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J. Pati (1998)
Implications of the superkamiokande result on the nature of new physicsarXiv: High Energy Physics - Phenomenology, 77
R. Gupta, Tanmoy Bhattacharya (1996)
Light quark masses and the CP violation parameterarXiv: High Energy Physics - Lattice, 53
D. Lewellen (1990)
Embedding higher-level Kac-Moody algebras in heterotic string models☆Nuclear Physics, 337
C. Albright, C. Albright, K. Babu, S. Barr (1998)
Minimality Condition and Atmospheric Neutrino OscillationsPhysical Review Letters, 81
K. Babu, J. Pati (1996)
The problems of unification-mismatch and low α3: A solution with light vector-like matterPhysics Letters B, 384
K. Dienes (1996)
String theory and the path to unification: A Review of recent developmentsPhysics Reports, 287
I. Antoniadis, G. Leontaris, J. Rizos (1990)
A three-generation SU(4)×O(4) string modelPhysics Letters B, 245
A. Faraggi, J. Pati (1997)
Meeting the Constraint of Neutrino-Higgsino Mixing in Gravity Unified TheoriesPhysics Letters B, 400
P. Langacker, N. Polonsky (1992)
Uncertainties in coupling constant unification.Physical review. D, Particles and fields, 47 9
M. Green, J. Schwarz (1984)
Anomaly cancellations in supersymmetric D=10 gauge theory and superstring theoryPhysics Letters B, 149
H. Georgi, C. Jarlskog (1979)
A new lepton-quark mass relation in a unified theoryPhysics Letters B, 86
F. Wilczek, Z. Zee (1977)
Discrete Flavor Symmetries and a Formula for the Cabibbo AnglePhysics Letters B, 70
E. Witten (1995)
String theory dynamics in various dimensionsNuclear Physics, 443
S. Weinberg (1979)
Baryon and Lepton Nonconserving ProcessesPhysical Review Letters, 43
S. Weinberg (1982)
Supersymmetry at ordinary energies. Masses and conservation lawsPhysical Review D, 26
J. Pati, A. Salam (1973)
Unified Lepton-Hadron Symmetry and a Gauge Theory of the Basic InteractionsPhysical Review D, 8
S. Mikheyev, A. Smirnov (1986)
Resonant amplification of ν oscillations in matter and solar-neutrino spectroscopyIl Nuovo Cimento C, 9
A. Kernan, B. Shen, E. Ma (1997)
High energy physics
V. Kuzmin, M. Shaposhnikov, V. Rubakov (1985)
On the Anomalous Electroweak Baryon Number Nonconservation in the Early UniversePhysics Letters B, 155
S. Dimopoulos, S. Raby, F. Wilczek (1982)
Proton decay in supersymmetric modelsPhysics Letters B, 112
J. Pati, A. Salam (1974)
Lepton Number as the Fourth ColorPhysical Review D, 10
H. Georgi, S. Glashow (1974)
Unity of All Elementary Particle ForcesPhysical Review Letters, 32
V. Barger, M. Berger, P. Ohmann (1992)
Supersymmetric grand unified theories: Two-loop evolution of gauge and Yukawa couplings.Physical review. D, Particles and fields, 47 3
P. Nath, A. Chamseddine, R. Arnowitt (1985)
Nucleon decay in supergravity unified theories.Physical review. D, Particles and fields, 32 9
J. Bahcall, P. Krastev, A. Smirnov (1998)
Where do we stand with solar neutrino oscillationsPhysical Review D, 58
K. Babu, S. Barr (1994)
Natural gauge hierarchy in SO(10).Physical review. D, Particles and fields, 50 5
P. Ginsparg (1987)
Gauge and Gravitational Couplings in Four-Dimensional String TheoriesPhysics Letters B, 197
H. Georgi, H. Quinn, S. Weinberg (1974)
Hierarchy of interactions in unified gauge theoriesPhysical Review Letters, 33
K. Babu, J. Pati, J. Pati, F. Wilczek (1997)
Suggested new modes in supersymmetric proton decayPhysics Letters B, 423
P. Langacker, Mingxing Luo (1991)
Implications of precision electroweak experiments for mt, rho 0, sin2 theta W, and grand unification.Physical review. D, Particles and fields, 44 3
F. Gürsey, P. Ramond, P. Sikivie (1976)
A Universal Gauge Theory Model Based on E6Physics Letters B, 60
Y. Golfand, E. Likhtman (1971)
EXTENSION OF THE ALGEBRA OF POINCARE GROUP GENERATORS AND VIOLATION OF P INVARIANCE.Jetp Letters, 13
