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Dive into the research topics where S. Matsumoto is active.

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Featured researches published by S. Matsumoto.


European Physical Journal C | 1994

A novel approach to confront electroweak data and theory

Kaoru Hagiwara; D. Haidt; Christina Kim; S. Matsumoto

AbstractA novel approach to study electroweak physics at one-loop level in generic SU(2)L×U(1)Y theories is introduced. It separates the 1-loop corrections into two pieces: process specific ones from vertex and box contributions, and universal ones from contributions to the gauge boson propagators. The latter are parametrized in terms of four effective form factorsn


European Physical Journal C | 1998

Analysis of electroweak precision data and prospects for future improvements

Kaoru Hagiwara; Dieter Haidt; S. Matsumoto


Physical Review D | 1997

One loop supersymmetric QCD radiative corrections to top quark production in p{bar p} collisions

Sher Alam; K. Hagiwara; S. Matsumoto

bar e^2 (q^2 ), bar s^2 (q^2 ), bar g_Z^2 (q^2 )


Progress of Theoretical Physics Supplement | 1996

Electroweak Precision Measurements and the Minimal Supersymmetric Standard Model

Youichi Yamada; Kaoru Hagiwara; S. Matsumoto


Physical Review D | 1993

Consequences of a possible [gamma][gamma] resonance at KEK TRISTAN

Kaoru Hagiwara; S. Matsumoto; M. M. Tanaka

n andn


Physical Review D | 1993

Consequences of a possibleγγresonance at KEK TRISTAN

Kaoru Hagiwara; S. Matsumoto; M. M. Tanaka


Physical Review D | 1993

Consequences of a Possible Di-Gamma Resonace at TRISTAN

Kaoru Hagiwara; S. Matsumoto; M. M. Tanaka

bar g_W^2 (q^2 )


Physical Review D | 1993

Consequences of a possible γ γ resonance at KEK TRISTAN

Kaoru Hagiwara; S. Matsumoto; M. M. Tanaka


European Physical Journal C | 1998

Constraints on four-Fermi contact interactions from low-energy electroweak experiments

Gi-Chol Cho; Kaoru Hagiwara; S. Matsumoto

n corresponding to the γγ, γZ,ZZ andWW propagators. Under the assumption that only the Standard Model contributes to the process specific corrections, the magnitudes of the four form factors are determined atq2=0 and atq2=mZ2 by fitting to all available precision experiments. These values are then compared systematically with predictions of SU(2)L×U(1)Y theories. In all fits αs(mZ) andn


Physics Letters B | 2000

Erratum to: Constraints on non-standard contributions to the charged-current interactions

Kaoru Hagiwara; S. Matsumoto

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