On 10/16/2019 2:50 PM, John Clark wrote:
On Wed, Oct 16, 2019 at 4:49 PM 'Brent Meeker'  <[email protected] <mailto:[email protected]>> wrote:

    /> I thought you read Carroll's book.  His example shows in what
    sense you can erase the information after the photon has hit the
    screen./


If you wait to erase the which way information until after the photon has hit the screen then the experiment would be much easier to perform, but the results of it are obvious and rather dull, you would see interference bands because there would be ambiguity over which slit the photon went through.

Here's Carroll's description from his blog...which is more interesting that just erase or not erase:

When we measured the recording spin in the vertical direction, the result we obtained was entangled with a definite path for the traveling electron: [↑] was entangled with (*L*), and [↓] was entangled with (*R*). So by performing that measurement, we knew that the electron had traveled through one slit or the other. But now when we measure the recording spin along the horizontal axis, that’s no longer true. After we do each measurement, we are again in a branch of the wave function where the traveling electron passes through both slits. If we measured spin-left, the traveling electron passing through the right slit picks up a minus sign in its contribution to the wave function, but that’s just math.

By choosing to do our measurement in this way, we have erased the information about which slit the electron went through. This is therefore known as a “quantum eraser experiment.” This erasure doesn’t affect the overall distribution of flashes on the detector screen. It remains smooth and interference-free.

But we not only have the overall distribution of electrons hitting the detector screen; for each impact we know whether the recording electron was measured as spin-left or spin- right. So, instructs our professor with a flourish, let’s go to our computers and separate the flashes on the detector screen into these two groups — those that are associated with spin- left recording electrons, and those that are associated with spin-right. What do we see now?

Interestingly, the interference pattern reappears. The traveling electrons associated with spin-left recording electrons form an interference pattern, as do the ones associated with spin-right. (Remember that we don’t see the pattern all at once, it appears gradually as we detect many individual flashes.) But the two interference patterns are slightly shifted from each other, so that the peaks in one match up with the valleys in the other. There was secretly interference hidden in what initially looked like a featureless smudge.

Adapted fromWikipedia <https://en.wikipedia.org/wiki/Delayed-choice_quantum_eraser>

In retrospect this isn’t that surprising. From looking at how our quantum state Ψ was written with respect to the spin-left and -right recording electrons, each measurement was entangled with a traveling electron going through both slits, so of course it could interfere. And that innocent-seeming minus sign shifted one of the patterns just a bit, so that when combined together the two patterns could add up to a smooth distribution.

You professor seems more amazed by this than you are. “Don’t you see,” she exclaims excitedly. “If we didn’t measure the recording photons at all, or if we measured them along the vertical axis, there was no interference anywhere. But if we measured them along the horizontal axis, there secretly was interference, which we could discover by separating out what happens at the screen when the recording spin was left or right.”

You and your classmates nod their heads, cautiously but with some degree of confusion.

“Think about what that means! The choice about whether to measure our recording spins vertically or horizontally could have been made long after the traveling photons splashed on the recording screen. As long as we stored our recording spins carefully and protected them from becoming entangled with the environment, we could have delayed that choice until years later.”

Sure, the class mumbles to themselves. That sounds right.

“But interference only happens when the traveling electron goes through both slits, and the smooth distribution happens when it goes through only one slit. That decision — go through both slits, or just through one — happens long before we measure the recording electrons! So obviously, our choice to measure them horizontally rather than vertically had to/send a signal backward in time/to tell the traveling electrons to go through both slits rather than just one!”

After a short, befuddled pause, the class erupts with objections. Decisions? Backwards in time? What are we talking about? The electron doesn’t make a choice to travel through one slit or the other. Its wave function (and that of whatever it’s entangled with) evolves according to the Schrödinger equation, just like always. The electron doesn’t make choices, it unambiguously goes through both slits, but it becomes entangled along the way. By measuring the recording photons along different directions, we can pick out different parts of that entangled wave function, some of which exhibit interference and others do not. Nothing really went backwards in time. It’s kind of a cool result, but it’s not like we’re building a frickin’ time machine here.

The more interesting thing to do is to make the decision on whether to erase the which way information or not to erase it until after the photon passes the slits but before it hits the screen; it turns out that if you decide to not erase the information then you don't get a interference pattern, but if you decide to erase it then you do get a interference pattern. And that exparament has already been performed and yes the results are weird because the decision to erase or not to erase the information was made long after, even billions of years after, the photon passed the slits so you might think it would make no difference as far as the picture on the screen is concerned, but it does.

And I think all of this is super interesting, *_but_* it is *_not_* the experiment Deutsch proposed. And you still haven't told me what your best guess is that Deutsch will find when he develops that all important photographic plate; will he see interference bands or no interference bands? I've already told you how I'd place my money.

I haven't because I'd have to re-read Deutsch's thought experiment, I don't remember how he proposed to erase the which-way.

Brent

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