J. Pati (1996)
The essential role of string-derived symmetries in ensuring proton-stability and light neutrino masses☆Physics Letters B, 388
J. Hisano, H. Murayama, T. Yanagida (1992)
Nucleon decay in the minimal supersymmetric SU(5) grand unificationNuclear Physics, 402
J. Pati, A. Salam (1973)
Is Baryon Number ConservedPhysical Review Letters, 31
K. Babu, S. Barr (1993)
Natural suppression of Higgsino-mediated proton decay in supersymmetric SO(10).Physical review. D, Particles and fields, 48 11
A. Faraggi (1992)
A New standard - like model in the four-dimensional free fermionic string formulationPhysics Letters B, 278
Y. Fukuda, T. Hayakawa, E. Ichihara, K. Inoue, K. Ishihara, H. Ishino, Y. Itow, T. Kajita, J. Kameda, S. Kasuga, Ken-ichiro Kobayashi, Y. Kobayashi, Y. Koshio, M. Miura, M. Nakahata, S. Nakayama, A. Okada, K. Okumura, N. Sakurai, M. Shiozawa, Y. Suzuki, Y. Takeuchi, Y. Totsuka, S. Yamada, M. Earl, A. Habig, E. Kearns, M. Messier, K. Scholberg, J. Stone, L. Sulak, C. Walter, M. Goldhaber, T. Barszczxak, D. Casper, W. Gajewski, P. Halverson, J. Hsu, W. Kropp, L. Price, F. Reines, M. Smy, H. Sobel, M. Vagins, K. Ganezer, W. Keig, R. Ellsworth, S. Tasaka, J. Flanagan, A. Kibayashi, J. Learned, S. Matsuno, V. Stenger, D. Takemori, T. Ishii, J. Kanzaki, Tomio Kobayashi, S. Mine, K. Nakamura, K. Nishikawa, Y. Oyama, A. Sakai, M. Sakuda, O. Sasaki, S. Echigo, M. Kohama, A. Suzuki, T. Haines, E. Blaufuss, B. Kim, R. Sanford, R. Svoboda, M. Chen, Z. Conner, J. Goodman, G. Sullivan, J. Hill, C. Jung, K. Martens, C. Mauger, C. Mcgrew, E. Sharkey, B. Viren, C. Yanagisawa, W. Doki, K. Miyano, H. Okazawa, C. Saji, M. Takahata, Y. Nagashima, M. Takita, Takashi Yamaguchi, M. Yoshida, S. Kim, M. Etoh, K. Fujita, A. Hasegawa, T. Hasegawa, S. Hatakeyama, T. Iwamoto, M. Koga, T. Maruyama, H. Ogawa, J. Shirai, A. Suzuki, F. Tsushima, M. Koshiba, M. Nemoto, K. Nishijima, T. Futagami, Y. Hayato, Y. Kanaya, K. Kaneyuki, Y. Watanabe, D. Kiełczewska, R. Doyle, J. George, A. Stachyra, L. Wai, R. Wilkes, K. Young (1998)
Evidence for oscillation of atmospheric neutrinosPhysical Review Letters, 81
H. Fritzsch (1977)
Calculating the Cabibbo anglePhysics Letters B, 70
[One major goal of this talk will be to stress that supersymmetric unification based on symmetries like SO(10) [15], or (for most purposes) a stringderived [6, 16] G(224) = SU(2)L × SU(2)R × SU(4)C, has implications not only for (i) gauge coupling unification and (ii) proton decay, but also for (iii) the masses and mixings of the charged fermions, as well as for (iv) those of the neutrinos. In fact, within a unified theory, all four features (i)–(iv) get intimately linked to each other, much more so than commonly thought. Each of these, including even charged fermion and neutrino-masses, provides some essential clue to the nature of higher unification. As regards the link between the four features, even neutrino masses turn out to have direct influence on proton decay. This is because the latter receives important contributions through a new set of d= 5 operators that depend directly on the Majorana masses of the right-handed neutrinos [17]. These new d= 5 operators, which were missed in the literature, contribute significantly to proton decay amplitudes, in addition of course to the “standard” d= 5 operators [11], which arise through the exchange of the color-triplet Higgsinos related to the electro-weak doublets. The standard and the new d= 5 operators, related to the charged fermion as well as the neutrino masses, together raise our expectation that proton decay should be observed in the near future [18].]
Published: Jan 1, 2008
Keywords: Yukawa Coupling; Minimal Supersymmetric Standard Model; Neutrino Masse; Gauge Coupling; Charged Lepton
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