In conventional quantum field theory the path integral for a free point particle quantum mechanics is written in Dirac’s bra and ket notations as áF|exp(iHT)|Iñ where I is the initial state and F is the final state. Exp(iHT) is the unitary operator and H is the Hamiltonian of kinetic energy function plus the potential energy function. T is the total of the time parameter between the quantum transition between I and F, and of course i is the imaginary unity.
However, if the unitary operator is replaced by the real Hadamard operator of square of energy as space-time quantum then the path integral become time independence and I and F can be replaced by the values of the fractal dimension. Since gauge invariance applies to fractal dimensions ½ is equivalent to 1½ or 2½ or 3½, so that the whole number parts can be simply ignored. The new path integral becomes á0|H|½ñ relative to the state of the quantum vacuum 0. Perfect symmetry implies that á0|H|½ñ=á½|H|0ñ. However, spontaneous symmetry breaking start to appear where and when the single Hadamard operator H is replaced by its compositions such that in general á0|HH···HH|½ñ≠á½| HH···HH|0ñ. Symmetry breakings allow 2 things to happen: (1) increase in mass decrease in energy or (2) decrease in mass increase in energy obeying the principle of mass and energy equivalence: E=mc. For the special case of perfect symmetry, c=1 and E=m. An example of a fractal path between fractal dimension ½ and 1/6 is á1/6|HH···HH|½ñ≠á½| HH···HH|1/6ñ. In reference to the algebra of yin-yang compositions, it can be shown that the mass is inverse proportional to the fractal dimension. However, at fractal dimension of ½ the rest mass of the free particle is exactly zero.


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