The Big Picture

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by Carroll, Sean M.


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  quantum system. If such a theory is true, it would have to be nonlocal—

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  parts of the system would have to directly interact with parts at other loca-

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  tions in space.

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  An even more radical approach is to simply deny the existence of an

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  underlying reality altogether. This would be an antirealist approach to

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  quantum mechanics, since it treats the theory as merely a bookkeeping de-

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  vice for predicting the outcomes of future experiments. If you ask an anti-

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  realist what aspect of the current universe that knowledge is about, they

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  will tell you that it’s not a sensible question to ask. There is, in this view, no

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  underlying “stuff” that is being described by quantum mechanics; all we are

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  ever allowed to talk about is the outcomes of experimental measurements.

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  Antirealism is a pretty dramatic step to take. It seems to have been ad-

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  vocated, however, by no less of an authority than Niels Bohr, the grandfa-

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  ther of quantum mechanics. His views were described as “There is no

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  quantum world. There is only an abstract physical description. It is wrong

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  to think that the task of physics is to find out how nature is. Physics con-

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  cerns what we can say about nature.”

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  Perhaps the biggest problem with antirealism is that it’s hard to see how

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  it could be a position that one holds with perfect consistency. It’s one thing

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  to say that our understanding of nature is incomplete; it’s another thing

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  entirely to say that there is no such thing as nature. For one thing, who is it

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  that’s doing the saying? Even Bohr, in the quote above, speaks of what we

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  can say “about nature.” That would seem to imply that there’s something

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  called “nature” that we can say things about.

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  Fortunately, we have not yet exhausted our possibilities. The simplest pos-

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  sibility is that the quantum wave function isn’t a bookkeeping device at all,

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  nor is it one of many kinds of quantum variables; the wave function simply

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  represents reality directly. Just as Newton or Laplace would have thought

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  of the world as a set of positions and velocities of particles, the modern

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  quantum theorist can think of the world as a wave function, full stop.

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  The difficulty with this robust brand of straightforward quantum real-

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  ism is the measurement problem. If everything is just wave function, what

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  makes states “collapse,” and why is the act of observation so important?

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  A resolution was suggested in the 1950s by a young physicist named

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  Hugh Everett III. He proposed that there is only one piece of quantum

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  ontology— the wave function— and only one way it ever evolves— via the

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  Schrödinger equation. There are no collapses, no fundamental division

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  between system and observer, no special role for observation at all. Everett

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  proclaimed that quantum mechanics fits perfectly comfortably into a de-

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  terministic Laplacian view of the world.

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  But if that’s right, why does it seem to us that wave functions collapse

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  when we observe them? The trick, in modern language, can be traced to a

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  feature of quantum mechanics called entanglement.

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  In classical mechanics, we can think of every different piece of the world

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  as having its own state. The Earth is moving around the sun with a particu-

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  lar position and velocity, and Mars has a position and velocity of its own.

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  Quantum mechanics tells a different story. There is not a wave function for

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  the Earth, another one for Mars, and so on through all of space. There is

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  only one wave function for the entire universe at once— what we call, with

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  no hint of modesty, the “wave function of the universe.”

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  A wave function is simply a number we assign to every possible measure-

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  ment outcome, like the position of a particle, such that the number tells us

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  the probability of obtaining that outcome. The probability is given by the

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  wave function squared; that’s the famous Born rule, after German physicist

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  Max Born. So the wave function of the universe assigns a number to every

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  possible way that objects in the universe could be distributed through

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  space. There’s one number for “the Earth is here, and Mars is over there,”

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  and another number for “the Earth is at this other place, and Mars is yet

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  somewhere else,” and so on.

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  The state of Earth can therefore be entangled with the state of Mars. For

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  big macroscopic things like planets this possibility isn’t realized in a de-

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  monstrable way, but for tiny things like elementary particles it happens all

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  the time. Say we have two particles, Alice and Bob, each of which could be

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  spinning either clockwise or counterclockwise. The wave function of the

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  universe could assign a 50 percent probability to Alice spinning clockwise

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  and Bob counterclockwise, and another 50 percent to Alice spinning coun-

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  terclockwise and Bob clockwise. We have no idea what answer we would

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  get were we to measure the spin of either particle; but we know that once

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  we measure one of them, the other is definitely spinning the other way.

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  They are entangled with each other.

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  Everett says that we should take the formalism of quantum mechanics

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  at face value. Not only is the system you’re going to observe described by a

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  wave function, but you are described by a wave function yourself. That

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  means that you can be in a superposition. When you make a measurement

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  of a particle to see whether it’s spinning clockwise or counterclockwise,r />
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  Everett suggests, the wave function doesn’t collapse into one possibility or

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  the other. It evolves smoothly into an entangled superposition, part of

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  which has “the particle is spinning clockwise” and “you saw the particle

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  spinning clockwise,” while the other of which has “the particle is spinning

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  counterclockwise” and “you saw the particle spinning counterclockwise.”

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  Both parts of the superposition actually exist, and they continue to exist

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  and evolve as the Schrödinger equation demands.

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  At last, then, we have a candidate for a final answer to the critical onto-

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  logical question “What is the world, really?” It is a quantum wave function.

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  At least until a better theory comes along.

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  Everett’s bare- bones approach to quantum mechanics— just wave functions

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  and smooth evolution, no new variables or unpredictable collapses or deni-

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  als of objective reality— has been dubbed the Many- Worlds Interpretation.

