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  • - In the 1930s, Albert Einstein was upset with quantum mechanics. He proposed a thought

  • experiment where, according to the theory, an event at one point in the universe could

  • instantaneously affect another event arbitrarily far away. He called this "spooky action at

  • a distance" because he thought it was absurd. It seemed to imply faster than light communication,

  • something his theory of relativity ruled out. But nowadays, we can do this experiment, and

  • what we find is, indeed, spooky. But in order to understand it, we must first understand

  • spin. All fundamental particles have a property called spin. No, they're not actually spinning,

  • but the analogy is appropriate. They have angular momentum, and they have an orientation

  • in space. Now, we can measure the spin of a particle, but we have to choose the direction

  • in which to measure it, and this measurement can have only one of two outcomes. Either

  • the particle’s spin is aligned with the direction of measurement, which we'll call

  • spin up, or, it is opposite the measurement, which we'll call spin down. Now, what happens

  • if the particle spin is vertical, but we measure it's spin horizontally? Well then, it has

  • a 50% chance of being spin up, and a 50% chance of being spin down, and after the measurement,

  • the particle maintains this spin, so measuring its spin actually changes the spin of the

  • particle. What if we measure spin at an angle 60 degrees from the vertical? Well now, since

  • the spin of the particle is more aligned to this measurement, it will be spin up 3/4 of

  • the time, and spin down 1/4 of the time. The probability depends on the square of the cosine

  • of half the angle. Now, an experiment like the one Einstein proposed can be performed

  • using two of these particles, but they must be prepared in a particular way. For example,

  • formed spontaneously out of energy. Now, since the total angular momentum of the universe

  • must stay constant, you know that if one particle is measured to have spin up, the other, measured

  • in the same direction, must have spin down. I should point out, it's only if the two particles

  • are measured in the same direction that their spins must be opposite. Now here's where things

  • start to get a little weird. You might imagine that each particle is created with a definite

  • well-defined spin, but that won't work, and here's why. Imagine their spins were vertical

  • and opposite. Now, if they're both measured in a horizontal direction, each one has a

  • 50/50 chance of being spin up. So, there's actually a 50% chance that both measurements

  • will yield the same spin outcome, and this would violate the law of conservation of angular

  • momentum. According to quantum mechanics, these particles don't have a well-defined

  • spin at all. They are entangled, which means their spin is simply opposite that of the

  • other particle. So, when one particle is measured, and its spin determined, you immediately know

  • what the same measurement of the other particle will be. This has been rigorously and repeatedly

  • tested experimentally. It doesn't matter at which angle the detectors are set, or how

  • far apart they are, they always measure opposite spins. Now just stop for a minute, and think

  • about how crazy this is. Both particles have undefined spins, and then you measure one,

  • and immediately you know the spin of the other particle, which could be light-years away.

  • It's as though the choice of the first measurement has influenced the result of the second faster

  • than the speed of light, which is, indeed, how some theorists interpret the result. But

  • not Einstein. Einstein was really bothered by this. He preferred an alternate explanation,

  • that all along the particles contained hidden information about which spin they would have

  • if measured in any direction. It's just that we didn't know this information until we measured

  • them. Now, since that information was within the particles from the moment they formed

  • at the same point in space, no signal would ever have to travel between the two particles

  • faster than light. Now, for a time, scientists accepted this view that there were just some

  • things about the particles we couldn't know before we measured them. But then along came

  • John Bell with a way to test this idea. This experiment can determine whether the particles

  • contain hidden information all along, or not, and this is how it works. There are two spin

  • detectors, each capable of measuring spin in one of three directions. These measurement

  • directions will be selected randomly, and independent of each other. Now, pairs of entangled

  • particles will be sent to the two detectors, and we record whether the measured spins are

  • the same, both up, or both down, or different. We'll repeat this procedure over and over,

  • randomly varying those measurement directions, to find the percentage of the time the two

  • detectors give different results, and this is the key, because that percentage depends

  • on whether the particles contain hidden information all along, or if they don't. Now, to see why

  • this is the case, let's calculate the expected frequency of different readings if the particles

  • do contain hidden information. Now, you can think of this hidden information like a secret

  • plan the particles agree to, and the only criterion that plan must satisfy is that if

  • the particles are ever measured in the same direction, they must give opposite spins.

  • So, for example, one plan could be that one particle will give spin up for every measurement

  • direction, and its pair would give spin down for every measurement direction. Or another

  • plan, plan two, could be that one particle could give spin up for the first direction,

  • spin down for the second direction, and spin up for the third direction, whereas its partner

  • would give spin down for the first direction, spin up for the second direction, and spin

  • down for the third direction. All other plans are mathematically equivalent, so we can work

  • out the expected frequency of different results using these two plans. Here, I'm visually

  • representing the particles by their plans, their hidden information. With plan one, the

  • results will obviously be different 100% of the time. It doesn't matter which measurement

  • directions are selected, but it does for particles using the second plan. For example, if both

  • detectors measure in the first direction, particle A gives spin up, while particle B

  • gives spin down. The results are different. But if instead, detector B measured in the

  • second direction, the result would be spin up, so the spins are the same. We can continue

  • doing this for all the possible measurement combinations, and what we find, is the results

  • are different five out of nine times. So, using the second plan, the results should

  • be different 5/9 of the time, and using the first plan, the results should be different

  • 100% of the time, so overall, if the particles contain hidden information, you should see

  • different results more than 5/9 of the time. So what do we actually see in experiment?

  • Well, the results are different only 50% of the time. It doesn't work, so the experiment

  • rules out the idea that all along, these particles contain hidden information about which spin

  • they will give in the different directions. So, how does quantum mechanics account for

  • this result? Well, let's imagine detector A measures spin in the first direction, and

  • the result is spin up. Now, immediately you know that the other particle is spin down

  • if measured in the first direction, which would happen randomly 1/3 of the time. However,

  • if particle B is measured in one of the other two directions, it makes an angle of 60 degrees

  • with these measurement directions, and recall, from the beginning of this video, the resulting

  • measurement should be spin up 3/4 of the time. Since these measurement directions will be

  • randomly selected 2/3 of the time, particle B will give spin up 2/3 times 3/4 equals half

  • of the time. So both detectors should give the same results half of the time, and different

  • results half of the time, which is exactly what we see in the experiment. So quantum

  • mechanics works. But there is debate over how to interpret these results. Some physicists

  • see them as evidence that there is no hidden information in quantum particles, and it only

  • makes sense to talk about spins once they've been measured, whereas other physicists believe

  • that entangled particles can signal each other faster than light to update their hidden information

  • when one is measured. So, does this mean that we can use entangled particles to communicate

  • faster than light? Well, everyone agrees that we can't. And that is because the results

  • that you find at either detector are random. It doesn't matter which measurement direction

  • you select, or what's happening at the other detector, there's a 50/50 probability of obtaining

  • spin up or spin down. Only if these observers later met up and compared notebooks, would

  • they realize that when they selected the same direction, they always got opposite spins.

  • Both sets of data would be random, just the opposite random from the other observer. That

  • is, indeed, spooky, but it doesn't allow for the communication, the sending of information

  • from one point to another, faster than light, so it doesn't violate the theory of relativity.

  • And that, at the very least, would make Einstein happy.

- In the 1930s, Albert Einstein was upset with quantum mechanics. He proposed a thought

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