Solution to the Strong CP Problem: Supersymmetry with Parity
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There is a natural solution to the strong CP problem in the Minimal Supersymmetric Standard Model if it arises from a parity symmetric theory which is spontaneously broken to MSSM at Planck, GUT or intermediate scales. The strong CP phase is zero at the tree level and is not induced to two loops. The SUSY phase problems are also solved. The universal soft SUSY breaking parameters A, B, \mu, m_{1/2} are all automatically real and the only additional CP violation effects of the low-energy MSSM are characterized by a Hermitian squark mass matrix whose phases depend on the CKM phase. Cases with non-universal boundary conditions are also considered.
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Lepton number violating signals of a parity symmetric model at $\mu$TRISTAN
In a parity-symmetric model with TeV-scale lepton number violation, a 10 TeV μ+μ+ collider can probe W' boson masses up to 16 TeV via on-shell and off-shell lepton number violating production.
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