The MYSTERIOUS NUMBER that Shaped our Universe! Fine Structure Constant

Enigmatic Universe
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Renowned Austrian physicist Wolfgang Pauli, for whom the Pauli Exclusion Principle is named,
once said, When I die, my first question to the devil will be,
What is the meaning of the fine structure constant? American physicist Richard Feynman
described it as a magic number that comes to us with no understanding. This constant,
represented by the Greek letter alpha, appears on the surface to be nothing special. It's just
a dimensionless number. So no matter what units you use, it will always have the same value,
approximately 1 over 137. Yet its precise value could not be more important. Some studies showed
that if it was different by just 4%, you and I would not exist, because stars could not make
carbon and oxygen, elements essential for life. Its value being so precise is one of the reasons
that some believe nature must be fine tuned for life. This constant seems to turn up everywhere
in physics, like the quantum theory governing the electromagnetic force. Yet its value cannot
currently be predicted directly from any theory. It's one of those fundamental constants we simply
have to measure experimentally in nature. It's one of the parameters that is inserted by hand
into the standard model of particle physics, our best theory of nature, to make the theory work.
Some numerologists have even suggested a mystical significance to the number 137,
because it seems to show up in other places in nature as well. What is this mysterious constant?
Why does it have the value that it does? And what does it represent? The complex physics
behind the constant, simplified to the best of my ability, is coming up right now.
First, what is the fine structure constant? Well, the equation for alpha looks like this.
At one time it was believed to be exactly 1 over 137, but advancing technology has allowed us to
measure this much more precisely. It's equal to the following. It is now one of the most precisely
measured constants we have. The predicted and measured value correspond with a standard
uncertainty of only 0.23 parts per billion. There are no units attached to this number because it
is dimensionless. Dimensionalist units are interesting because they are independent of
any arbitrary measuring units we might use, such as meters or seconds or grams. It's like pi. It's
a kind of ratio. If an alien race was advanced enough to figure out the same science that we
have, they would come up with exactly the same number for pi and the fine structure constant
when converted to log base 10. Now we use log base 10 because we have 10 fingers and toes.
Aliens may use base 2 or 8 or 12 or whatever. 10 is arbitrary.
Numbers and equations are nice, but now the question is,
what is the physical interpretation of the formula that leads to this mystery number?
If we examine the formula closely, there are a few different ways
that we can write it out and think of what that number represents.
First, if we rewrite the formula in a slightly different way, we get a ratio that looks like
This represents the ratio of two energies. The energy needed to overcome the electrostatic
repulsion of two electrons that are a distance d apart and the energy of a photon with the wavelength
lambda. Another way to rearrange the formula results in a ratio that may be even easier to
understand. This essentially represents the ratio of the speed of an electron in a classical orbit
to the speed of light. In other words, the speed of an electron orbiting the classical
model of an atom is about 1 137th the speed of light, or the electron travels
at 1 137th the maximum speed allowed in nature. Keep in mind that this understanding would be
in the Bohr model of the atom, which modeled it as a negative point charge spinning around
a positively charged nucleus. Our understanding of the model of an atom today is different.
With the advent of the Schrodinger equation and a deeper knowledge of quantum mechanics,
our modern model of the atom shows the electron being a negatively charged
probability cloud around a fuzzy, positively charged nucleus.
Now how is this number useful in modern physics? The number is directly related to the strength
of the electromagnetic force. In other words, it represents the strength of the interaction
between two charged particles. So for example, the higher the value, the greater the strength
of attraction between an electron and a proton. And equivalently, the greater the strength of
repulsion between two of the same charges, such as two electrons. You might say, well,
this sounds a lot like Coulomb's constant in Coulomb's law, which relates what the force
between two charges separated by a distance r would be. Well, you'd be spot on because one
way to think of the fine structure constant is like Coulomb's constant expressed in dimensionless
units. This constant is found everywhere because in our macro world, the two fundamental forces
we directly experience most are gravity and electromagnetism. You know how important gravity
is, but electromagnetism is everywhere too. For example, in the form of light, which are
electromagnetic waves, your cell phone electronics, and chemistry, since it's the interaction of
negatively charged electrons and atomic nuclei in atoms and molecules. Thus, the chemistry of life
is determined by electromagnetism. Since the fine structure constant characterizes the strength of
this electromagnetic force, it's critical for life. One way to visualize the fine structure constant
is by using Feynman diagrams. This diagram comes from the math of the quantum theory describing
electromagnetic force called quantum electrodynamics or QED. The arrows represent
two charged particles and the wavy line represents photons. So in this diagram, what we're seeing is
two electrons moving near each other, exchanging a photon, and then being repelled away from each
other. QED shows us that it's the exchange of photons that causes repulsion or attraction.
I have a full video on QED if you want to know the details of this. The vertex is the point where
the charged particles release or absorb a photon. And it's this vertex where alpha, or the fine
structure constant, plays a crucial role because it is the coupling constant that tells us the exact
strength of this interaction. Alpha is related to the probability that an electron will emit or
absorb a photon. We've known this constant for more than a hundred years. It was German theoretical
physicist Arnold Sommerfeld who introduced it in 1916 when he was expanding the Bohr model of the
atom. In 1912, Niels Bohr came up with a model of the atom where the electrons orbited around the
atomic nucleus like planets orbiting the sun. But unlike planets, Bohr proposed that electrons can
only occupy certain energy levels proportional to Planck's constant, which he called atomic orbitals.
In other words, the energies of electrons in these orbitals were quantized. And when electrons changed
from a higher orbital to a lower orbital, they released energy in the form of photons.
