Unimodular Matrices Homomorphic to Lorentz Transformations
نویسنده
چکیده
deutet und N die oben mit e~lF bezeichnete Größe ist, woraus dann die FREDHOLMsche Lösung der Integralgleichung (15) folgt. Da bei unserem Verfahren derselbe Ausdruck für 5 ( 1 , 1 \ g ) folgt wie bei MATTHEWS und SALAM, so sollte die entsprechende Reihenentwicklung nach Potenzen von g zu der FREDHOLMschen Lösung führen. Dabei müßte eine Identität bestehen zwischen den entsprechenden Koeffizienten, die in beiden Fällen dieselben Kombinationen der nach den beiden Verfahren beziehungsweise berechneten Propagatorausdrücke enthalten. Man würde erwarten, daß dadurch die Identität der entsprechenden Propagatoren folgen würde. Jedoch dürfte eine eingehende Untersuchung der betreffenden Propagatoren auf Grund des hier vorgeschlagenen Verfahrens erforderlich sein, um diese Frage zu entscheiden.
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تاریخ انتشار 2012