Summary from example phase transitions... so far

Bringing everything together from the above examples, there are a number of rules which can be used to create phase transition diagrams:

1. Phase shifts must always occur in opposing pairs.

2. A phase shift may occur as a means to simply transpose the positions of two particles.

3. One or more Rishon-triplet anti-triplets may be brought into temporary existence as a means to join multiple paired phase-shifts back-to-back, as long as each of the triplet and its anti-triplet pair is the input and output of simultaneous phase-shifts. (In Standard Models these pairs would be termed "gluons").

4. Under certain circumstances, one of each type of lighter quark - four in total - may be brought into existence from a spontaneous event represented as "VT*". VT* when treated as a Feynmann Diagram may also result in four lighter quarks being erased (with zero gamma radiation), or it may be used as a means to join any four VT0 transforms (two matched pairs) together as two inputs to a matched pair of transforms and two outputs to another pair.

5. Phase shifts involving Rishon I-Frame compound particles occur between the middle and one end of the I-Frame's three triplets, and at the same time the remaining triplet at the other end must be involved in a phase shift with another triplet from another particle (whether that be a singlet such as an electron, one of a double-particle such as a pion, or one of another I-Frame).

6. Two-particle bodies (e.g. Pions) require that both particles be involved in phase shifts, both for creation and destruction.

7. Under certain circumstances, two quarks (a Pion+, Pion0 or Pion-) may be brought into temporary existence, for less than one wavelength of the resonant frequency of an individual Rishon, where both quarks must be both the input and output of matched VT0 phase-shifts, such that the temporary particle is destroyed literally at the same time as it is created (reminder: the Standard Model calls these particles "gluons").

Rule 4 requires some additional clarification. A VT* event may be one of the following:

• The spontaneous creation of an up, anti-up, down and anti-down quark set
• The spontaneous destruction of an up, anti-up, down and anti-down quark set with no gamma radiation emitted
• The "mathematically-convenient" transformation of two quarks from the output of one pair of matched VT0 phase transforms into their opposites as the input to another pair of matched VT0 phase transforms.

Throughout all of these there really is nothing else: there is really no concept at all of "decay": there really are no other particles other than the four (twelve if phase aka "colour" is included) Rishons, which merely represent one of two different dimensions of matter with two opposite signs (and three phases 120 degrees apart). All that is happening is that energy in the form of waves that are synchronised closely in phase and location simply exchange energy between themselves in a profoundly simple and highly symmetrical way.

However when we move to the next example, involving Kaons, things get a little more complex and need further examination.