2010
DOI: 10.1103/physrevd.82.035018
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Higgs mass constraints on a fourth family: Upper and lower limits on CKM mixing

Abstract: Limits on the Higgs boson mass restrict Cabibbo-Kobayashi-Maskawa quark-mixing matrix (CKM) mixing of a possible fourth family beyond the constraints previously obtained from precision electroweak data alone. Existing experimental and theoretical bounds on m H already significantly restrict the allowed parameter space. Zero CKM mixing is excluded and mixing of order Cabbibo is allowed. Upper and lower limits on 3-4 CKM mixing are exhibited as a function of m H . We use the default inputs of the electroweak wor… Show more

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Cited by 26 publications
(15 citation statements)
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“…[1,2] for reviews. It is now common knowledge that a fourth family is not excluded by electroweak precision constraints [3][4][5][6][7][8][9][10][11] or by flavor constraints [12][13][14][15][16][17]. Moreover, this extension (SM4) of the standard model also offers several desired features:…”
Section: Introductionmentioning
confidence: 99%
“…[1,2] for reviews. It is now common knowledge that a fourth family is not excluded by electroweak precision constraints [3][4][5][6][7][8][9][10][11] or by flavor constraints [12][13][14][15][16][17]. Moreover, this extension (SM4) of the standard model also offers several desired features:…”
Section: Introductionmentioning
confidence: 99%
“…We shall assume that the dominant decay modes for these two heavy quarks are t ′ → W b and b ′ → tW → W W b, which is consistent with current bounds [6,7]. It is known that the multivariate analysis methods [8], like the neural network method and the boost decision tree method, can be quite useful to separate signal to background.…”
mentioning
confidence: 89%
“…The expressions for Y 0 , S 0 , C 0 , D 0 and E 0 can be found in Appendix A, and H(x) is given in (3. 15). Note that D 0 (x) and E 0 (x) diverge logarithmically for x → 0, but G 0 (x) vanishes for x → 0.…”
Section: Four-lepton Transitionsmentioning
confidence: 99%