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Cosmological Constraint on the Minimal Universal Extra Dimension Model

Cosmological Constraint on the Minimal Universal Extra Dimension Model. Mitsuru Kakizaki (Bonn Univ. & ICRR, Univ. of Tokyo). 28 September, 2006 @ DESY. In collaboration with Shigeki Matsumoto (KEK) Yoshio Sato (Saitama Univ.) Masato Senami (ICRR, Univ. of Tokyo). Refs:

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Cosmological Constraint on the Minimal Universal Extra Dimension Model

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  1. Cosmological Constraint on the Minimal Universal Extra Dimension Model Mitsuru Kakizaki (Bonn Univ. & ICRR, Univ. of Tokyo) 28 September, 2006 @ DESY In collaboration with • Shigeki Matsumoto (KEK) • Yoshio Sato (Saitama Univ.) • Masato Senami (ICRR, Univ. of Tokyo) Refs: • PRD 71 (2005) 123522 [hep-ph/0502059] • NPB 735 (2006) 84 [hep-ph/0508283] • PRD 74 (2006) 023504 [hep-ph/0605280]

  2. 1. Motivation • Observations of • cosmic microwave background • structure of the universe • etc. [http://map.gsfc.nasa.gov] Non-baryonic cold dark matter • Weakly interacting massive particles (WIMPs) Correct relic abundance of CDM • Neutralino (LSP) in supersymmetric (SUSY) models • 1st KK mode of the B boson (LKP) in universal extra dimension (UED) models • etc. Today’s topic Mitsuru Kakizaki

  3. Outline This work • Reevaluation of the relic density of LKPs including both coannihilation and resonance effects Cosmological constraint on the minimal UED model c.f.: SUSY Motivation Universal extra dimension (UED) models Relic abundance of KK dark matter Coannihilation processes Resonance processes Summary [From Ellis, Olive, Santoso,Spanos, PLB565 (2003) 176] Mitsuru Kakizaki

  4. 2. Universal extra dimension (UED) models Macroscopic Idea: All SM particles propagate in flat compact spatial extra dimensions Magnify Microscopic [Appelquist, Cheng, Dobrescu, PRD64 (2001) 035002] • Dispersion relation: Momentum along the extra dimension = Mass in four-dimensional viewpoint Mass spectrum for • compactification with radius : KK tower is quantized • Momentum conservation in the extra dimension Conservation of KK number at each vertex Mitsuru Kakizaki

  5. Minimal UED (MUED) model • In order to obtain chiral zero-mode fermions, the extra dimension is compactified on an orbifold • Conservation of KK parity [+ (--) for even (odd) ] The lightest KK particle (LKP) is stable c.f. R-parity and LSP More fundamentaltheory The LKP is a good candidate for dark matter • Only two new parameters appear in the MUED model: : Scale at which boundary terms vanish : Size of extra dimension The Higgs mass remains a free parameter • Constraints coming from electroweak measurements are weak [Appelquist, Cheng, Dobrescu PRD64 (2001); Appelquist, Yee, PRD67 (2003);Gogoladze, Macesanu, hep-ph/0605207] for for Mitsuru Kakizaki

  6. Mass spectra of KK states 1-loop corrected mass spectrum at the first KK level • KK particles are degenerate in mass at tree level: • Compactification  5D Lor. inv. Orbifolding  Trans. Inv. in 5th dim. Radiative corrections relax the degeneracy • Lightest KK Particle (LKP): Degenerate in mass (mixture of ) • KK particles of leptons and Higgs bosons are highly degenerate with the LKP [From Cheng, Matchev, Schmaltz, PRD66 (2002) 036005] • Coannihilation plays an important rolein calculating the relic density Mitsuru Kakizaki

  7. Co-moving number density Decoupling 3. Relic abundance of KK dark matter Increasing Thermal equilibrium • Generic picture • Dark matter particles were in thermal equilibrium in the early universe • After the annihilation rate dropped below the expansion rate, the number density per comoving volume is almost fixed • Relic abundance of the LKP [Servant, Tait, NPB 650 (2003) 391] 3 flavors Without coannihilation Including coannihilation • Coannihilation only with the NLKP • No resonance process Mitsuru Kakizaki

  8. 4. Coannihilaition processes • Previous calculation: Relic abundance of the LKP • Inclusion of coannihilation modes with all 1st KK particles reduces the effective cross section Disfavored byEWPT [Burnell, Kribs, PRD73(2006); Kong, Matchev, JHEP0601(2006)] • The Higgs mass is fixed to • No resonance process is considered Without coannihilation WMAP • We emphasize: • The relic abundance depends on the SM Higgs mass • Resonance effects also shift the allowed mass scale [From Kong, Matchev, JHEP0601(2006)] Mitsuru Kakizaki

  9. Masses of the KK Higgs bosons Contour plot of mass splitting • 1st KK Higgs boson masses: -0.5 % [Cheng, Matchev, Schmaltz, PRD66 (2002) 036005] • Larger Larger ; smaller (Enhancement of the annihilation cross sections for the KK Higgs bosons) • Too large The 1st KK charged Higgs boson is the LKP Mitsuru Kakizaki

  10. New Allowed region without resonance processes • We investigate dependence of the LKP relic abundance on the Higgs mass, including all coannihilation modes with 1st KK particles • Bulk region (small ) The result is consistent with previous works KK Higgs coannihilation region • KK Higgs coannihilation region Bulk region (large ) The relic abundance decreasesthrough the Higgs coannihilation Larger is allowed Mitsuru Kakizaki

