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Featured researches published by R. Kajikawa.


Nuclear Physics | 1988

A study of K−π+ scattering in the reaction K−p→K−π+n at 11 GeV/c

D. Aston; N. Awaji; T. Bienz; F. Bird; J. D'Amore; W. Dunwoodie; R. Endorf; K. Fujii; H. Hayashi; S. Iwata; W.B. Johnson; R. Kajikawa; P. Kunz; D. W. G. S. Leith; L. Levinson; T. Matsui; B. T. Meadows; A. Miyamoto; M. Nussbaum; H. Ozaki; C.O. Pak; B. N. Ratcliff; D. Schultz; S. Shapiro; T. Shimomura; P.K. Sinervo; A. Sugiyama; S. Suzuki; G. Tarnopolsky; T. Tauchi

Results from a high statistics study of the reaction K−p→K−π+n are presented. These results are based on data obtained with an 11 GeV/c beam using the LASS spectrometer at SLAC. The mass dependence of the spherical harmonic moments provides clear evidence for the production of the complete leading orbitally excited K∗ series up through JP = 5−. These moments are used to perform an energy independent partial wave analysis of the K−π+ system from threshold to 2.6 GeV/c2 using a t-dependent parametrization of the production amplitudes. The amplitudes corroborate the leading K∗(892), K2∗(1430), K3∗(1780), K4∗(2060), and K5∗(2380) resonances observed directly in the moments, and also provide new evidence for underlying states. The 0+ amplitude contains the K0∗(1350) and a second 0+K∗(1950) at higher mass. The 1−K∗(1790) seen earlier two and three-body analyses is confirmed, and evidence is provided for suppressed K−π+ decay mode of a second 1− state, the K∗(1410), which has been seen in earlier three-body analyses.


Nuclear Physics | 1988

A study of the Ks0Ks0 system in the reaction K−p→Ks0Ks0Λ at 11 GeV/c

D. Aston; N. Awaji; T. Bienz; F. Bird; J. D'Amore; W. Dunwoodie; R. Endorf; K. Fujii; H. Hayashii; S. Iwata; W.B. Johnson; R. Kajikawa; P. Kunz; D. W. G. S. Leith; L. Levinson; T. Matsui; B. T. Meadows; A. Miyamoto; M. Nussbaum; H. Ozaki; C.O. Pak; B. N. Ratcliff; D. Schultz; S. Shapiro; T. Shimomura; P.K. Sinervo; A. Sugiyama; S. Suzuki; G. Tarnopolsky; T. Tauchi

Abstract A 4.1 event/nb sample of 11 GeV/c K−p interactions in the LASS spectrometer at SLAC has been used in an analysis of the exclusive Ks0Ks0Λ final state. The Ks0Ks0 mass distribution exhibits a small cluster of events near threshold, but the mass spectrum is dominated by the f2′(1525), which an amplitude analysis shows to be produced by both natural and unnatural parity exchange. This analysis also provides evidence for an S-wave state in the f2′(1525) region, while production of the f2(1720) is not observed. However, there is structure at ∼ 2.2 GeV/c2 which is similar in shape to that observed in the region of the X(2220) in radiative J/ψ decay; an analysis of the angular distribution indicates a spin of at least 2 in this region. This, together with results from other analyses, indicates that the X(2220) may be the 2++ or 4++, mainly s s , state expected near this mass in the conventional quark model.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1987

A gas sampling electromagnetic calorimeter using conductive plastic tubes

J. Fujimoto; R. Kajikawa; S. Kuroda; H. Ozaki; H. Masuda; A. Sugiyama; S. Suzuki; T. Takahashi; T.F. Tsukamoto; T.Y. Tsukamoto; M. Ueda; S. Uno

A prototype of gas sampling electromagnetic calorimeter with conductive plastic tubes was studied under practical conditions. An energy resolution of σEE = 20.4(E(GeV))−12 (%) was obtained in the few-GeV region and the spatial resolu for 4 GeV electrons was σx = 5.4 mm for pads and σx = 2.2 mm for strips. No appreciable effect on the energy resolution was found by magnetic field of 1 kG applied perpendicularly to the anode wire.


