ality ▁rel ates ▁not ▁only ▁the ▁ch iral ▁limit ▁but ▁also ▁the ▁full ▁de formation ▁space ▁of ▁the ▁theory . ▁ ▁In ▁the ▁special ▁case ▁in ▁which ▁ ▁the ▁IR ▁fixed ▁point ▁is ▁a ▁n ont rivial ▁interact ing ▁super con form al ▁field ▁theory . ▁For ▁a ▁super con form al ▁field ▁theory , ▁the ▁anom alous ▁scaling ▁dimension ▁of ▁a ▁ch iral ▁super field ▁ ▁where ▁R ▁is ▁the ▁R - charge . ▁This ▁is ▁an ▁exact ▁result . ▁ ▁The ▁dual ▁theory ▁contains ▁a ▁fundamental ▁" mes on " ▁ch iral ▁super field ▁M ▁which ▁is ▁color ▁neutral ▁but ▁transform s ▁as ▁a ▁b if und amental ▁under ▁the ▁flav or ▁symmet ries . ▁ ▁The ▁dual ▁theory ▁contains ▁the ▁super pot ential ▁. ▁ ▁Rel ations ▁between ▁the ▁original ▁and ▁dual ▁theories ▁ ▁Being ▁an ▁S - du ality , ▁Se i berg ▁du ality ▁rel ates ▁the ▁strong ▁coupling ▁regime ▁with ▁the ▁weak ▁coupling ▁regime , ▁and ▁inter changes ▁chrom oe lect ric ▁fields ▁( gl u ons ) ▁with ▁chrom om agnet ic ▁fields ▁( gl u ons ▁of ▁the ▁dual ▁gauge ▁group ), ▁and ▁chrom oe lect ric ▁charges ▁( qu arks ) ▁with ▁non abel ian ▁' t ▁H oo ft – Pol y akov ▁mon op oles . ▁In ▁particular , ▁the ▁H ig gs ▁phase ▁is ▁dual ▁to ▁the ▁conf in ement ▁phase ▁as ▁in ▁the ▁dual ▁super con duct ing ▁model . ▁ ▁The ▁mes ons ▁and ▁b ary ons ▁are ▁preserved