Sin-Itiro Tomonaga mentioned in his Nobel Lecture, May 6, 1966 that between the years 1942 and 1946, he formulated a theory describing the probability amplitude of quantum mechanics using Dirac’s many-time theory. And by unitary transformation, one could then theoretically pass over to the Heisenberg-Pauli theory, which was based on one-time Hamiltonian formalism.
If time is analogous to angles then using compass and straightedge, one can easily bisect by geometric procedures. Here, it is taken for granted that plane angles are defined only for 2-dimensional space. But how do we bisect a solid angle of 3D-space? For example, it is possible to bisect the earth by passing a plane through the equator and separating it into two equal hemispheres. For 4D-space or even higher n-spaces, how can we construct an n-space bisector? What is the 1-dimensional analogue of the 2D plane angles?
It seems logical that a time bisector makes a lot of sense if and only if time is 1-dimensional. This bisector separates the timeline between past and future with the present moment called ‘now’. And the value of time for ‘now’ is set at zero, the time values of the past are negative integers and the positive integers for the time values of the future.


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