TY - JOUR
T1 - Search for lepton flavor violation in the Higgs boson decay at a linear collider
AU - Kanemura, Shinya
AU - Matsuda, Koichi
AU - Ota, Toshihiko
AU - Shindou, Tetsuo
AU - Takasugi, Eiichi
AU - Tsumura, Koji
N1 - Funding Information:
The authors would like to thank Chikara Fukunaga, Masafumi Koike, Yoshitaka Kuno, Yasuhiro Okada, and Minoru Tanaka for valueable discussions. We also would like to thank Michael Peskin and Isamu Watanabe for useful suggestions and comments at the YITP Meeting on Phenomenology in June 2004. This work was supported, in part, by JSPS Research Fellowship for Young Scientists (Nos. 15-3693, -3700, -3927).
PY - 2004/10/7
Y1 - 2004/10/7
N2 - We discuss possibility of direct search for lepton flavor violation (LFV) in Yukawa interaction by measuring the branching ratio for the decay of the lightest Higgs boson (h 0) into a τ-μ pair at a linear collider (LC). We study the significance of the signal process, e +e -→Z*→Zh 0→Zτ ±μ ∓, against the backgrounds such as e +e -→Zτ +τ -→Zτ ±μ ∓+ missings. After taking appropriate kinematic cuts, the number of the background event is considerably reduced, so that the signal can be visible when the branching ratio of h 0→τ ±μ ∓ is larger than about 10 -4. In a minimal supersymmetric Standard Model scenario, the effective coupling of h 0τ ±μ ∓ can be generated at the loop level due to the slepton mixing. When supersymmetric mass parameters are larger than TeV scales, the branching ratio can be as large as several times 10 -4. Therefore, the signal can be marginally visible at a LC. In the general two-Higgs-doublet model, the possible maximal value for the branching ratio of h 0→τ ±μ ∓ can reach to a few times 10 -3 within the available experimental bound, so that we can obtain larger significance.
AB - We discuss possibility of direct search for lepton flavor violation (LFV) in Yukawa interaction by measuring the branching ratio for the decay of the lightest Higgs boson (h 0) into a τ-μ pair at a linear collider (LC). We study the significance of the signal process, e +e -→Z*→Zh 0→Zτ ±μ ∓, against the backgrounds such as e +e -→Zτ +τ -→Zτ ±μ ∓+ missings. After taking appropriate kinematic cuts, the number of the background event is considerably reduced, so that the signal can be visible when the branching ratio of h 0→τ ±μ ∓ is larger than about 10 -4. In a minimal supersymmetric Standard Model scenario, the effective coupling of h 0τ ±μ ∓ can be generated at the loop level due to the slepton mixing. When supersymmetric mass parameters are larger than TeV scales, the branching ratio can be as large as several times 10 -4. Therefore, the signal can be marginally visible at a LC. In the general two-Higgs-doublet model, the possible maximal value for the branching ratio of h 0→τ ±μ ∓ can reach to a few times 10 -3 within the available experimental bound, so that we can obtain larger significance.
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U2 - 10.1016/j.physletb.2004.08.024
DO - 10.1016/j.physletb.2004.08.024
M3 - Article
AN - SCOPUS:4444332041
SN - 0370-2693
VL - 599
SP - 83
EP - 91
JO - Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
JF - Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
IS - 1-2
ER -