Physics Letters B | 1993

Measurement of the inclusive cross section of jets in γγ interactions at TRISTAN

H. Hayashii; A. Miyamoto; M. Iwasaki; S. Noguchi; N. Fujiwara; T. Abe; K. Abe; I. Adachi; M. Aoki; S. Awa; R. Belusevic; K. Emi; R. Enomoto; H. Fujii; K. Fujii; T. Fujii; J. Fujimoto; K. Fujita; B. Howell; N. Iida; H. Ikeda; R. Itoh; H. Iwasaki; R. Kajikawa; S. Kato; S. Kawabata; H. Kichimi; M. Kobayashi; D. Koltick; I. Levine

Abstract We have investigated the properties of jet production in almost real γγ collisions at √s=58 GeV with the TOPAZ detector at the TRISTAN e+e− collider. The data were analyzed with a jet-clustering method based on a cone algorithm. The jet rate shows evidence for a hard scattering effect of the hadronic constituents of a photon (resolved photon processes). We have also observed a substantial energy flow in the small-angle region, which is additional evidence for resolved photon processes. We present the transverse momentum dependence of the inclusive jet and two-jet cross sections and compare them with different model predictions.


Physics Letters B | 1988

Evidence for two strangeonium resonances with JPC=1++ and 1+− in K−p interactions at 11 GeV/c☆

D. Aston; N. Awaji; T. Bienz; F. Bird; J. D'Amore; W. Dunwoodie; R. Endorf; K. Fujii; H. Hayashi; S. Iwata; W.B. Johnson; R. Kajikawa; P. Kunz; D. W. G. S. Leith; L. Levinson; T. Matsui; B. T. Meadows; A. Miyamoto; M. Nussbaum; H. Ozaki; C.O. Pak; B. N. Ratcliff; D. Schultz; S. Shapiro; T. Shimomura; P.K. Sinervo; A. Sugiyama; S. Suzuki; G. Tarnopolsky; T. Tauchi

Abstract The results of a partial wave analysis of the low mass KKπ system produced in the reactions K − p →K 0 s K ± π ± Λ at 11 GeV/ c using the LASS spectrometer are presented. Evidence is given for two ss axial-vector meson states: one with quantum numbers J PC = 1 ++ , mass ∼ 1530 MeV/ c 2 , and width ∼ 100 MeV/ c 2 , and the other with quantum numbers J PC =1 +− , mass ∼ 1380 MeV/ c 2 , and width ∼ 80 MeV/ c 2 . These states are good candidates to be the mostly strangeonium members of the ground state 1 ++ and 1 +− nonets predicted by the quark model.


Physics Letters B | 1995

Measurement of inclusive particle spectra and test of MLLA prediction in e+e− annihilation at s=58Gev

R. Itoh; M. Yamauchi; A. Yamaguchi; K. Abe; Tomohiro Abe; I. Adachi; K. Adachi; Masato Aoki; S. Awa; K. Emi; R. Enomoto; H. Fujii; K. Fujii; T. Fujii; J. Fujimoto; K. Fujita; N. Fujiwara; H. Hayashii; B. Howell; N. Iida; Y. Inoue; H. Iwasaki; M. Iwasaki; K. Kaneyuki; R. Kajikawa; S. Kato; S. Kawabata; H. Kichimi; M. Kobayashi; D. Koltick

Abstract Inclusive momentum spectra are measured for all charged particles and for each of π ± , K ± , K 0 K 0 , and p p in hadronic events produced via e + e − annihilation at s =58 Gev . The measured spectra are compared with QCD predictions based on the modified leading log approximation (MLLA). The MLLA model reproduces the measured spectra well. The energy dependence of the peak positions of the spectra is studied by comparing the measurements with those at other energies. The energy dependence is also well described by the MLLA model.


