The way this works is, the Laws of Spin and Statistics say that since electrons are fermions, they can't occupy the same state or they will cancel out, and that would violate energy conservation, charge conservation, and lepton number conservation. This is a direct result of the fact that half-integer spin implies that if you rotate a fermion 360 degrees, it is distinguishable from its unrotated counterpart; it must be rotated 720 degrees to be indistinguishable. Thus, only one electron can occupy one quantum state at one time.
It was here I noticed the missing concept.
It's phase. Spin, for a quantum (which an electron is), is a concept that involves phase. The reason that quanta must always have either integer or half-integer spins is that they must remain in phase with themselves. If they could vary their phase, then they could cancel out and disappear- and this would violate conservation laws (generally mass/energy conservation, and specifically conservation of any charge they might carry). I might post somewhere else on where conservation laws come from (a tease: they're based on symmetries), but for the moment just accept that they exist, and are absolute, and are the result of the characteristics of the geometry of spacetime. If you think of the phase of a quantum with an integer spin, it duplicates itself every time the quantum rotates once. That means that wherever the phase of the wave function that defines that spin is high on one rotation, it's high on the next one- and every one thereafter. Spin is an inherent parameter of quanta, like their mass, or the charges they carry; and the phase of that spin can either be in phase on each rotation, which is integer spin, or out of phase on each rotation, which is half-integer spin.
Now, two waves that are precisely out of phase can cancel one another. Since the phase of the spin of a half-integer spin quantum isn't out of phase with itself
at the same time, but on the next rotation, it doesn't cancel. And because it comes around to the same phase on the next rotation, it reinforces its own existence. But if two of them could occupy precisely the same position, then if one had positive spin and the other negative,
they could cancel one another out, and this would violate conservation laws for their charges, and their masses, and so forth. So half-integer spin quanta cannot occupy the exact same location; they are
exclusive, in that the occupation of a location by a half-integer spin quantum excludes the possibility of any other identical quantum occupying that spot.
Now, remember that the wave functions of the spin are Schroedinger wave functions; that means they are probability waves. So what this means is that
the probability of two half-integer spin identical quanta occupying the same spot is zero. Physicists called this the Pauli exclusion principle for a long time, and some still do, because it was discovered by Wolfgang Pauli.
But the integer spin particles behave exactly the other way; they cannot cancel. They reinforce one another. The wave function for two integer spin particles at the same spot is twice as high. They are in phase, and they reinforce. And since the waves are probability waves, that means that
the probability of two integer spin identical quanta occupying the same spot is twice the probability of them occupying different spots. And this is the reason for lasers, and Bose-Einstein condensates.
These two principles of spin are called the
Laws of Spin and Statistics. The statistics of the integer spin quanta were first worked out by Albert Einstein and Satyendra Nath Bose, and are therefore called Bose-Einstein statistics. The statistics of half-integer spin quanta were first worked out by Enrico Fermi, the man who led the part of the Manhattan Project during World War II that led to the creation of the first nuclear reactor, and the first sustained nuclear reaction, and Paul Dirac, the creator of the most complete, accurate, and precise theory in the history of all of science, quantum electrodynamics, and these statistics are therefore called Fermi-Dirac statistics. Quanta of the former type are called bosons, and of the latter, fermions. It is worth mentioning that of the four, only Bose did not win a Nobel prize; and there is significant feeling that he should have, particularly among Indians. It should be noted that India has a long tradition of mathematical scholarship, and that the widely (but not universally) acknowledged greatest mathematical talent to have lived so far is Srinivasa Ramanujan; and never forget that Einstein spoke of the piercing comprehension of Subrahmanyan Chandrasekhar's mathematical realization of Einstein's field equations for gravity, and Karl Schwarzchild's conception of the black hole, in his work on determining the Chandrasekhar limit, which is the limit in mass beyond which a star is capable of forming a black hole, as "shuddering before the beautiful."
Because of the Laws of Spin and Statistics, we identify bosons as energy; bosons are gregarious, congregating together and trying to squeeze as many of themselves as possible into the same space, reinforcing one another, forming aggregates where one can hardly be told from the other, passing through one another as if the other were not there. Because of the Laws of Spin and Statistics, we identify fermions as matter; fermions are exclusive, pulled together by gravity, but collecting not into ultimately tiny packets, but into finite-sized chunks which grow ever larger as more of them congregate, which cannot be penetrated by any other such chunk. The bosons form the basis of all fields and forces; the fermions, that on which those forces and fields act.
BECs, or Bose-Einstein condensates, are a state of matter in which the atoms overall each are bosons; although they are made of fermions, electrons and quarks, they can behave gregariously as bosons do. This makes them curious amalgams of the qualities of both matter and energy, a sort of halfway state, and their quantum behavior intrudes into the macroscopic realm in a way impossible for most other materials. We are just discovering the things they can do; many interesting applications for these unusual states of matter will doubtless appear in coming years.
It is worth noting that when Ludwig Boltzmann worked out the laws of thermodynamics, he used spinless particles. Spinless particles are also what James Clerk Maxwell used for his work on thermodynamics, and so the statistics of spinless particles are sometimes called Maxwell-Boltzmann statistics. It was the realization that these statistics do not actually apply to real matter and energy that led to the creation of the fluctuation theorem, which has revolutionized quantum thermodynamics in the last few years and led to the first known laboratory demonstration of violations of the Second Law of Thermodynamics. Note, however, all you optimistic woos who might be reading this, that these violations can only occur over very small volumes, for very short times, and only at the expense of overall increase of entropy of the system. However, even such minor violations were considered impossible or so improbable as to be unduplicatable in the laboratory only a decade ago.
Last, but hardly least, the Laws of Spin and Statistics are why Star Wars' "Light Sabers" are so ridiculous. No weapon can be made from bosons; it will merely pass through another such weapon, or even through solid matter, without doing much. If you want to do real damage, you need exclusion; you need fermions. Which means you need matter.