And they absorbed energy when they moved from lower to higher orbitals. His original equation
looked like this. The original Bohr equation from 1913 simply states that the energy depends
on the quantum number n, which is simply the orbital that the electron is sitting in. This
model solved several problems in classical physics and contributed to our current understanding of
quantum mechanics, but it failed to precisely reproduce experimental results of the light
emitted by atoms. The energy levels appeared to split in two, whereas Bohr's model only predicted
one. Those additional levels were very close to each other, but they indicated that Bohr's model
was incomplete. It was too simplistic. It did not take into account the spin of electrons or
relativistic effects. It only predicted the coarse structure of atoms based on the main orbitals.
Sommerfeld was able to show that there is a finer structure of the atom,
that it has sub-orbitals. Sommerfeld modeled the hydrogen atom as Bohr did, but incorporated a
factor that was the ratio of the electron's velocity to the speed of light. He incorporated
the fine structure constant, which more accurately described the observed results
of the energy emission of the atom. Sommerfeld's modified version of Bohr's equation looks like this.
This equation takes Bohr's original equation and adds an additional factor, the stuff to the right
of the plus sign. You'll notice that alpha, the fine structure constant, shows up in the additional
factor. This factor has to be added by hand after making measurements to find out what it is.
This was a brilliant modification by Sommerfeld that gave us a deeper understanding,
and he accomplished all this without having access to the superb online learning platform
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So the next question is, how is the fine structure constant measured?
Alpha can be measured experimentally at cyclotron accelerators like Fermilab in Illinois.
This is done by accelerating an electron in a magnetic field and measuring its magnetic moment.
In very general terms, the electron acts like a spinning bar magnet.
The magnetic moment is related to the strength and direction of the magnetic field created by
this electron. The alpha value can then be figured out from this measurement.
Now, why is the number 1 over 137 so significant? Well, for one thing, it's a small number. This
means that electromagnetism is relatively weak, at least compared to the strong nuclear force.
The consequence of this is that electrons orbit on average at a substantial distance away from
the proton. This can be understood explicitly from the Bohr radius, which is the radius of
hydrogen atom. Where A-naught is the radius, h-bar is the reduced Planck's constant,
m-e is the electron mass, c is the speed of light, and alpha is the fine structure constant.
We see that because the radius of the atom depends on the inverse of alpha, then a smaller alpha
gives us a large radius. For example, if the nucleus of an atom was the size of a golf ball,
the size of the electron probability cloud would extend to 2.5 kilometers.
This distance allows electrons to be relatively available for exchange with other atoms,
so that chemistry can take place, and thus life is possible. On the other hand,
this number is not too large, because otherwise atoms would not form in the first place.
So in our universe, it is relatively balanced, not too low and not too high.
You might say the fine structure constant is in the Goldilocks zone.
In 1967, English astronomer Fred Hoyle and others worked out the process by which stars
produce heavy elements such as carbon, nitrogen, and oxygen. They found that the abundance of
carbon in the universe could be explained only if the fine structure constant had a value
that made the nuclei of helium atoms more likely to fuse to produce carbon nuclei than otherwise.
This higher probability of fusion makes it possible for all these heavier atoms like
carbon to exist. And the existence of these elements is the reason life exists on earth.
Scientists calculated that if this constant was different by about 4%,
we may not have had these heavier elements because either helium would not fuse,
or stars would burn out too quickly due to too much fusion.
What then determines the value of alpha? Well, scientists are still trying to figure this out,
since there is no theory that predicts it. Some believe that the value of alpha was set
at the moment of the big bang due to the initial conditions from quantum fluctuations.
Some think that they are tiny hidden dimensions as predicted for example in string theory,
and that it is the geometry of these dimensions that fixes the value of the
structure along with other fundamental constants as well. Most scientists believe there must be
some way to calculate this value. We just haven't figured it out yet.
Now why do some people assign it a mystical meaning? Mainly because 137 seems to appear
elsewhere too. For example, some say that it can't be a coincidence that the age of the universe
is 13.7 billion years. This is a stretch because current best estimates say that the number is
about 13.8 billion years. The number also shows up in Jewish mysticism as well as the Christian
Bible. I think Richard Feynman said it best, it's one of the greatest damn mysteries of physics.
You might say the hand of God wrote that number, but we don't know how he pushed his pencil.
Is alpha really a constant though? The answer is no. Alpha actually changes as a function of
energy conditions under which you perform your experiments. This is what the theory of QED shows,
that the coupling that is alpha changes depending on the energy of the system.
It is indeed very close to 137 at about 0 Kelvin, which is roughly the temperature of the universe.
Actually, it's a little over 2 Kelvin. In the grand scheme of things,
even room temperature or about 300 Kelvin is also very low energy. But at very high temperatures,
like 10 to the 15 Kelvin, such as was present near the time of the big bang,
it would not be the same as it is today. It would have been around 1 over 127 or larger.
But after a few minutes, as temperatures and energies reduced, it would have reached
1 over 137 as today. So this means that alpha was higher in the early history of the universe.
So why then do we call it a constant if it actually isn't? The answer is simple.
For most practical purposes, we use it to describe systems that are
so cold that the temperature dependence doesn't affect its value.
So when we say that alpha is 1 over 137, we mean that it is this value at low temperatures.
And in that limit, it's a constant. This, however, doesn't tell us why it is 1 over 137.
As with other parameters of the standard model, we don't know why they have the values that they do.
You could invoke the anthropic principle because we do know that the universe would probably look
very different if the value of alpha was sufficiently different from what it is right now.
But until we have a more complete theory of nature, like a grand unified theory,
the enigma of alpha remains. If you liked this video,
please subscribe and I'll see you in the next video my friend.
