“…The second school uses a Grassmannian manifold to represent gauge fields using a type of gauge-theory embedding [35,36,3,13,15,17,9,11,10,49,5,6,47,48,51,44,45,22,16,21,14,4,39,12] [ 34,27,30]. The third school introduces alternative variables for gauge theory that uncover a hidden spatial metric which reproduces the gauge fields [23,19,20,33,28,29,41,38,53]. Each of the schools start with a different geometrical representation which then faithfully maps onto the traditional gauge fields A µ .…”