Room Temperature Quantum Computers

Re:http://www.fetzer-franklin-fund.org/events/emqm17/

argument between Tegmark and Hameroff at the recent Fetzer Meeting on Bohm in London.

Boltzmann factor exp(-hf/kT)

 

hf/kTnon-eq = hf/kTeq +/- (sigma)P/hf^2  Ansatz 2 (dimensionless equation)

 

Sigma = coupling cross-section of external pump power flux real quanta to target quanta

“real” = on mass shell (QFT) “virtual” = off mass shell 

P ~ external pump power flux [P] = energy/area x time

f = frequency of real pump quanta

+ for continuous energy eigenvalues of real target quanta Tnon-eq remains positive —> 0 with a Tc > 0 for BEC Frohlich-Glauber coherent state

- for discrete energy eigenvalues of real target quanta Tnon-eq goes negative (discrete energy eigenvalue population inversion) creating BEC above critical pump threshold Pc at Tnon-eq = 0 critical point for non-equilibrium dynamical quantum phase transition.

 

 

Ansatz 3

 

PQM back-reaction ~ [(particle 4-velocity vu ) - weak pilot wave 4-current density jw /4-density (jwujw^u)^1/2) 

 

~ (sigma)(P - Pc)Step Function(P - Pc)/hf’^2

 

Note that f’ is frequency of target quanta, do not confuse with f = frequency of pump quanta.

 

 

Step function = 0 when P < Pc, = 1 when P > Pc