2017
DOI: 10.1103/physrevd.96.035004
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LHC constraints on color octet scalars

Abstract: We extract constraints on the parameter space of the MW model by comparing the cross-sections for dijet, top-pair, dijet-pair, tttt and bbbb productions at the LHC with the strongest available experimental limits from ATLAS or CMS at 8 or 13 TeV. Overall we find mass limits around 1 TeV in the most sensitive regions of parameter space, and lower elsewhere. This is at odds with generic limits for color octet scalars often quoted in the literature where much larger production cross-sections are assumed. The cons… Show more

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Cited by 31 publications
(30 citation statements)
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References 58 publications
(79 reference statements)
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“…However, the limits obtained from this channel are still not better than those obtained for √ s = 8 TeV in Ref. [70].…”
Section: Introductioncontrasting
confidence: 53%
See 1 more Smart Citation
“…However, the limits obtained from this channel are still not better than those obtained for √ s = 8 TeV in Ref. [70].…”
Section: Introductioncontrasting
confidence: 53%
“…The most stringent limits on the direct production of these scalars come from Ref. [70], where the single and pair production of neutral scalars was studied. The recent release of high-luminosity experimental searches for massive resonances decaying into heavy quarks [72][73][74][75] makes now possible to improve those bounds.…”
Section: Introductionmentioning
confidence: 99%
“…Concerning the scalar messengers, we have two pairs of these, the σ a ∼ ð8; 1; 0Þ, which are singlets under SUð2Þ L , and the η a , which transform as weak doublets, η a ∼ ð8; 2; 1=2Þ. As color octets, these would also be copiously produced at a hadron collider of sufficient energy [28]. However, their masses are expected to lie well above the reach of the LHC.…”
Section: Color Octets At Hadron Collidersmentioning
confidence: 99%
“…In addition, direct searches for ± are also performed by the Tevatron [51], ATLAS [52], and CMS [53] experiments, among which most constraints depend strongly on the underling Yukawa structures. Recently, by comparing the cross-sections for the dijet, top-pair, dijet-pair, , and production at the LHC with the strongest available experimental limits from ATLAS or CMS at 8 or 13 TeV, Hayreter, and Valencia [54] has extracted constraints on the parameter space of the ManoharWise model [24], which is equivalent to type C 2HDM discussed here. Interestingly, they found that masses below 1 TeV have not been excluded for color-octet scalars as is often claimed in the literature.…”
Section: Results In the 2hdms With Mfvmentioning
confidence: 99%