Higher dimensional seesaw Atsushi WATANABE Niigata Univ. & The Max-Planck-Institute for Nuclear Physics 23 rd February HRI, Allahabad Based on the.

Slides:



Advertisements
Similar presentations
Obtaining a nonzero  13 in lepton models based on SO(3)  A 4 Yuval Grossman and Wee Hao Ng, Cornell University Phenomenology 2014 arXiv: [hep-ph]
Advertisements

Neutrino physics using Nuclear Reactors J. Magnin Centro Brasileiro de Pesquisas Físicas Rio de Janeiro - Brazil.
Resonant Leptogenesis In S4 Model Nguyen Thanh Phong Cantho University In cooperation with Prof. CSKim, SKKang and Dr. YHAhn (work in progress)
Non-zero |U e3 | and Quark-Lepton in Discrete Symmetry Y.H.Ahn based on Phys.Rev.D83:076012,2011. working with Hai-Yang Cheng and S.C.Oh 년 8 월 17.
 Symmetries and vanishing couplings in string-derived low-energy effective field theory              Tatsuo Kobayashi 1.Introduction.
Phenomenological aspects of magnetized brane models Tatsuo Kobayashi
Morimitsu TANIMOTO Niigata University, Japan Prediction of U e3 and cosθ 23 from Discrete symmetry XXXXth RENCONTRES DE MORIOND March 6, La Thuile,
Quark and Lepton Mixing in S 4 Flavor Model September 28, 2010 Max-Planck-Institut für Kernphysik Heidelberg, Germany Morimitsu Tanimoto (Niigata University)
TeV scale see-saws from higher than d=5 effective operators Neutrino masses and Lepton flavor violation at the LHC Würzburg, Germany November 25, 2009.
A two-loop calculation in quantum field theory on orbifolds Nobuhiro Uekusa.
The classically conformal B-L extended standard model Yuta Orikasa Satoshi Iso(KEK,SOKENDAI) Nobuchika Okada(University of Alabama) Phys.Lett.B676(2009)81.
Twisted Flavors and Tri-bimaximal Neutrino Mixing Atsushi Watanabe (Kyushu U. ) with Koichi Yoshioka (Kyushu U.), Naoyuki Haba (Tokushima U. & Munich,
Higgs Quadruplet for Type III Seesaw and Implications for → e and −e Conversion Ren Bo Coauther : Koji Tsumura, Xiao - Gang He arXiv:
Hadronic EDMs in SUSY GUTs
June 18, 2004Mitsuru Kakizaki1 Democratic (s)fermions and lepton flavor violation Mitsuru Kakizaki (ICRR, University of Tokyo) June 18, 2004 We propose.
May 25, 2004Kakizaki, Mitsuru1 Flavor structure in supersymmetric models Kakizaki, Mitsuru (ICRR, University of Tokyo) May 25, 2004 We proposed a new alignment.
Oct. 25, 2004Mitsuru Kakizaki1 Flavor structure in supersymmetric models Mitsuru Kakizaki (ICRR, University of Tokyo) Oct. 25, Ochanomizu University.
Introduction to universal extra dimensions (UEDs) Mitsuru Kakizaki (ICRR, University of Tokyo) May 10, KEK Refs: Original idea: Appelquist, Cheng,
July 19, 2005Mitsuru Kakizaki1 Hadronic EDMs in SUSY GUTs Mitsuru Kakizaki (ICRR, Univ. of Tokyo) July 19, IPPP We investigate hadronic EDMs induced.
Models of Neutrino Mass G.G.Ross, IPPP December 2005 Origin of mass and mass hierarchy What do we learn from the mixing angles?
Aug 29-31, 2005M. Jezabek1 Generation of Quark and Lepton Masses in the Standard Model International WE Heraeus Summer School on Flavour Physics and CP.
Fermion Masses G.G.Ross, Corfu, September 2005 The Standard Model.
Basics of Physics in Extra Dimensions. Motivation for extra dimensions Hierarchy problem –Vast expanse between the scales of weak interactions and gravitational.
Introduction to Gauge Higgs unification with a graded Lie algebra Academia Sinica, Taiwan Jubin Park (NTHU)  Collaboration with Prof. We-Fu.
 Collaboration with Prof. Sin Kyu Kang and Prof. We-Fu Chang arXiv: [hep-ph] submitted to JHEP.
Texture of Yukawa coupling matrices in general two-Higgs doublet model Yu-Feng Zhou J. Phys. G: Nucl. Part. Phys.30 (2004) Presented by Ardy.
Generalized solution for metric in Randall-Sundrum scenario Alexander Kisselev IHEP, NRC “Kurchatov Institute”, Protvino, Russia The XIII-th International.
