“…Before discussing orbifold compactifications of the heterotic string, let us demonstrate how the previous problems are solved in a bottom-up approach with two extra dimensions 6 . For simplicity, we construct the previously described Pati-Salam times U(1) X model in four dimensions.…”
Section: Proton Hexality and Local Grand Unificationmentioning
confidence: 99%
“…5 Note that in the case of matter parity as a subgroup of SO(10) we would need a 126-dimensional representation to get the desired symmetry breakdown. 6 In the spirit of [14] this may correspond to a compactification of the heterotic string on T 6 /Z M × Z N , where our T 2 appears as a fixed torus under the Z N factor. For a list of possible Z M × Z N orbifolds see e.g.…”
Section: Proton Hexality and Local Grand Unificationmentioning
confidence: 99%
“…Anomaly cancellation restricts the spectrum of a gauge theory leading to a finite number of possible discrete symmetries, which can be obtained in such a way. The authors of [6] looked through all such symmetries and identified proton hexality, P 6 , as the only other phenomenologically interesting discrete symmetry. On SM fields P 6 , as defined by the charge assignments in Table 1, acts as a Z 6 symmetry which is the product of baryon triality and matter parity.…”
Section: Proton Hexalitymentioning
confidence: 99%
“…Interactions including right-handed neutrinos do not introduce baryon number violating terms, since their B 3 charge is zero. All terms needed for the see-saw mechanism are allowed by P 6 [6].…”
Section: Proton Hexalitymentioning
confidence: 99%
“…The situation becomes much more dramatic for the remaining fields: (4, 1, 2) 7 , (4, 1, 2) −7 and the fields in eqn. (6). These are embedded in SO (12) representations containing weights of the form (±7/2, .…”
Proton hexality is a discrete symmetry that avoids the problem of too fast proton decay in the supersymmetric extension of the standard model. Unfortunately it is inconsistent with conventional grand unification. We show that proton hexality can be incorporated in the scheme of "Local Grand Unification" discussed in the framework of model building in (heterotic) string theory.
“…Before discussing orbifold compactifications of the heterotic string, let us demonstrate how the previous problems are solved in a bottom-up approach with two extra dimensions 6 . For simplicity, we construct the previously described Pati-Salam times U(1) X model in four dimensions.…”
Section: Proton Hexality and Local Grand Unificationmentioning
confidence: 99%
“…5 Note that in the case of matter parity as a subgroup of SO(10) we would need a 126-dimensional representation to get the desired symmetry breakdown. 6 In the spirit of [14] this may correspond to a compactification of the heterotic string on T 6 /Z M × Z N , where our T 2 appears as a fixed torus under the Z N factor. For a list of possible Z M × Z N orbifolds see e.g.…”
Section: Proton Hexality and Local Grand Unificationmentioning
confidence: 99%
“…Anomaly cancellation restricts the spectrum of a gauge theory leading to a finite number of possible discrete symmetries, which can be obtained in such a way. The authors of [6] looked through all such symmetries and identified proton hexality, P 6 , as the only other phenomenologically interesting discrete symmetry. On SM fields P 6 , as defined by the charge assignments in Table 1, acts as a Z 6 symmetry which is the product of baryon triality and matter parity.…”
Section: Proton Hexalitymentioning
confidence: 99%
“…Interactions including right-handed neutrinos do not introduce baryon number violating terms, since their B 3 charge is zero. All terms needed for the see-saw mechanism are allowed by P 6 [6].…”
Section: Proton Hexalitymentioning
confidence: 99%
“…The situation becomes much more dramatic for the remaining fields: (4, 1, 2) 7 , (4, 1, 2) −7 and the fields in eqn. (6). These are embedded in SO (12) representations containing weights of the form (±7/2, .…”
Proton hexality is a discrete symmetry that avoids the problem of too fast proton decay in the supersymmetric extension of the standard model. Unfortunately it is inconsistent with conventional grand unification. We show that proton hexality can be incorporated in the scheme of "Local Grand Unification" discussed in the framework of model building in (heterotic) string theory.
Proton hexality is a discrete symmetry ensuring the stability of the proton under dimension four and five interactions. We discuss the embedding of proton hexality into Grand Unified Theories. This leads naturally to the concept of extra dimensions and string theory. This talk is based on a collaboration with results to be published shortly [1].
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