1985
DOI: 10.1007/bf01159182
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Hermitian geometry and involutive algebras

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Cited by 13 publications
(3 citation statements)
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“…An intuitively obvious picture is that the diquark and the spectator quark form a configuration for which the interaction asymptotically becomes a single string extending between diquark and quark. Such a picture does indeed hold for highly excited baryons [3,4], but evidently fails for three-quark ground states, as was shown both in non-relativistic [5] and relativistic [6] approaches. More recently, it has been argued that latticecalculation results for the baryon electromagnetic structure [7] indicate only a small reduction of the scalar-diquark distribution radius relative to the vectordiquark distribution [-8].…”
Section: Introductionmentioning
confidence: 81%
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“…An intuitively obvious picture is that the diquark and the spectator quark form a configuration for which the interaction asymptotically becomes a single string extending between diquark and quark. Such a picture does indeed hold for highly excited baryons [3,4], but evidently fails for three-quark ground states, as was shown both in non-relativistic [5] and relativistic [6] approaches. More recently, it has been argued that latticecalculation results for the baryon electromagnetic structure [7] indicate only a small reduction of the scalar-diquark distribution radius relative to the vectordiquark distribution [-8].…”
Section: Introductionmentioning
confidence: 81%
“…The spin-isospin functions must be combined with the spatial wave functions to produce the three-quark wave function (J, fully symmetric under any exchange of two quarks, the antisymmetry being taken care of by the colour degrees of freedom. Then ~ can be decomposed as follows, O = ~s~s + ~Ms~s + ~*A~MA" (4) This wave function satisfies the Schr6dinger equation …”
Section: Construction Of Three-quark Wave Functionmentioning
confidence: 99%
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