Extra Dimensions (XD) Xiaozhou zhou 9/25/2007. Outline  What does extra dimension mean?  Why extra dimensions?  Why can’t we see extra dimensions?
1 Rare Processes as Windows onto Extra Dimensions Gela Devidze High Energy Physics Institute, Tbilisi State University Content 1. Introduction Charged.
Generalized solution for RS metric and LHC phenomenology Alexander Kisselev IHEP, NRC “Kurchatov Institute”, Protvino, Russia The Third Annual Conference.
Large extra dimensions and CAST Biljana Lakić Rudjer Bošković Institute, Zagreb Joint ILIAS-CAST-CERN Axion Training, , CERN Joint ILIAS-CAST-CERN.
A viable RS Model for Quarks and Leptons with T´ Flavor Symmetry Felix Yu University of California, Irvine Pheno 2010 M-C. Chen, K. T. Mahanthappa, FY.
Duality in Left-Right Symmetric Seesaw Mechanism Michele Frigerio Service de Physique Théorique, CEA/Saclay Rencontres de Physique des Particules March.
March 7, 2005Benasque Neutrinos Theory Neutrinos Theory Carlos Pena Garay IAS, Princeton ~
Takaaki Nomura(Saitama univ)
Nobuchika Okada The University of Alabama Miami 2015, Fort Lauderdale, Dec , GeV Higgs Boson mass from 5D gauge-Higgs unification In collaboration.
Tree-level unitarity in Gauge-Higgs Unification Yutaka Sakamura (KEK) with Naoyuki Haba (Osaka Univ.) and Toshifumi Yamashita (Nagoya Univ.) January 20,
SUSY GUT Predictions for Neutrino Oscillation Mu-Chun Chen Brookhaven National Laboratory DUSEL Workshop, January 4-7, 2005 University of Colorado at Boulder.
Renormalization of the Higgs Triplet Model Mariko Kikuchi ( Univ. of Toyama ) Collaborators M. Aoki ( Kanazawa Univ. ), S. Kanemura ( Univ. of Toyama ),
03/31/2006S. M. Lietti - UED Search at SPRACE 1 Universal Extra Dimensions Search at SPRACE S. M. Lietti DOSAR Workshop at U.T. Arlington.
Z’ Signals from KK Dark Matter Sabine Riemann (DESY) LCWS, Stanford, March 18-22, 2005 Outline  Universal extra dimensions (UED)  KK dark matter?  Sensitivity.
Collider Signals of Extra Dimension Scenarios
THE CONNECTION BETWEEN NEUTRINO EXPERIMENTS AND LEPTOGENESIS Alicia Broncano Berrocal MPI.
Tree-level unitarity in Gauge-Higgs Unification Yutaka Sakamura (RIKEN) with Naoyuki Haba (Osaka Univ.) and Toshifumi Yamashita (Nagoya Univ.) December.
1-2 Mass Degeneration in the Leptonic Sector Hiroyuki ISHIDA (Tohoku University) Collaboration with : Takeshi ARAKI (MISC) Ref ; T. Araki and H.I. arXiv.
Carla Biggio Universidad Autónoma de Madrid Neutrino masses and new TeV scale HEP 2007, Manchester, England, 19-25/07/07 Based on: Antusch, CB,
and what we unsuccessfully tried to explain (so far)
Charged Higgs boson decay in supersymmetric TeV scale seesaw model
Modeles Theoriques Andrea Romanino CERN.
Universal Extra Dimension models with right-handed neutrinos
Takaaki Nomura(Saitama univ)
Non-unitary deviation from the tri-bimaximal mixing and neutrino oscillations Shu Luo The Summer Topical Seminar on Frontier of Particle Physics.
Neutrinos in the Standard Model and Beyond
Classically conformal B-L extended Standard Model
Magnetic supersymmetry breaking
Hadronic EDMs in SUSY GUTs
Lepton Flavor Violation
Exploring SUSY breaking mechanism with B decays
Brane world in f(T) gravity Fo-Guang-Shan, Kaohsiung, Taiwan
Quark and lepton masses
Yasuhiro Okada (KEK/Sokendai) October 18, 2007
Yasuhiro Okada (KEK) FPCP 2004, Deagu, Korea October 7, 2004
Introduction to universal extra dimensions (UEDs)
Searching for New Physics in muon lepton flavor violating processes
Lepton Flavor Violation
Collider Signals of Large Extra Dimension
High Energy Physics On the Fukugita-Tanimoto-Yanagida Ansatz with Partially Non-degenerate Right-handed Majorana Neutrinos 29 October,
Kaluza-Klein states and the geography of extra dimensions
Presentation transcript:

Higher dimensional seesaw Atsushi WATANABE Niigata Univ. & The Max-Planck-Institute for Nuclear Physics 23 rd February HRI, Allahabad Based on the work with K. Yoshioka (Kyoto Univ.), H. Ishimori, Y. Shimizu, M. Tanimoto (Niigata Univ.)

Contents The interplay between neutrino physics and the extra dimensions The bulk right-handed neutrinos KK expansion and the propagator Flavor symmetry breaking on orbifolds

The bulk right-handed neutrinos SM gravity right-handed neutrinos [Dienes,Dudas,Gherghetta,1999] [Arkani-Hamed,Dimopoulos,Dvali,March-Russell,1999] Standard Model + Dirac Yukawa An interesting range of the neutrino mass shows up Suppressed Dirac mass Neutrino mass

Localizationof the wave function Localization of the wave function [Grossman, Neubert, 99] (SM) Dirac (kink) mass in the S1/Z2 bulkZero mode function [Chang, Hisano, Nakano, Okada, Yamaguchi, 99]

Seesaw in five dimensions [Dienes,Dudas,Gherghetta,99] [Lukas, Ramond, Romanino, Ross, 00] Neutrino mass after the seesaw

Options available in 5D ■ The mass terms (Majorana, Dirac, Lorentz-violating …) ■ The bulk geometry (Flat, Warped, Others …) ■ The boundary conditions for the bulk fields

Seesaw with the bulk Dirac mass [AW, Yoshioka, 2009] for eV neutrino mass Bulk Dirac The neutrino mass becomes

Inverse seesaw small The zero mode function Zero mode is negligible in seesaw Whole neutrino mass matrix

On the warped geometry Randall-Sumdrum background Planck (y=0)TeV (y=L) How does the background change the neutrino mass ?

By the usual KK expansion, … It is hard to perform seesaw diagonalization

The equations for the bulk propagator the warped effect is vanishing away at the low-energy limit Alternative to the KK expansion ⇒ 5D propagator

The result is ・ The neutrino mass is not much affected by the background ・ The result is the same for more general metric ・ The seesaw mass can be calculated without knowing the KK expansion Even with a complicated backgroud where a suitable KK expansion cannot be find, the seesaw neutrino mass is calculable.

Flavor symmetry breaking at the boundaries S 4 group Irreducible representations: Exmaple of the triplet S 4 breaking boundary conditions elements of the S4 group

Lagrangian of neutrino sector 4D Lagrangian is obtained by

Example I: KK expansionMajorana mass matrix after the seesaw ・ only one mixing angle ・ degenerate masses

Example II: The result is

3 effective parameters: Deviation from the tri-bimaximal mixing

Summary We have explored ``bulk seesaw” ・ Inverse seesaw (bulk Dirac mass) ・ Geometry free nature of the neutrino mass ・ Flavor symmetry breaking at the boundaries

Charged-lepton sector For Example ⇒ small mixing for the left-handed direction