2016
DOI: 10.1007/jhep11(2016)052
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A collider observable QCD axion

Abstract: We present a model where the QCD axion is at the TeV scale and visible at a collider via its decays. Conformal dynamics and strong CP considerations account for the axion coupling strongly enough to the standard model to be produced as well as the coincidence between the weak scale and the axion mass. The model predicts additional pseudoscalar color octets whose properties are completely determined by the axion properties rendering the theory testable.

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Cited by 83 publications
(62 citation statements)
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“…[41][42][43] for models of a visible axion as an explanation of the diphoton excess. 2 There is an alternative way to form domain walls in a multi-axion scenario, where the system exhibits a chaotic behavior (axion roulette) during a mass level crossing between two axions [48,49].…”
Section: Jhep08(2016)044mentioning
confidence: 99%
“…[41][42][43] for models of a visible axion as an explanation of the diphoton excess. 2 There is an alternative way to form domain walls in a multi-axion scenario, where the system exhibits a chaotic behavior (axion roulette) during a mass level crossing between two axions [48,49].…”
Section: Jhep08(2016)044mentioning
confidence: 99%
“…The behavior of the η can be studied in the framework of new exotic confining color groups, which are prevalent in model building to address the strong CP problem [20][21][22][23][24][25][26][27][28][29][30][31]. Heavy or visible axion models predominately utilize exotic color groups to alter the typical (m a , f a ) relationship [22][23][24][25][26][28][29][30][31][32][33]. There are generic features of chiral phase transitions in dynamical axion models that set them apart from general confining hidden sector models.…”
Section: Introductionmentioning
confidence: 99%
“…Interesting models implementing the mechanism of [12] were proposed in [14][15][16][17][18], applications to models of inflation were studied in [19]. Other approaches to modify the axion mass within QCD were proposed in [20][21][22][23] while in [24][25][26][27][28][29][30] the axion mass is raised by coupling it to a new confining gauge group.…”
Section: Introductionmentioning
confidence: 99%