Slide 1: Overview Slide 2: particle content of the MSSM Slide 3: listing of complex parameters in the MSSM; where can CPV effects occur? Slide 4: stop/sbottom sector of the MSSM incl. complex parameters Slide 5: not all phases are physical! Listing of possible physical combinations Slide 6: chargino/neutralino sector of the MSSM incl. complex parameters Slide 7: Higgs sector of the MSSM with real parameters Slide 8: Higgs sector of the MSSM with complex parameters Slide 9: No CPV in the Higgs sector at tree-level. How can we get rid of the phases? PQ-Transformation, A-Tadpole = 0. Slide 10: Generic SUSY contributions to EDMS => possibly too large! Slide 11: example for experimental restrictions on phases Slide 12: overview about the MSSM constraints on phases: where do they appear? Why can the effects be large Slide 13: CP-even Higgs sector at tree-level, mass formulas, mh < MZ Slide 14: how to evaluate higher-order corrections to the CP-even Higgs sector for masses and mixings Slide 15: listing of complex parameters in the MSSM; effects enter Higgs sector via loop corrections; CP-even and CP-odd fields mix => 3 neutral Higgs bosons mix; h1, h2, h3 with M_h1 < M_h2 < M_h3 Slide 16: how to evaluate higher-order corrections to the neutral Higgs sector (mixed CP-even and -odd) for masses and mixings Slide 17: M_h1 as a function of phi_At at the one-loop and two-loop level Slide 18: M_h1 as a function of phi_Mgluino at the two-loop level Slide 19: Higgs boson mixings: examples for external Higgs bosons; => important to ensure on-shell properties of the external Higgs bosons! Slide 20: Introduction of the Z-Matrix that ensures these on-shell properties Slide 21: Higgs boson mixings: examples for internal Higgs bosons; => important to ensure unitarity of the mixing matrix. Slide 22: two possibilities for a unitary mixing matrix: p^2 on-shell: U-Matrix p^2 = 0 : R-Matrix Slide 23: Limit p^2 -> 0 of the Z-Matrix yields the U-Matrix => important consistency check Slide 24: comparison of U- and R-Matrix: two checks proposed: 1) comparison with full calculation (Z-Matrix) 2) how well describe U and R pure CP-even or -odd states? Slide 25: example for test (2) => U-Higgs can be better However: U-Higgs has problems with decoupling properties Slide 26: comparison of Z-, U- and R-Higgs for external Higgs bosons => Z-Higgs = full result, U-Higgs closer, R-Higgs a bit more far away Slide 27: summary of the treatment of higher-order corrections for external and internal Higgs bosons Slide 28: CPV effects on Higgs searches: example of CPX scenario at LEP; comparison of various Higgs final states Slide 29: LEP results in the CPX scenario for two m_top values => unexcluded areas for low M_h1 values (CPX holes), e.g. at M_h1 = 45 and tan_beta = 8. Slide 30: new theoretical developments: - new two-loop corrections for masses and mixings incl. complex par. - new one-loop calculation for h2 -> h1 h1 decay Slide 31: re-evaluation of CPX holes using HiggsBounds => holes confirmed Slide 32: chapter 3: Higgs in decays - renormalization; repitition of slide 15. Slide 33: phases enter in tree-level couplings of Higgses to scalar fermions; existing analyses restricted to tree-level results; => full one-loop calculation needed. Slide 34: full one-loop calculation needed: overview about 2-body decay channels; => all sectors of the MSSM enter Slide 35: list of renormalizations included for the various sectors Slide 36: example of renormalization of complex parameters: At, theta_stop, Ab, theta_sbot, M1, M2, mu Slide 37: list of channels that have been evaluated; no numerical results yet. :-( Slide 38: conclusions Slide 39: back-up starts Slide 40: comparison of Z-, U- and R-Higgs as a function of phi_Xt Slide 41: example of effects of imaginary parts of Higgs self-energies Slide 42: comparison of U_33^2 and R_33^2