In 1637 Fermat proposed what is known as his last theorem where
an + bn = cn only works when n = 1 or 2
After 358 in 1994 Andrew Wiles proved it and got a Nobel Gong.
In the addenda of my edition of ‘A brief history of time’ 1988, Hawkins leaves us the ‘mirror box puzzle’ petitioning us from time, to ghost-bust this spook.
In the Biverse Mirror Box:
All thru passages have an equal affect. T
All reflections have another type of equal affect. R
In box 2
)))→SM1 50% photon waves → Block→antiphoton waves →SM1
50% →SM2 25%→E→∞→Av→SM1
25%→N→∞→Av→SM1
In Box 3
North-bound photons from SM2 prefer to circle back and head south via the neighboring photon’s pathway. They return at an opposite phase and cancel each other’s journey all the way back to SM1.
The pathways have been affected the same obstacle sets—RRT = TRR.
From SM2 →100% photons →E
They have different obstacle sets —RRR≠TRR at SM2
Therefore 50%→N→∞→Av=antiverse→SM1
50%→E→∞→Av→SM1
Light will only interfere with light of the same polarization.
In Box 4
)))→ SM1→50%→N→E→D1.
Photon waves are detected at D1 which takes some data ‘∆’ from their wave function which ceases to be complete. Partially depolarised it now cannot interfere with other photon wave functions at SM2.
From D1→∆→ SM1 (Ph-∆)→SM2 50%→N→∞→Av→SM1 50%→E→∞→Av→SM1
OR
)))→ SM1→50%→E→SM2 50% )))→N→∞←Av→SM1
50% )))→E→∞←Av→SM1
NB. If photons passing thru the detector maintain their unadulterated wave function then at SM2 they would interfere like those in box 3 – viz 100% & 0%,
which they don’t.
Bi-verse circulation presents this solution to spooky duality????