constructed with superconducting magnets, which have a cold bore aperture of 6.9 cm in the arcs. The RHIC specific design challenges posed by intrabeam scattering of heavy ions, passage through transition energy with slow-ramping superconducting magnets, and control of magnetic errors in the low-beta triplet quadrupoles are addressed. r 2002 Elsevier Science B.V. All rights reserved.
Physical Review Letters | 1997
P. Kitching; Tomoyuki Nakano; M. Rozon; R. Soluk; Stephen L. Adler; M. S. Atiya; I-H. Chiang; J. S. Frank; J. S. Haggerty; T. F. Kycia; K. K. Li; L. S. Littenberg; A. Sambamurti; A. Stevens; R. C. Strand; C. Witzig; W. C. Louis; D. S. Akerib; M. Ardebili; M. R. Convery; M. M. Ito; D. Marlow; Robert McPherson; P. D. Meyers; M. Selen; F. C. Shoemaker; A. J. S. Smith; E. W. Blackmore; D. A. Bryman; L. Felawka
The first observation of the decay K + ! � + is reported. A total of 31 events was observed with an estimated background of 5.1±3.3 events in the � + momentum range from 100 MeV/c to 180 MeV/c. The corresponding partial branching ratio, B(K + ! � + , 100 MeV/c < P�+ < 180 MeV/c), is (6.0±1.5{stat}±0.7{sys})×10 7 . No K + ! � + decay was observed in the � + momentum region greater than 215 MeV/c. The observed � + momentum spectrum is compared with the predictions of chiral perturbation theory.
Physical Review Letters | 1997
Stephen L. Adler; Atiya; I-H. Chiang; J. S. Frank; J. S. Haggerty; T. F. Kycia; K. K. Li; L. S. Littenberg; A. Sambamurti; A. Stevens; R. C. Strand; C. Witzig; W. C. Louis; D. S. Akerib; M. Ardebili; M. R. Convery; M. M. Ito; D. Marlow; Robert McPherson; P. D. Meyers; Selen; F. C. Shoemaker; A. J. S. Smith; E. W. Blackmore; D. A. Bryman; L. Felawka; A. Konaka; Y. Kuno; James MacDonald; T. Numao
We have observed the rare decay K+ --> pi+ mu+ mu- and measured the branching ratio Gamma(K+ --> pi+ mu+ mu-)/Gamma(K+ --> all) = (5.0 +/- 0.4 (stat.) +/- 0.7 (sys.) +/- 0.6 (theor.)) x 10^{-8}. We compare this result with predictions from chiral perturbation theory and estimates based on the decay K+ --> pi+ e+ e-.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992
M. S. Atiya; I-H. Chiang; J.S. Frank; E. Garber; J. S. Haggerty; M. M. Ito; T.F. Kycia; K.K. Li; L. S. Littenberg; C. Ng; I. Polk; R. Rosenka; A.K. Sambamurti; A. Stevens; R.C. Strand; C. Zein; D. S. Akerib; H. Edwards; W.C. Louis; Daniel Marlow; P. D. Meyers; M.A. Selen; F. C. Shoemaker; A. J. S. Smith; S. Ahmad; Ewart W. Blackmore; D. A. Bryman; J.V. Cresswell; L. Felawka; N. Khan
Abstract The detector built for experiment 787 to measure the decay K + → π + ν ν at Brookhaven National Laboratory is describe
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1985
E.J. Bleser; J. G. Cottingham; P. Dahl; R.J. Engelmann; R. Fernow; M. Garber; A. Ghosh; C. Goodzeit; A. Greene; J. Herrera; S. Kahn; J. Kaugerts; E. Kelly; H. Kirk; R.J. Leroy; G. Morgan; Robert B. Palmer; A. Prodell; D. Rahm; W. Sampson; R. Shutt; A. Stevens; M. J. Tannenbaum; P. Thompson; P. Wanderer; E. Willen
Abstract The superconducting magnets that were designed and tested for the BNL colliding beam accelerator are described, including dipoles, quadrupoles and trim coils. The dipoles had an effective length of 436 cm, a good field aperture of 8.8 cm diameter, and were designed for an operating field of 5.28 T in a temperature range between 2.6 K and 3.8 K (provided by supercritical helium). The quadrupoles had the same aperture, an effective length of 138.5 cm, and were designed to operate in series with the dipoles, with a gradient of 70.8 T/m. The dipoles incorporated internal sextupole, octupole, and decapole trim coil windings; the quadrupole trim coils consisted of dipole, quadrupole, and dodecapole windings. The design, construction, and performance (training, field quality, quench protection characteristics) of prototype magnets are discussed in considerable detail.
Physical Review Letters | 1996
Stephen L. Adler; M. S. Atiya; I-H. Chiang; J. S. Frank; J. S. Haggerty; T. F. Kycia; K. K. Li; L. S. Littenberg; A. Sambamurti; A. Stevens; R. C. Strand; C. Witzig; W. C. Louis; D. S. Akerib; M. Ardebili; M. R. Convery; M. M. Ito; D. Marlow; Robert McPherson; P. D. Meyers; M. Selen; F. C. Shoemaker; A. J. S. Smith; E. W. Blackmore; D. A. Bryman; L. Felawka; P. Kitching; A. Konaka; V. A. Kujala; Y. Kuno
An upper limit on the branching ratio for the decay
Physical Review Letters | 1989
M. S. Atiya; I-H. Chiang; J. S. Frank; J. S. Haggerty; M. M. Ito; T. F. Kycia; K. K. Li; L. S. Littenberg; A. Stevens; R. C. Strand; W. C. Louis; D. S. Akerib; Michael Hildreth; D. Marlow; P. D. Meyers; M. A. Selen; F. C. Shoemaker; A. J. S. Smith; G. Azuelos; E. W. Blackmore; D. A. Bryman; L. Felawka; P. Kitching; Y. Kuno; James MacDonald; T. Numao; P. Padley; J.-M. Poutissou; R. Poutissou; J. Roy
K^+ \! \rightarrow \! \pi^+ \nu \overline{\nu}
Physical Review Letters | 2000
Stephen L. Adler; M. S. Atiya; I-H. Chiang; M. V. Diwan; J. S. Frank; J. S. Haggerty; S. H. Kettell; T. F. Kycia; K. K. Li; L. S. Littenberg; A. Sambamurti; A. Stevens; R. C. Strand; C. Witzig; T. K. Komatsubara; M. Kuriki; N. Muramatsu; Shigeki Sugimoto; T. Inagaki; S. Kabe; Michiko Kobayashi; Y. Kuno; Tadashi Sato; Takao Shinkawa; Y. Yoshimura; Y. Kishi
is set at
Physical Review Letters | 1993
Atiya; I-H. Chiang; J. S. Frank; J. S. Haggerty; Masaharu Ito; T. F. Kycia; K. K. Li; L. S. Littenberg; A. Sambamurti; A. Stevens; R. C. Strand; W. C. Louis; D. S. Akerib; D. Marlow; P. D. Meyers; Selen; F. C. Shoemaker; A. J. S. Smith; E. W. Blackmore; D. A. Bryman; L. Felawka; P. Kitching; A. Konaka; Y. Kuno; J. A. Macdonald; Toshio Numao; P. Padley; J.-M. Poutissou; R. Poutissou; J. Roy
2.4 \times 10^{-9}