Counterfeit
Suppose you have a $100 bill, and a molecule-for-molecule counterfeit of one. You know which is which.
You put both into a black box, and spin and shake it.
At some point, it becomes absolutely undecidable which is real, and which is the counterfeit. That knowledge is lost to the universe.
Open the box. What is the status of the 2 hundred dollar bills?
* Is one real and one fake, and this truth is unknowable?
* Or are they both in some kind of half-real/half-fake state?
* Or are they both real?
* Or?
You put both into a black box, and spin and shake it.
At some point, it becomes absolutely undecidable which is real, and which is the counterfeit. That knowledge is lost to the universe.
Open the box. What is the status of the 2 hundred dollar bills?
* Is one real and one fake, and this truth is unknowable?
* Or are they both in some kind of half-real/half-fake state?
* Or are they both real?
* Or?
Comments (24)
The physical assumptions underlying this thought experiment could be questioned. For example, the no-cloning theorem says that it is impossible to make an exact copy of a physical system. And the no-hiding theorem says that information is never destroyed.
That aside, it's of course possible for a human being to lose track of which bill is the real one. That just means that the status of the bills is unknown, it doesn't change the fact that one is real and the other is counterfeit (per the original designation).
It doesn't have to be an identical copy. Merely close enough so that for any conceivable test of genuineness that the real dollar passes, the counterfeit passes as well.
I'm having a hard time wrapping my head around the no hiding theorem. Right now I'm thinking of a 10 digit number. I'm not repeating it, and there's no way I will remember it in 5 minutes. Could a sufficiently clever alien, arriving on a venus like earth 10 million years from now, retrieve it?
Would you answer the same way if the no hiding theorem turned out to be false? Or true, but information can still be irretrievably, in principle as well as practice, lost and inaccessible?
I think the no hiding theorem is more about quantum information than about memory.I think it is
totally possible to retrieve your memory if it is stored in the form of waves.
Presumably the authentic bill is issued by a central bank that keeps records of the total legal tender in circulation. So that information exists. The knowledge isn't lost to the universe.
Then so far as the central bank is concerned, it just has to cut up one of the two bills.
Which one doesn't matter. But what does matter is that one is erased so that the records are kept right.
A better example would be a promissory note assigning a fixed amount ($100) worth from one person to another.
If it's molecularly similar there's no difference and only 'counterfeit' due to the fact it was not legally printed from a government-backed institution. The reason I say all this is because of the serial number. It's only valid for one note. Granted if you pass a bill with a duplicate or erroneous (random) serial number to some random clerk or individual it's not like they're going to or even can check to see if it's valid and alert that someone needs to be investigated for financial crimes.
If we're ever in a scenario where we can molecularly replicate something exactly, a paper note would be the last thing to do it with.
Contradiction! If the two $100 bills were indistinguishable right from the beginning then how would you know whether:
1. Both are real
2. One is real and the other counterfeit
3. Both are counterfeit
? :chin:
In fact, as far as you're concerned all three possibilities are true.
If it is that exact of a copy then it shouldn't be considered a counterfeit and is there any other distinguishing feature you haven't mentioned.
In principle, yes. For example, suppose the Earth's system were isolated with respect to the alien. Since no information has been lost, the alien could perform a physical transformation on the Earth's system that, in effect, runs the laws of physics in reverse until it's back to you thinking of the number. That process would be akin to unscrambling a scrambled egg.
Quoting hypericin
I would answer the same way if the information were merely irretrievable, since the information does still exist. But if the information does not exist, then there would be no basis for a distinction between the real and counterfeit bills.
As it happens, exactly this issue arises in quantum mechanics - see the Hong–Ou–Mandel effect. Suppose the photon coming in from above represents the real bill and the photon coming in from below represents the counterfeit bill (see the four possibilities diagram). State 2 has both photons transmitting, while state 3 has both photons reflecting. In the experiment, states 2 and 3 destructively interfere (i.e., are not experimentally observed) which means that there is no "which-way" information distinguishing those two states. So for states 1 and 4 that are observed, there is no longer any basis for regarding one photon as representing the real bill and the other photon as representing the counterfeit bill - that information does not exist. There are simply two photons that have a shared history.