Physics Letters B | 1989

Search for SUSY Particles in e+ e- Annihilation at Tristan

I. Adachi; H. Aihara; H.B. Dijkstra; R. Enomoto; H. Fujii; K. Fujii; T. Fujii; J. Fujimoto; K. Fujiwara; N. Fujiwara; H. Hayashii; S. Higashi; B. Howell; N. Iida; A. Imanishi; H. Ikeda; T. Ishii; R. Itoh; H. Iwasaki; S. Iwata; R. Kajikawa; T. Kamae; S. Kato; S. Kawabata; Y. Kayahara; H. Kichimi; T. Kishida; M. Kobayashi; D. Koltick; Shigeru Kuroda

Abstract The TOPAZ detector has accumulated about 11 pb−1 of data in the energy range s =52−57 GeV . Charged supersymmetric particles have been searched for. Assuming the photino to be massless, we place limits on the chargino of m χ GeV , on the scalar muon, tau, and quark of m μ GeV , m τ GeV , and m q GeV . The scalar electron can be excluded up to a mass of ∼ 28 GeV. Other cases are examined.


Physics Letters B | 1994

Measurement of the D ± Cross Section using a Soft-Pion Analysis in Two-Photon Processes

R. Enomoto; K. Abe; Tomohiro Abe; I. Adachi; Masato Aoki; S. Awa; R. Belusevic; K. Emi; H. Fujii; K. Fujii; T. Fujii; J. Fujimoto; K. Fujita; N. Fujiwara; H. Hayashii; B. Howell; N. Iida; H. Ikeda; R. Itoh; H. Iwasaki; M. Iwasaki; R. Kajikawa; K. Kaneyuki; S. Kato; S. Kawabata; H. Kichimi; M. Kobayashi; D. Koltick; I. Levine; S. Minami

Abstract The differential cross section of dσ(e + e − → e + e − D ∗± X) dP T was measured using a soft-pion analysis D ∗± → π s ± D 0 (D 0 ) at TRISTAN. The average s was 58.7 GeV and the integrated luminosity used in this analysis was 198 pb − , respectively.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1985

A cathode readout gas sampling calorimeter with conductive plastic tubes

K. Fujii; J. Fujimoto; H. Hayashii; R. Kajikawa; Y. Masatani; H. Ozaki; A. Sugiyama; R. Suzaki; S. Suzuki; T.Y. Tsukamoto; T.F. Tsukamoto; S. Uno; S. Iwata

Abstract We constructed and tested a prototype gas sampling electromagnetic calorimeter of the Pb-proportional tube sandwich type. The calorimeter uses conductive plastic tubes and cathode pad readout with a tower structure which resulted in reasonable energy and spatial resolutions for electrons in the momentum range 0.5–4.0 GeV/c; σ E E = 21% (E( GeV ) ) 1 2 , σ x = 6 mm (at 3 GeV /c). This paper describes the test and the performance studied under various conditions.


Physics Letters B | 1994

Measurement of the photon structure function F2γ and jet production at TRISTAN

K. Muramatsu; H. Hayashii; S. Noguchi; N. Fujiwara; K. Abe; Tomohiro Abe; I. Adachi; Masato Aoki; S. Awa; R. Belusevic; K. Emi; R. Enomoto; H. Fujii; K. Fujii; T. Fujii; J. Fujimoto; K. Fujita; B. Howell; N. Iida; H. Ikeda; R. Itoh; H. Iwasaki; M. Iwasaki; R. Kajikawa; K. Kaneyuki; S. Kato; S. Kawabata; H. Kichimi; M. Kobayashi; D. Koltick

Abstract We have measured the photon structure function F2γ in the reaction e+e− → e+e− hadrons for average Q2 values from 5.1 to 338 GeV2 by using data collected by the TOPAZ detector at TRISTAN. The data have been corrected for detector effects and are compared with theoretical expectations based on QCD. The structure function F2γ increases as ln Q2, as expected. A sample of events with one or two distinct jets has been identified in the final state. Although two-jet events can be explained solely by the point-like perturbative part, one-jet events require a significant hadron-like part in addition.

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