2001
DOI: 10.1016/s0370-2693(01)00699-2
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Nonanomalous R-symmetry in supersymmetric unified theories of quarks and leptons

Abstract: A discrete R-symmetry often appears as an exact gauge symmetry in the low energy effective theory of superstring theories. We search for such discrete Rsymmetries from a phenomenological point of view and find that Z 9R and Z 18R are candidates of the nonanomalous R-symmetry in the case of the minimal supersymmetric standard model. We also find Z 4R and Z 20R in the case that quarks and leptons are embedded in the SU(5) GUT multiplets. Interesting is that in the latter case all the solutions predict some extra… Show more

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Cited by 80 publications
(98 citation statements)
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References 26 publications
(37 reference statements)
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“…Such a matter field is actually introduced by e.g. models which do not have quantum anomaly in R-symmetry [21,22]. The matter field gives the contributions in two ways [16,18].…”
Section: Gaugino Masses From a Vector-like Matter Fieldmentioning
confidence: 99%
“…Such a matter field is actually introduced by e.g. models which do not have quantum anomaly in R-symmetry [21,22]. The matter field gives the contributions in two ways [16,18].…”
Section: Gaugino Masses From a Vector-like Matter Fieldmentioning
confidence: 99%
“…the MSSM superpotential (supplemented by heavy neutrino Majorana mass terms in accord with the seesaw mechanism [48]), this condition then necessitates that [47] (see also [34,49])…”
Section: Unique Discrete R Symmetry For Pure Gravity Mediationmentioning
confidence: 99%
“…If their masses are comparable, because they have the structure of a complete SU(5) multiplet, they will not spoil (and can even improve) gauge coupling unification. 4 If at high energies the R symmetry was anomaly-free with respect to the SM nonabelian gauge groups, the low-energy theory will be anomalous. In the same way, if the high energy anomalies with respect to SU(3) and SU(2) were universal, they will no longer be in the low energy theory, as fields with different R charges coupling to the different gauge groups have been integrated out.…”
Section: Jhep01(2014)011mentioning
confidence: 99%
“…We conclude this section by discussing unification in more detail: it has been argued that non-universal axion couplings in the low-energy spoils gauge coupling unification, 4 Unification of coupling, with different R charges for such fields, might arise, for example, in the sort of direct product representations discussed in [11], or in string theory models [7]. 5 In the model presented above, we almost always have mq < m ; this is because for most of our parameter space, S2 > S1; then, the field coupling to S2 will in general be heavier.…”
Section: Jhep01(2014)011mentioning
confidence: 99%
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