Biomedical Engineering Reference
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theoretical eigenvaluebasisfor QFT.
Ax
= λ
x
(A.1)
( x , t ) = i
H
t ( x , t )
(A.2)
ω o (A.3)
The three equations (A.1)-(A.3) demonstrate the situation
described above. Equation (A.1) is the usual form of a
generalmathematicaleigenvalueequation.Equation(A.2)isthe
Shrodinger equation where the left- and right-hand sides have
beentransposedlefttorightandrighttolefttodemonstratethe
fact that Planck's (reduced) constant is inserted heuristically
from the experiment in QM. (Planck's reduced number) is a
consequence of the formulation in Eq. (A.3) and does not come
fromexperiment.IfwereworkSFTinthewaveequationsofQFT,
this would result in a new formulation for QFT one that was
deterministic, notprobabilistic.
(b) The equations of SFT are identical with those of uncertainty
(Heisenberg's uncertainty principle [HUP]), except the inequal-
ityconditionisreplacedby two equalityconditions,onerelating
tothemotionsduetotheelectriccurrentsandtheotherrelating
to the motionsdue to the magnetic currents of each particle.
p x x
m e v
2
o
=
2
(A.4)
2
o
m e v
= 2 ω o
(A.5)
2
c = 2 ω c (A.6)
It turns out that in EM applications only two particles can be
connected to each other. They are connected by a stream of
photons. Each domain from cosmological and above, down to
photon and below, can only connect to a small discrete number
of particles (two, three or higher).
(c) WhileBohr'stheoryoftheelectronisstillrecognisedasauseful
theoretical model of the electron in the hydrogen atom, it does
not include a theory of the electron's magnetic (H) field, nor
the proton's. SFT supplies the missing theory for this simple
model.IntermsofSFTBohrtheoryissaidtobe'mono-spinorial',
m e v
 
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