  11. 5. Resonance processes • KK particles are non-relativistic when they decouple (Incident energy of two 1st KK particles) (Masses of 2nd KK particles) Annihilation cross sections are enhanced through s-channel 2nd KK particle exchange at loop level • Important processes: c.f. Mitsuru Kakizaki

  12. New Allowed region including coannihilation and resonance • Cosmologically allowed region is shifted upward by • Bulk region: -res. are effective Without resonance • KK Higgs coannihilation region: -res. contributes as large as -res. • For the LKP may be the KK graviton ‘KK graviton problem’ • Some mechanism to make the KK graviton heavy is proposed Including resonance [Dienes PLB633 (2006)] Mitsuru Kakizaki

  13. 6. Summary • UED models contain a candidate particle for CDM: The 1st KK mode of the B boson (LKP) • In UED models • Coannihilation should be included • Resonance • We calculated the LKP relic abundance in the MUED model including the resonance processes in all coannhilation modes • Cosmologically allowed region in the MUED model Mitsuru Kakizaki

  14. Backup slides Mitsuru Kakizaki

  15. Calculation of the LKP abundance • The 1st KK particle of the B boson is assumed to be the LKP • The LKP relic abundance is dependent on effective annihilation cross section • Naïve calculation without coannihilation nor resonance WMAP data [Servant, Tait, NPB650 (2003) 391] • Coannihilation • Resonance Coannihilation with KK right-handed leptons ; [Servant, Tait, NPB650 (2003) 391] Coannihilation with all 1st KK particles [MK, Matsumoto, Sato, Senami, PRD71 (2005) 123522; NPB735 (2006) 84; PRD74 (2006) 023504] [Burnell, Kribs, PRD73(2006); Kong, Matchev, JHEP0601(2006)] ; Coannihilation with KK Higgs bosons for large [Matsumoto, Senami, PLB633 (2006)] ; Mitsuru Kakizaki

  16. Constraint on in the MUED model • Constraints coming from electroweak measurements are weak [Appelquist, Cheng, Dobrescu PRD64 (2001); Appelquist, Yee, PRD67 (2003);Gogoladze, Macesanu, hep-ph/0605207] Allowed • Requiring that LKPs account for the CDM abundance in Universe, the parameter space gets more constrained Excluded (Under the assumption of thermal production) [From Gogoladze, Macesanu, hep-ph/0605207] Mitsuru Kakizaki

  17. Relic abundance of the LKP (without coannihilation) • The --resonance in annihilation effectively reduces the number density of dark matter • The resonance effect shifts upwards the LKP mass consistent with the WMAP data Mitsuru Kakizaki

  18. KK Higgs coannihilation region [Matsumoto, Senami, PLB633 (2006)] Dependence of the LKP relic abundance on the Higgs mass (ignoring resonance effects) • Larger Higgs mass (larger Higgs self--coupling) • Mass degeneracy between 1st KK Higgs bosons and the LKP in MUED WMAP • Larger annihilation cross sections for the 1st KK Higgs bosons Coannihilation effect with 1st KK Higgs bosons efficiently decrease the LKP abundance • of 1 TeV is compatible with the observation of the abundance Mitsuru Kakizaki

  19. KK Higgs coannihilation region Freeze-out • For larger (larger Higgs self-coupling) • Degeneracy between the LKP and • Free from a Boltzmann suppression Larger [Matsumoto, Senami, PLB633 (2006)] • The effective cross section can increase after freeze-out The LKP abundance can sizably decrease even after freeze-out Mitsuru Kakizaki

  20. New Inclusion of resonance processes • Cosmologically allowed region is shifted upward by • For the LKP may be the KK graviton Without resonance ‘KK graviton problem’ like the gravitino problem • Some mechanism to make the KK graviton heavy is proposed [Dienes PLB633 (2006)] Including resonance Mitsuru Kakizaki

  21. Origin of the shift • Bulk region -res. are effective res. Without resonance • KK Higgs co- annihilation region -res. contributes as large as -res. Including resonance Mitsuru Kakizaki

  22. Positron experiments • The HEAT experiment indicated an excess in the positron flux: • Unnatural dark matter substructure is required to match the HEAT data in SUSY models [Hooper, Taylor, Silk, PRD69 (2004)] • KK dark matter may explain the excess [Hooper, Kribs, PRD70 (2004)] • Future experiments (PAMELA, AMS-02, …) will confirm or exclude the positron excess Mitsuru Kakizaki

  23. Including coannihilation with 1st KK singlet leptons • The LKP is nearly degenerate with the 2nd KK singlet leptons Coannihilation effect is important • Annihilation cross sections The allowed LKP mass region is lowered due to the coannihilation effect c.f. SUSY models: coannihilation effect raises the allowed LSP mass Mitsuru Kakizaki

  24. 4. Coannihilaition processes • KK particles of leptons and Higgs bosons are highly degenerate with the LKP Coannihilation plays an important rolein calculating the relic density • In generic: e.g.: coannihilation with KK leptons: e.g.: coannihilation with KK Higgs bosons: Mitsuru Kakizaki

  25. 4. Coannihilaition processes • KK particles of leptons and Higgs bosons are highly degenerate with the LKP: • Coannihilation plays an important role in calculating the relic density • In generic: e.g.: coannihilation with KK leptons: e.g.: coannihilation with KK Higgs bosons: Mitsuru Kakizaki

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