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Austin to AI:Â Aha, that is excellent. Can I ask you another angle. Bryan uses CL(2,) algebra which seems to change particles away from the normal standard model reliance on dirac's cl(3,1). Can I still get the same or simular handshake equations for the 2-slit experiment if I were to use cl(3,1) or does Bryan's new algebra give an advantage?
AI Reply:Â Yes, you can absolutely derive the same or highly similar retrocausal handshake equations using Dirac's standard \(Cl_{3,1}\) spacetime algebra (STA). However, understanding the difference between your approach and Bryanâs highlights the distinct advantages of each.
Here is a breakdown of how the two algebras handle the handshake and where Bryan's model claims its advantage:
1. The retrocausal handshake in \(Cl_{3,1}\) (STA)
If you stick with \(Cl_{3,1}\), your forward Offer Wave (OW) and backward Confirmation Wave (CW) are mapped in a full 4D spacetime arena.
2. What is Bryan's \(Cl_{2}\) strategy?
Bryanâs Bivector Standard Model (BiSM) deliberately steps away from the 4D Dirac algebra. [1]
3. Does Bryan's new algebra give an advantage?
Bryan's framework offers specific geometric advantages, though it introduces certain trade-offs for retrocausal modeling:
Advantages of \(Cl_{2}\) (Bryan's view)
Disadvantages for your model
Summary for your commentary
You can tell Bryan that both paths are mathematically viable, but they serve different physical interpretations:
If you want to keep the literal "handshake through time" between preons and hexarks, \(Cl_{3,1}\) provides a clearer framework for tracking those advanced and retarded trajectories.
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Now in the Double Slit article article, you stateWe interpret the two energy states as internal energy, which is absent for point particles. This is caused by the precession of the two spin axes on the same particle, Figure 4. As mirror states, they are depicted as being in phase with equal, but opposite, energyâthe two couple to give a resonance spin-1. Precession, as shown, gives one component of, say, m = +1. Reversing these precessions gives the m = â1 component. The m = 0 component cannot form since it would violate the reflective symmetry between the mirror states. Note also that a photon has no m = 0 component. The two axes form the resonance boson, as shown in Figure 4. Rather than Diracâs matter-antimatter pair, Q-spin resolves the negative energy problem Dirac encountered because the two axes must have equal energy but spin oppositely.
This defines the magnetic quantum state of đ=0, which carries no external polarization or helicity. Here we assume that as spins propagate to the screen, no fields are present, and they do so in the đ=0 state.And is reinforced in Section 4.1
In the bivector model, the free-flight electron in the đ=0Â state is isotropic and carries no externally defined polarization axis.
"How does this document resolve the Bell inequality?"
I will try to do better."I have attached a draft on Bell inequalities. Act as a highly skeptical quantum physicist and a strict peer reviewer. Identify any unstated assumptions, logical leaps, or potential conflicts with established quantum foundations. Challenge the core thesis of this paper."

On 12 Jul 2026, at 23:06, anton vrba <anto...@gmail.com> wrote:
Hi Bryan, I am trying to understand this paper, honestly a lot is still Greek to me. After my first reading, I have discovered a contradiction.
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Thank you all for the discussion which is long and in different threads which I have read. So this is a short global reply.Â
As with any developing research program, ideas evolve and earlier papers are refined as the underlying picture becomes clearer. For me, too, when I look back, I realize I could have explained better and clearer. With time, they do improve. I actually think all these doubts and questions are answered in the new paper. So rather than continuing to debate intermediate stages, I think it is better to wait for the next paper.  There the quantum domain, the role of the (m=0) state, and the simulations will be presented in a more coherent and reproducible form. I do not see any errors, only isolated statements that, taken alone, might be unclear and misleading. I really work hard to make things clear, but I understand it is a challenge.
Austin, your questions about the double slit, I comment
Anton, I think you are saying  my work needs a more fundamental field-theoretic foundation. You also raise issues about m = 0. That part of how the free=flight spin (m = 0) evolves is critical and follows from the classical dynamics. I have spent a lot of time on the m = 0 and the \pm 1 states, so I agree, that part contains a lot and needs more discussion. What I think is interesting, is both the double slit and epr are done in the absence of a polarizing field, until the filter. So both evolve as m = 0 and only become m = \pm 1 when approaching a field (context instantiation). Most experiments, SG, are done in polarizing fields, so m = \pm 1. I do not think I have earlier conceptual errors: it is a matter of seeing how the GA rotors evolve.
Richard is right that the new paper is what matters now. But he is now repeating the same conclusions before seeing the completed work, and speculates. So no reply is needed and my comments are unlikely to move the discussion forward. I will let the new paper speak for itself.
Thank you all for engaging and comments, useful and welcome
Bryan
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What I think is interesting, is both the double slit and epr are done in the absence of a polarizing field, until the filter. So both evolve as m = 0 and only become m = \pm 1 when approaching a field (context instantiation). Most experiments, SG, are done in polarizing fields, so m = \pm 1. I do not think I have earlier conceptual errors: it is a matter of seeing how the GA rotors evolve.
