Constraints on the new particle in Σ → p μμ

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Constraints on the new part icle in Σ→ pμμ Yu-Kuo Hsiao With the collaborator C.Q. Geng National Tsing-Huang University, Taiwan Based on ph/0509175, to appear in PLB. Experiment Constraints from other modes Summary Comparison

description

Constraints on the new particle in Σ → p μμ. Yu-Kuo Hsiao With the collaborator C.Q. Geng National Tsing-Huang University, Taiwan Based on ph/0509175, to appear in PLB. Experiment Constraints from other modes Summary Comparison. New particles with different masses?. - PowerPoint PPT Presentation

Transcript of Constraints on the new particle in Σ → p μμ

Page 1: Constraints on the new particle in  Σ → p μμ

Constraints on the new particle in Σ→ pμμ

Yu-Kuo HsiaoWith the collaborator C.Q. Geng

National Tsing-Huang University, TaiwanBased on ph/0509175, to appear in PLB.

• Experiment• Constraints from other modes• Summary• Comparison

Page 2: Constraints on the new particle in  Σ → p μμ

New particles with different masses?

Dark matter particle with mass of (ph/0508572)

Axion-like particle with mass of 0.7 meV-2 meV from PVLAS Collaboration. (ex/0507107)

A light scalar boson of mass 1-10 MeV, accounting for the fluxes of 511 keV gamma ray.(PLB 624, 162)

Intermediate boson with mass of 214.3 MeV from HyperCP Collaboration. (PRL94, 021801)

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ExperimentExperiment

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The effective Hamiltonian

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The Amplitude

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The form factors

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The Form FactorsThe Form Factors

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Constraints from K→ Constraints from K→ ππμμμμ

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ConstraintsConstraints from KL→ from KL→μμμμ

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Constraints from KL→μμ

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The models?

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The models?

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Comparison

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Summary