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RaritaSchwinger Equation
 The massless RaritaSchwinger equation has a gauge symmetry, under the gauge transformation of , where is an arbitrary spinor field.
 The massless RaritaSchwinger_equation has a gauge symmetry, under the gauge transformation of , where is an arbitrary spinor field.
 In order to avoid the difficulty we generalize the RaritaSchwinger equation so that redundant spin ½ parts are contained.
 Other aspects of this subject such as solutions of the RaritaSchwinger_equation (spin 3) and the role of generalized Hertz potentials are also discussed.

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