Abstract:We consider the top forward-backward (FB) asymmetry at the Tevatron and top charge asymmetry at the LHC within chiral U(1)′ models with flavor-dependent U(1) ′ charges and flavored Higgs fields, which were introduced in the Ref. [68]. In this model, one has to include the flavor changing couplings of the Higgs bosons as well as the Z ′ to the up-type quarks. The models could enhance not only the top forward-backward asymmetry at Tevatron, but also the top charge asymmetry at LHC, without too large same-sign to… Show more
“…In fact, the present authors recently constructed a new class of multi-Higgs doublet models which were designed to accommodate the top forward-backward asymmetry at the Tevatron without conflict with the upper bounds on the same sign top pair production at the LHC [6,7,24]. The model was based on the flavor dependent leptophobic U (1)…”
Section: Resultsmentioning
confidence: 99%
“…X can have the Yukawa couplings, λ ij Xq Li U Rj , which allow the extra quark to decay. We can avoid tree-level FCNC contributions if X does not get VEV, and X becomes a cold dark matter (CDM) candidate [6,7].…”
Section: Type-ii and Type-iv 2hdmsmentioning
confidence: 99%
“…The set similar to the Type-II model could cancel the anomaly, changing the charge assignment of the extra fields properly, and good cold dark matter candidates could be realized, as mentioned in Refs. [6,7].…”
Section: Type-iii 2hdmmentioning
confidence: 99%
“…Some of these extra new particles might have influences on the production rates and decay branching ratios of Higgs bosons. In certain models, we find that some particles are stable and can play a role of nonbaryonic cold dark matter of the universe [6,7].…”
Section: Phenomenologymentioning
confidence: 99%
“…These issues are more model-dependent, and more careful study on the Higgs boson phenomenology is required for each type of 2HDMs proposed in this Letter. This is left for a future work [11].…”
“…In fact, the present authors recently constructed a new class of multi-Higgs doublet models which were designed to accommodate the top forward-backward asymmetry at the Tevatron without conflict with the upper bounds on the same sign top pair production at the LHC [6,7,24]. The model was based on the flavor dependent leptophobic U (1)…”
Section: Resultsmentioning
confidence: 99%
“…X can have the Yukawa couplings, λ ij Xq Li U Rj , which allow the extra quark to decay. We can avoid tree-level FCNC contributions if X does not get VEV, and X becomes a cold dark matter (CDM) candidate [6,7].…”
Section: Type-ii and Type-iv 2hdmsmentioning
confidence: 99%
“…The set similar to the Type-II model could cancel the anomaly, changing the charge assignment of the extra fields properly, and good cold dark matter candidates could be realized, as mentioned in Refs. [6,7].…”
Section: Type-iii 2hdmmentioning
confidence: 99%
“…Some of these extra new particles might have influences on the production rates and decay branching ratios of Higgs bosons. In certain models, we find that some particles are stable and can play a role of nonbaryonic cold dark matter of the universe [6,7].…”
Section: Phenomenologymentioning
confidence: 99%
“…These issues are more model-dependent, and more careful study on the Higgs boson phenomenology is required for each type of 2HDMs proposed in this Letter. This is left for a future work [11].…”
We present U (1) flavor models for leptophobic Z ′ with flavor dependent couplings to the right- We also show that the extension could realize cold dark matter candidates.
It is well known that generic two-Higgs-doublet models (2HDMs) suffer from potentially large Higgs-mediated flavor-changing neutral current (FCNC) problem, unless additional symmetries are imposed on the Higgs fields thereby respecting the Natural Flavor Conservation Criterion (NFC) by Glashow and Weinberg. A common way to respect the NFC is to impose Z 2 symmetry which is softly broken by a dim-2 operator. Another new way is to introduce local U(1) H Higgs flavor symmetry that distinguishes one Higgs doublet from the other. In this paper, we consider the Higgs phenomenology in Type-I 2HDMs with the U(1) H symmetry with the simplest U(1) H assignments that the SM fermions are all neutral under U(1) H , and we make detailed comparison with the ordinary Type-I 2HDM. After imposing various constraints such as vacuum stability and perturbativity as well as the electroweak precision observables and collider search bounds on charged Higgs boson, we find that the allowed Higgs signal strengths in our model are much broader than those in the ordinary Type-I 2HDM, because of newly introduced U(1) H -charged singlet scalar and U(1) H gauge boson. Still the ATLAS data on gg → h → γγ cannot be accommodated. Our model could be distinguished from the ordinary 2HDM with the Z 2 symmetry in a certain parameter region and some channels. If the couplings of the new boson turn out to be close to those in the SM, it would be essential to search for extra U(1) H gauge boson and/or one more neutral scalar boson to distinguish two models.
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