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  The two parts of the wave function of the universe, one in which you saw

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  the particle spinning clockwise and the other in which you saw it spinning

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  counterclockwise, subsequently evolve completely independently of each

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  other. There is no future communication or interference between them.

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  That’s because you and the particle become entangled with the rest of

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  the universe, in a process known as decoherence. The different parts of the

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  wave function are different “branches,” so it’s convenient to say that they

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  describe different worlds. (There’s still one “world” in the sense of “the

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  natural world,” described by the wave function of the universe, but there are

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  many different branches of that wave function, and they evolve indepen-

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  dently, so we call them “worlds.” Our language hasn’t yet caught up to our

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  physics.)

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  There’s a lot to love about the Everett/ Many- Worlds approach to quan-

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  tum mechanics. It is lean and mean, ontologically speaking; there’s just the

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  quantum state and its single evolution equation. It’s perfectly deterministic,

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  even though individual observers can’t tell which world they are in before

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  they actually look at it, so there is necessarily some probabilistic component

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  when it comes to people making predictions. And there’s no difficulty in

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  explaining things like the measurement process, or any need to invoke

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  conscious observers to carry out such measurements. Everything is just a

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  wave function, and all wave functions evolve in the same way.

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  There are, of course, an awful lot of universes.

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  Many people object to Many- Worlds because they simply don’t like the

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  idea of all of those universes out there. Especially unobservable universes—

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  the theory predicts them, but there’s no practical way of ever seeing them.

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  This is not a very thoughtful objection. If our best theory predicts that

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  something is true, we should place a relatively high Bayesian credence that

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  it actually is true, until a better theory comes along. If you have some vis-

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  ceral or a priori bad feeling about multiple universes, then by all means

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  work on better formulations of quantum mechanics. But a bad feeling is

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  not a principled stance.

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  The secret to making your peace with Many- Worlds is to appreciate that

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  the approach doesn’t start with the formalism of quantum mechanics and

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  add in a preposterously big multiverse. All those other universes are already

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  there, at least potentially, in the formalism. Quantum mechanics describes

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  individual objects as being in superpositions of different measurement out-

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  comes. The wave function of the universe automatically includes the pos-

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  sibility that the whole universe is in such a superposition, which we then

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  choose to talk about as “multiple worlds.” It’s all the other versions of quan-

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  tum mechanics that have to work to get rid of the extra worlds— by chang-

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  ing the dynamics, or adding in new physical variables, or denying the

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  existence of reality itself. But you gain nothing in explanatory or predictive

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  power, and have unnecessarily made a simple framework more elaborate—

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  at least as Everettians see things.

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  Which isn’t to say that there aren’t very good reasons to be concerned

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  about Everettian quantum mechanics. According to Everett, the branching

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  of the wave function into different parallel worlds isn’t an objective feature;

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  it’s simply a convenient way of talking about the underlying reality. But

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  what exactly determines the best way of drawing the line between uni-

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  verses? Why do we see the emergence of a reality that is well approximated

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  by the rules of classical mechanics? These are perfectly respectable

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  questions— though ones that seem quite answerable to partisans of Many-

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  Worlds.

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  There are two important things to take away from this discussion, as far

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  as the big picture is concerned. One is that, while we don’t have a finished

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  understanding of quantum mechanics at a fundamental level, there is noth-

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  ing we know about it that necessarily invalidates determinism (the future

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  follows uniquely from the present), realism (there is an objective real world),

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  or physicalism (the world is purely physical). All of these features of the

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  Newtonian/ Laplacian clockwork universe can easily still hold true in

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  quantum mechanics— but we don’t know for sure.

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  The other important takeaway is a feature common to all interpreta-

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  tions of quantum mechanics: what we see when we look at the world is

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  quite different from how we des
cribe the world when we’re not looking at

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  it. As human knowledge has progressed over the centuries, we have occa-

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  sionally been forced to dramatically rearrange our planets of belief to ac-

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  commodate a new picture of the physical universe, and quantum mechanics

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  certainly qualifies as that. In a sense it is the ultimate unification: not only

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  does the deepest layer of reality not consist of things like “oceans” and

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  “mountains”; it doesn’t even consist of things like “electrons” and “pho-

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  tons.” It’s just the quantum wave function. Everything else is a convenient

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  way of talking.

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  The Core Theory

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  Quantum mechanics is, as far as we currently know, the way the

  universe works. But quantum mechanics isn’t a specific theory of

  the world; it’s a framework within which particular theories can

  be constructed. Just as classical mechanics includes the theory

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  of planets moving around the sun, or the theory of electricity and magne-

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  tism, or even Einstein’s theory of general relativity, there are an enormous

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  number of particular physical models that qualify as “ quantum-

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  mechanical.” If we want to know how the world really works, we need to

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  ask, “The quantum- mechanical theory of what?”

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  Your first guess might be “particles and forces.” When we talk about

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  atoms, for example, the central nucleus is a collection of particles called

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  protons and neutrons, while orbiting around the nucleus are particles called 26

  electrons. The protons and neutrons are bound to each other by a force (the

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  nuclear force), and the electrons are bound to the nucleus by a different

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  force (electromagnetism), and everything pulls toward everything else be-

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  cause of yet another force (gravitation). Particles and forces are reasonable

 

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