The Constant Alpha 


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Summary: The value of the fine structure constant Alpha in low energy limit and its significance based on the discrete measurement space, is discussed. We have so far described the system in terms of measurements. A measurement has two components, (i) an application of the measurement force (ii) the measurement of response. Both these components combined together are called an interaction. An interaction and a measurement are analogous to each other. We make a simple hypothesis that, " Every observer making a measurement of the environment or a system, is simultaneously measured by the environment or the system." Above statement is a generalization of the the Newton's third law of equal and opposite reaction. It differs from the classical definition in the sense that the object interacting with each other, are of different capabilities. Therefore the measurement forces applied by the objects in jspace will be different and may not be measurable by the objects interacting with each other. We can also say that the object with significantly lower capability may not know that it is being measured. In classical mechanics both objects have equal capabilities and hence equal and opposite reactions. An equivalent statement can also be made that an observer in the discrete measurement space can not make an measurement without being measured. In an atomic structure the electrons interact with each other with photons. Which is equivalent to saying that the electrons measure and are measured with photons. Further the waveparticle duality allows the photons to be represented by the electromagnetic waves. The electromagnetic waves have the vectors E (electric vector) and H(magnetic vector) representing a relationship which is progressing with time and defined classically by Maxwell's equations. The vectors E and H are considered to be at a phase difference of π/2 in the physical space. We also derived a relationship for the information progress in jspace as,
Let us consider
the value of Y
for q = 3, it is 8.616 x 10^{2}.
The value is calculated based on assumption that the angle between E
and H
is π/2.
The corresponding value of 1/Y^{2}
is 134.7. The standard value for 1/Y^{2}
is approximately 137.04. The exact value of the finestructure constant
corresponds to q ~ 3.009.
We have to keep in mind that q is calculated based on the ratio of two
irrational functions hence can not be an exact natural number. The known standard values are shown in parenthesis. The number 0.8542455 for the variable Y represents the amplitude for an electron to emit or absorb a photon also known as the coupling constant. We square to get the finestructure constant alpha (1/137.04). The
relationship e^{1q}÷(π/2)
does not require any prior knowledge of a physical structure and it
does not use any measured physical constants such as electric charge e,
speed of light c
or the Planck's constant h
in its derivation.
This relationship should be applicable to stable structures in
discrete jspace, which are measured using electromagnetic
interaction with the specific structure. Thus the introduction of the
value of π/2
provides results for the phenomena in which the measurement using
electronphoton interaction, plays an important role.
We also note
that the values calculated using the factor e^{1q},
represent the values in the asymptotic region as each q
value represent a PE1 event. For phenomena where interactions between
the structure being measured and the measurement signal, are of nature
other than EM, appropriate dimensionless constant(s) need to be
introduced in place of π/2.
We have described the nature of the system based on PE1
measurements. These measurements do not assume preexistence of
variables or coordinate systems. Only condition placed is the
requirement of PE1 events. The description provided by the observer
is based on the measurements only and the variables or reference
systems must be derived from the information obtained from these
measurements. The description of the system using the Cartesian
coordinates or spacetime coordinates will be required when the
application of the measurement force is necessary to make an
observation, and correlation needs to be made with experimental results.
What we are suggesting is that the
physical structures measured are the components of the information
space represented by (e^{1q}) whereas the
observer's measurement capability (π/2)
is represented by the phase
relationship between E
and H. The finestructure constant under the
lowenergy limit tells us
where do we stand in terms of measuring an infinite information space
in a discrete measurement space. We take note that we are
essentially measuring δ_{i} in jspace.
The
term "finestructure constant" represents
electronphoton coupling in zeroenergy limits. It is known that the
value of alpha approaches 1/128 for the interaction energies above
80GeV. Thus alpha is not really a constant but dependent on the
interaction energy. The relationship of alpha with qvalues also shows
it, as the interaction energy would be higher for lowq values and
therefore the value of alpha would go up with increasing interaction. It is often asked if alpha is not really constant then why worry about explaining its value? We need to remember that the value 1/137 still represents the one end of the spectrum, the end at which we exist and experience. Therefore it is important to understand the value of alpha at the low energy limit. If the interaction energies are increased further the value of alpha would go up then what does that mean in terms of qvalues? The value 80GeV corresponds to Δq equal to approximately .068. The ionization potential of 13.6eV corresponds to Δq equal to approximately 1.16×10^{10}. Our playing ground is fairly small in qspace.
We may
also want to think, if the atomic structure is q=3 state, then what is
the significance of q = 2 state? Admittedly it represents more
information than available for q = 3 state.
It will be most interesting to find out or even be able to predict what
type of structures would we observe, if we could measure q = 2 state.
One thing for sure that there is a huge amount of energy involved.
And then what do the value of q higher than 3 represent? Surely these
structures are easily measurable or in other words they should be right in front of us.
Also if we can not measure the origin
accurately, how can we be so sure that the vectors E and H are at exact 90^{o} angle
to each other? How can we correlate this specific issue of angle
between E and H being exactly 90^{o
}to the restriction of the 3dimensional space? We will
attempt to answer this question next. Information on
www.ijspace.org is licensed under a Creative Commons
Attribution 4.0 International License.

" I believe that it will only be possible to write the conclusion if a theory will be established which will determine the value of the finestructure constant and will thus explain the atomistic structure of electricity, which is such an essential quality of all atomic sources of electric fields actually occurring in Nature."  Wolfgang Pauli, "Exclusion principle and quantum mechanics", Nobel Lecture, December 13, 1946. "It has been a mystery ever since it was discovered more than fifty years ago, and all good theoretical physicists put this number up on their wall and worry about it."  Feynman writing about the finestructure constant in "QED: The strange theory of light and matter", Princeton University Press. Bethe, Hans A. and Salpeter, Edwin E., “Quantum Mechanics of One and Twoelectron Atoms”, Springer Verlag and Academic Press, 1957, is a good reference. The correlation between the electromagnetic mass, rest mass and the fine structure constant is discussed in Brillouin, L., “Science and Information Theory”, Academic Press, New York, 1962 