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3.2Difficulties with the wave equation

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As we now show, the wave equation (3.1) presents a number of problems which will eventually lead us to abandon it.

Locality

The wave equation (3.1) has an unwanted property: In order to determine the change in the solution at the point in an infinitesimal time interval (t, t + dt), we must know the function for time t at all points . This property is contained in the Taylor expansion of the Hamilton operator in powers of the Laplacian and is referred to as non-locality. It is also evident from the form of the solution (3.4) by noting that


which upon using the Taylor expansion in p2 becomes


Foundations of Quantum Field Theory

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