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made, the reality of the particle’s position or state consists only of these probabilities. By measuring or observing the system, the observer causes<br />

the wave function to collapse and one distinct position or state to snap into place.<br />

In a letter to Schrödinger, Einstein gave a vivid thought experiment showing why all this discussion of wave functions and probabilities, and of<br />

particles that have no definite positions until observed, failed his test of completeness. He imagined two boxes, one of which we know contains a<br />

ball. As we prepare to look in one of the boxes, there is a 50 percent chance of the ball being there. After we look, there is either a 100 percent or a<br />

0 percent chance it is in there. But all along, in reality, the ball was in one of the boxes. Einstein wrote:<br />

I describe a state of affairs as follows: the probability is ½ that the ball is in the first box. Is that a complete description? no: A complete<br />

statement is: the ball is (or is not) in the first box. That is how the characterization of the state of affairs must appear in a complete description.<br />

yes: Before I open them, the ball is by no means in one of the two boxes. Being in a definite box comes about only when I lift the covers. 19<br />

Einstein clearly preferred the former explanation, a statement of his realism. He felt that there was something incomplete about the second<br />

answer, which was the way quantum mechanics explained things.<br />

Einstein’s argument is based on what appears to be common sense. However, sometimes what seems to make sense turns out not to be a<br />

good description of nature. Einstein realized this when he developed his relativity theory; he defied the accepted common sense of the time and<br />

forced us to change the way we think about nature. Quantum mechanics does something similar. It asserts that particles do not have a definite state<br />

except when observed, and two particles can be in an entangled state so that the observation of one determines a property of the other instantly. As<br />

soon as any observation is made, the system goes into a fixed state. 20<br />

Einstein never accepted this as a complete description of reality, and along these lines he proposed another thought experiment to Schrödinger<br />

a few weeks later, in early August 1935. It involved a situation in which quantum mechanics would assign only probabilities, even though common<br />

sense tells us that there is obviously an underlying reality that exists with certainty. Imagine a pile of gunpowder that, due to the instability of some<br />

particle, will combust at some point, Einstein said. The quantum mechanical equation for this situation “describes a sort of blend of not-yet and<br />

already-exploded systems.” But this is not “a real state of affairs,” Einstein said, “for in reality there is just no intermediary between exploded and<br />

not-exploded.” 21<br />

Schrödinger came up with a similar thought experiment—involving a soon-to-be-famous fictional feline rather than a pile of gunpowder—to show<br />

the weirdness inherent when the indeterminacy of the quantum realm interacts with our normal world of larger objects. “In a lengthy essay that I have<br />

just written, I give an example that is very similar to your exploding powder keg,” he told Einstein. 22<br />

In this essay, published that November, Schrödinger gave generous credit to Einstein and the EPR paper for “providing the impetus” for his<br />

argument. It poked at a core concept in quantum mechanics, namely that the timing of the emission of a particle from a decaying nucleus is<br />

indeterminate until it is actually observed. In the quantum world, a nucleus is in a “superposition,” meaning it exists simultaneously as being<br />

decayed and undecayed until it is observed, at which point its wave function collapses and it becomes either one or the other.<br />

This may be conceivable for the microscopic quantum realm, but it is baffling when one imagines the intersection between the quantum realm<br />

and our observable everyday world. So, Schrödinger asked in his thought experiment, when does the system stop being in a superposition<br />

incorporating both states and snap into being one reality?<br />

This question led to the precarious fate of an imaginary creature, which was destined to become immortal whether it was dead or alive, known as<br />

Schrödinger’s cat:<br />

One can even set up quite ridiculous cases. A cat is penned up in a steel chamber, along with the following device (which must be secured<br />

against direct interference by the cat): in a Geiger counter there is a tiny bit of radioactive substance, so small, that perhaps in the course of<br />

the hour one of the atoms decays, but also, with equal probability, perhaps none; if it happens, the counter tube discharges and through a relay<br />

releases a hammer which shatters a small flask of hydrocyanic acid. If one has left this entire system to itself for an hour, one would say that the<br />

cat still lives if meanwhile no atom has decayed. The psi-function of the entire system would express this by having in it the living and dead cat<br />

(pardon the expression) mixed or smeared out. 23<br />

Einstein was thrilled. “Your cat shows that we are in complete agreement concerning our assessment of the character of the current theory,” he<br />

wrote back. “A psi-function that contains the living as well as the dead cat just cannot be taken as a description of a real state of affairs.” 24<br />

The case of Schrödinger’s cat has spawned reams of responses that continue to pour forth with varying degrees of comprehensibility. Suffice it<br />

to say that in the Copenhagen interpretation of quantum mechanics, a system stops being a superposition of states and snaps into a single reality<br />

when it is observed, but there is no clear rule for what constitutes such an observation. Can the cat be an observer? A flea? A computer? A<br />

mechanical recording device? There’s no set answer. However, we do know that quantum effects generally are not observed in our everyday visible<br />

world, which includes cats and even fleas. So most adherents of quantum mechanics would not argue that Schrödinger’s cat is sitting in that box<br />

somehow being both dead and alive until the lid is opened. 25<br />

Einstein never lost faith in the ability of Schrödinger’s cat and his own gunpowder thought experiments of 1935 to expose the incompleteness of<br />

quantum mechanics. Nor has he received proper historical credit for helping give birth to that poor cat. In fact, he would later mistakenly give<br />

Schrödinger credit for both of the thought experiments in a letter that exposed the animal to being blown up rather than poisoned. “Contemporary<br />

physicists somehow believe that the quantum theory provides a description of reality, and even a complete description,” Einstein wrote<br />

Schrödinger in 1950.“This interpretation is, however, refuted most elegantly by your system of radioactive atom + Geiger counter + amplifier +<br />

charge of gunpowder + cat in a box, in which the psi-function of the system contains the cat both alive and blown to bits.” 26<br />

Einstein’s so-called mistakes, such as the cosmological constant he added to his gravitational field equations, often turned out to be more<br />

intriguing than other people’s successes. The same was true of his parries against Bohr and Heisenberg. The EPR paper would not succeed in<br />

showing that quantum mechanics was wrong. But it did eventually become clear that quantum mechanics was, as Einstein argued, incompatible<br />

with our commonsense understanding of locality—our aversion to spooky action at a distance. The odd thing is that Einstein, apparently, was far<br />

more right than he hoped to be.<br />

In the years since he came up with the EPR thought experiment, the idea of entanglement and spooky action at a distance—the quantum<br />

weirdness in which an observation of one particle can instantly affect another one far away—has increasingly become part of what experimental<br />

physicists study. In 1951, David Bohm, a brilliant assistant professor at Princeton, recast the EPR thought experiment so that it involved the<br />

opposite “spins” of two particles flying apart from an interaction. 27 In 1964, John Stewart Bell, who worked at the CERN nuclear research facility<br />

near Geneva, wrote a paper that proposed a way to conduct experiments based on this approach. 28

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