Realization of a spontaneous gauge and supersymmetry breaking vacuum

Kobayashi, Tatsuo; Omura, Yuji; Seto, Osamu; Ueda, Keishi

doi:10.1007/jhep11(2017)073

Cited by 8 publications

(5 citation statements)

References 44 publications

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“…This feature was pointed out in the Z 3 invariant NMSSM [104]. The NUGM scenario is realized in GUT models [105][106][107][108][109][110][111][112] as well as the so-called mirage mediation [113][114][115][116][117][118]. The phenomenology of the mirage mediation in the NMSSM is discussed in Refs.…”

Section: Neutralino Mass and Dark Matter Physicsmentioning

confidence: 94%

A low-scale flavon model with a ℤN symmetry

Higaki

Kawamura

2020

J. High Energ. Phys.

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We propose a model that explains the fermion mass hierarchy by the Froggatt-Nielsen mechanism with a discrete Z F N symmetry. As a concrete model, we study a supersymmetric model with a single flavon coupled to the minimal supersymmetric Standard Model. Flavon develops a TeV scale vacuum expectation value for realizing flavor hierarchy, an appropriate µ-term and the electroweak scale, hence the model has a low cutoff scale. We demonstrate how the flavon is successfully stabilized together with the Higgs bosons in the model. The discrete flavor symmetry Z F N controls not only the Standard Model fermion masses, but also the Higgs potential and a mass of the Higgsino which is a good candidate for dark matter. The hierarchy in the Higgs-flavon sector is determined in order to make the model anomaly-free and realize a stable electroweak vacuum. We show that this model can explain the fermion mass hierarchy, realistic Higgs-flavon potential and thermally produced dark matter at the same time. We discuss flavor violating processes induced by the light flavon which would be detected in future experiments. N sym-1 Recently, it is proposed that a flavon can be identified as the QCD axion [3-8] 2 See, e.g., Refs. [35,36] for recent models with a flavor modular symmetry and also for such interactions in string models.3 Models with a combination of Higgs doublets H u H d as a flavon are studied in Refs. [41][42][43].

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Section: Neutralino Mass and Dark Matter Physicsmentioning

confidence: 94%

A low-scale flavon model with a ℤN symmetry

Higaki

Kawamura

2020

J. High Energ. Phys.

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“…It is hoped that these results will be of direct use to those currently working on grand unified theories [12][13][14][15][16][17][18][19], extra dimensions [20][21][22][23][24], and non-commutative geometry [25][26][27][28][29]. Furthermore, it may lend helpful clues to those working in related fields such as supersymmetry [30][31][32][33][34][35][36], and other topics closely related to the division algebras [37][38][39][40]. Finally, the possibility of an extra B−L symmetry mentioned here is particularly exciting given the recent findings of [41][42][43][44].…”

Section: Introductionmentioning

confidence: 98%

$$SU(3)_C\times SU(2)_L\times U(1)_Y\left( \times U(1)_X \right) $$ S U ( 3 ) C × S U

Furey

2018

Eur. Phys. J. C

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We demonstrate a model which captures certain attractive features of SU (5) theory, while providing a possible escape from proton decay. In this paper we show how ladder operators arise from the division algebras R, C, H, and O. From the SU (n) symmetry of these ladder operators, we then demonstrate a model which has much structural similarity to Georgi and Glashow's SU (5) grand unified theory. However, in this case, the transitions leading to proton decay are expected to be blocked, given that they coincide with presumably forbidden transformations which would incorrectly mix distinct algebraic actions. As a result, we find that we are left withFinally, we point out that if U (n) ladder symmetries are used in place of SU (n), it may then be possible to find this same, together with an extra U (1) X symmetry, related to B − L.

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“…In this paper, we discuss another possibility, namely, a constrained NMSSM with non-universal gaugino masses. A non-universal gaugino mass spectrum can be realized in theoretically well-motivated frameworks such as the mirage mediation [38][39][40][41][42][43][44], nonminimal GUT models [45][46][47][48][49][50][51][52][53], models with a non-universal gauge kinetic function via string compactifications [54,55], and so on, and found to be advantageous for the electroweak naturalness problem [56,57]. These observations have stimulated many studies on non-universal gaugino masses so far [58][59][60][61][62][63][64][65][66][67][68][69][70][71][72][73][74][75].…”

Section: Introductionmentioning

confidence: 99%

Non-universal gaugino masses in the NMSSM

Kawamura

Kobayashi

2018

J. High Energ. Phys.

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The Next-to-Minimal Supersymmetric Standard Model (NMSSM) provides a natural framework to realize a low-scale supersymmetric (SUSY) model, where a singlet superfield is added to the minimal model to generate a SUSY-scale higgsino mass term with its vacuum expectation value. Due to the presence of the extra singlet field, the vacuum conditions to realize the correct electroweak symmetrybreaking become fairly restrictive especially if we impose universality conditions at the unification scale. In this paper, we show that a non-universal gaugino mass spectrum can significantly relax this restriction even though the scalar masses and trilinear couplings are subject to universality conditions. With the gaugino nonuniversality, we find that higgsino can be the lightest SUSY particle and its thermal relic abundance can reproduce the observed dark matter density in a wide range of parameter space in which the 125 GeV Higgs-boson mass is obtained. This higgsinolike dark matter may be probed in direct detection experiments. We also find that there is an upper bound on the masses of supersymmetric particles in this scenario, and many model points predict colored particles such as gluino to be within the reach of a future 100 TeV collider. Implications for no-scale/gaugino-mediation models are also discussed. *

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Realization of a spontaneous gauge and supersymmetry breaking vacuum

Cited by 8 publications

References 44 publications

A low-scale flavon model with a ℤN symmetry

A low-scale flavon model with a ℤN symmetry

$$SU(3)_C\times SU(2)_L\times U(1)_Y\left( \times U(1)_X \right) $$ S U ( 3 ) C × S U

Non-universal gaugino masses in the NMSSM

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