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Weakly-interacting massive particles in non-supersymmetric SO(10) grand unified models

机译:非超对称的弱相互作用颗粒(10)大统一模型

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A bstract Non-supersymmetric SO(10) grand unified theories provide a framework in which the stability of dark matter is explained while gauge coupling unification is realized. In this work, we systematically study this possibility by classifying weakly interacting dark matter candidates in terms of their quantum numbers of SU(2)~( L ) ? U(1)~( Y ) , B ? L , and SU(2)~( R ). We consider both scalar and fermion candidates. We show that the requirement of a sufficiently high unification scale to ensure a proton lifetime compatible with experimental constraints plays a strong role in selecting viable candidates. Among the scalar candidates originating from either a 16 or 144 of SO(10), only SU(2)~( L ) singlets with zero hypercharge or doublets with Y = 1 / 2 satisfy all constraints for SU(4)~( C ) ? SU(2)~( L ) ? SU(2)~( R ) and SU(3)~( C ) ? SU(2)~( L ) ? SU(2)~( R ) ? U(1)~( B ? L ) intermediate scale gauge groups. Among fermion triplets with zero hypercharge, only a triplet in the 45 with intermediate group SU(4)~( C ) ? SU(2)~( L ) ? SU(2)~( R ) leads to solutions with M ~(GUT) & M ~(int) and a long proton lifetime. We find three models with weak doublets and Y = 1 / 2 as dark matter candidates for the SU(4)~( C ) ? SU(2)~( L ) ? SU(2)~( R ) and SU(4)~( C ) ? SU(2)~( L ) ? U(1)~( R ) intermediate scale gauge groups assuming a minimal Higgs content. We also discuss how these models may be tested at accelerators and in dark matter detection experiments.
机译:Bstract非超对称SO(10)大统一理论提供了一种框架,其中解释了暗物耦合统一的暗物质的稳定性。在这项工作中,我们通过在苏(2)〜(L)的量子数量方面进行弱互动的暗物质候选来系统地研究这种可能性? U(1)〜(y),b? L,Su(2)〜(r)。我们考虑标量和费米尔候选人。我们表明,需要足够高的统一规模,以确保与实验约束兼容的质子寿命在选择可行的候选者方面发挥着强大作用。在源自如此(10)的16或144的标量候选中,仅具有零超充电或带Y = 1/2的双重的SU(2)〜(L)单体满足SU(4)〜(C)的所有约束还是su(2)〜(l)? su(2)〜(r)和su(3)〜(c)? su(2)〜(l)? su(2)〜(r)? U(1)〜(b?l)中间尺度计组。在零超充电量的Fermion三胞胎中,45中的三重态中间组苏(4)〜(c)? su(2)〜(l)? SU(2)〜(R)导致M〜(肠道)&gt的溶液。 m〜(int)和长型寿命。我们发现三种型号,弱双头和y = 1/2作为苏(4)〜(c)的暗物质候选者? su(2)〜(l)? su(2)〜(r)和su(4)〜(c)? su(2)〜(l)? U(1)〜(r)中间秤仪表,假设HIGGS内容最小。我们还讨论如何在加速器和暗物质检测实验中测试这些模型。

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