Yes. Which is to say, there's no difference between the bills that makes a difference. ;-)
But if it were irretrievable, from our perspective the situation is identical with that where it doesn't exist.
Can you tell them apart before you put them in the box?
No.
Can you tell them apart after you put them in the box?
No
In my humble opinion, there was no knowledge to begin with. So, no knowledge is lost.
:chin: However, note that after shaking the box, you're relying on information content of the bills themselves and nothing else to tell them apart but that information, as I said, never really existed.
For all practical purposes, sure. But I think the conceptual distinction remains. Before the bills go in the box, you know which one is real and which one is the counterfeit. After the bills go in the box, you lose track of them, but they still have a definite history as their positions change over time.
So, in effect, all that has changed before and after is your knowledge of that definite history.
Whether something can be known (or retrievable) or not depends on what is being done. If a coin is flipped inside the event horizon of a black hole (and subsequently destroyed), then it is going to be essentially impossible for external observers to retrieve the result. On the other hand, if you send a photon into a suitably configured Mach-Zehnder interferometer, it can be predicted with certainty which detector the photon will arrive at (despite being impossible to predict using classical theory).
In both cases, quantum information is conserved. Here's a PBS Space Time video on this - Why Quantum Information is Never Destroyed. The idea of quantum computing, then, is to exploit the special characteristics of quantum information (i.e., qubits) to solve problems that are beyond the capabilities of classical computers.
Quoting tim wood
The way I would put it is that information about the stone hitting the water is exhibited in the ocean itself. We can see it in the ripple. Of course there is a lot that we don't see and measure, and the ripple soon disappears. But that information is nonetheless retained in the environment which is, in principle, measurable.
Quoting tim wood
In terms of the no-hiding theorem, if a system is randomized, information about the randomization operation will be stored in the environment external to the system. That information can then be used to perfectly reconstruct the original system. Here's an experiment demonstrating this:
Quoting Quantum no-hiding theorem experimentally confirmed for first time
Conservation of information also applies in classical physics. Here's a couple of snippets from Leonard Susskind's lectures on statistical mechanics and classical mechanics (videos available on Youtube):
Quoting Statistical Mechanics - Entropy and conservation of information - Susskind
Quoting Classical Mechanics - Liouville’s theorem - Susskind
To give an example, consider a simple system with six states, like the sides of a die. The dynamical laws in this system for each time step are:
1 -> 2 -> 3 -> 4 -> 5 -> 6 -> 1
Information is conserved. For any given state, the next state and the previous state can be predicted. Whereas in the following system, information is not conserved since the state prior to state 3 can't be predicted.
1 -> 3 <- 2
Quoting tim wood
Information (or state) is an abstraction of physical systems. Quantum information is just a different abstraction than we're used to with classical information. A classical bit is just a 0 or a 1. Whereas a qubit is a linear combination of 0 and 1 that, when measured, collapses to a 0 or a 1. That seems like information has been erased. But the lost information has simply moved elsewhere (e.g., to an ancilla qubit or heat in the environment).
:up:
Quoting tim wood
Be careful not to reify information. Consider a coin that has landed tails-up on a table. The state of the coin (tails) is not itself a system, it's the form of the system in a specific context (where form is the linguistic root of information).
Quoting tim wood
It depends. For the stone-kicking question, perhaps the whole atmosphere (or even light cone) is required. Whereas the question of whether it rained earlier today could be answered from more easily accessible evidence.
Information is conserved in both cases and accessible in principle, if not in practice.
Consider again the no-hiding experiment referenced earlier where the system was randomized via a bleaching process. The original state of the system was recoverable from the ancilla qubits. But if that information had instead leaked into the external environment, then it would not be recoverable by present technology, but that information would still be somewhere.
Quoting tim wood
I'm not sure I understand your objection. But let's apply your comments to the six-state die system that I presented in the previous post (which cycles from 1 to 6). Given the rules of that system and a current state (e.g., 3), then the previous state is necessarily implied (i.e., 2). I don't see how a meta-state arises here.
Been watching Good Girls, ? :)