I Minimal vs Instrumental vs Ensemble

  • #51
I see the difference, and that difference is crucial. For the single system the state (statistical operator) represents a preparation procedure. Concerning the properties, i.e., the values of observables, of this state it only describes the statistics for the outcome of measurements for an ensemble of equally and independently prepared systems.
 
Physics news on Phys.org
  • #52
vanhees71 said:
... For the single system the state (statistical operator) represents a preparation procedure. ...
Not in his preferred interpretation. Or can you quote him saying exactly this?
 
  • #53
vanhees71 said:
One should also note that physics is not so much about "text exegesis", but about formulating clear concepts.
That's a very appealing statement, thanks. Of course it will get you into trouble. :oldbiggrin:
 
  • #54
martinbn said:
Not in his preferred interpretation. Or can you quote him saying exactly this?
I quoted him above in #49. The scan is from Ballentine's famous RMP paper where he explains the minimal statistical interpretation in detail:

L. E. Ballentine, The Statistical Interpretation of Quantum
Mechanics, Rev. Mod. Phys. 42, 358 (1970),
https://doi.org/10.1103/RevModPhys.42.358
 
  • #55
vanhees71 said:
I quoted him above in #49. The scan is from Ballentine's famous RMP paper where he explains the minimal statistical interpretation in detail:

L. E. Ballentine, The Statistical Interpretation of Quantum
Mechanics, Rev. Mod. Phys. 42, 358 (1970),
https://doi.org/10.1103/RevModPhys.42.358
Yes, and he clearly says that the state represents an ensemble not an individual system!!!!!!!!!!!
 
  • #56
Yes, but he says both! Please read the quoted text above carefully again. The first sentence says:

"We see a quantum state is a mathematical representation of the result of a certain preparation procedure."
 
  • #57
vanhees71 said:
Yes, but he says both! Please read the quoted text above carefully again. The first sentence says:

"We see a quantum state is a mathematical representation of the result of a certain preparation procedure."
But this doesn't say that the state is of an individual system. The preparation procedure produces many systems. And the state describes the ensemble, not the individuals. I think you need to read it carefully.
 
  • #58
vanhees71 said:
Yes, but he says both! Please read the quoted text above carefully again. The first sentence says:

"We see a quantum state is a mathematical representation of the result of a certain preparation procedure."
You're going to hate this: What do you make of the distinction between a preparation procedure, and the result of a preparation procedure?

Consider this logic:
- The state represents the result of a preparation procedure
- A single system, a statistical sample, and an infinite ensemble are all hypothetical results of a preparation procedure
- Quantum theory only makes direct statements about infinite ensembles
- Therefore: The state represents an infinite ensemble, the result of a prepartion procedure
 
  • Like
Likes gentzen and martinbn
  • #59
vanhees71 said:
I'd not make the issue more complicated than it is. I call an ensemble ensemble also when it's in fact a statistical sample of a real-world experiment in the lab. Anybody knows what's meant. One must be pedantic with the language at other places, where there's really a lot of confusion caused by sloppy language. In this forum you can observe this: the words getting almost unusable since there's no clear use of them in the foundation community are not "ensemble" but rather "local" and "nonlocal" ;-)).
I don't object to the use of a phrase like "finite ensemble", but my understanding is the "ensemble" in ensemble interpretations is necessarily infinite. Ensemble interpretations attempt to overcome apparent ambiguities when discussing individual systems, and a statistical sample is still, in a sense, an individual system (e.g. see this post of mine). Any statistical sample/finite ensemble falls back into the trappings of quantum theories of individual systems.
 
  • #60
Morbert said:
Any statistical sample/finite ensemble falls back into the trappings of quantum theories of individual systems.
But maybe the trappings of ... individual systems are not so bad overall, as long one is sufficiently careful to apply "good taste":
gentzen said:
Now I admit that "good taste" allows to relax those "rules" significantly in practice. But the idealized description should still be the one explained above. It is simply too easy to fool oneself with statistics, not least because our human intuition is not very good in that domain.
 
  • #61
gentzen said:
you must associate a single system with a state
PeterDonis said:
In the minimal statistical interpretation, no, you don't do this. States do not describe single systems in this interpretation. They either describe abstract ensembles, or they describe preparation procedures.
Wait, I just see that you quoted from a very long sentence of mine here:
gentzen said:
If you look at SEI from an operational verification perspective, then yes, you must associate a single system with a state before you know the results of the non-preparation measurements.
OK, I see that my sentences seem to be much too long. I will try to work on it. For me, the meaning of the quoted part changed significantly by leaving out the "before you know" part. And stripping away an "if ... then" part in general also risks to change meaning. However, I would also have stripped it away in this case, because it didn't impact the meaning.
 
  • #62
The preparation procedure prepares each single system, forming together the ensemble. You cannot prepare an ensemble if you cannot prepare individual system independently. The state preparation, however, does not determine all properties (i.e., the values of all observables) of the single system, and thus its meaning concerning the properties refers to the statistical properties for the outcome of measurements and thus refers to the ensemble. The important point is this distinction between preparation (referring to prerparation procedures for single systems) and observation (referring to statistical properties of the corresponding ensembles of equally prepared systems).
 
  • #63
vanhees71 said:
observation (referring to statistical properties of the corresponding ensembles of equally prepared systems)
maybe not important, but this parenthetical clarification is not helpful for me
 
  • #64
What is not helpful? I tried to explain what I mean when I say a state represents a preparation procedure for a single system and at the same time describes the statistical properties for the outcomes of measurements on an ensemble of equally so prepared systems.
 
  • #65
vanhees71 said:
What is not helpful? I tried to explain what I mean when I say a state represents a preparation procedure for a single system and at the same time describes the statistical properties for the outcomes of measurements on an ensemble of equally so prepared systems.
The description of a state and a preparation procedure was helpful. But the text in the parenthesis behind the word "observation" doesn't make sense to me.
 
  • #66
vanhees71 said:
Sigh. Do I really have to copy the parts from the texts I quoted.
No, you just have to read what they actually say instead of what you would like them to say.
 
  • #67
vanhees71 said:
The preparation procedure prepares each single system, forming together the ensemble.
That's not what Ballentine says. Ballentine says the ensemble is not the actual group of actual systems that are prepared by some preparation procedure. It is the abstract set of an infinite number of abstract systems that could be prepared by that preparation procedure.
 
  • Like
Likes bhobba and vanhees71
  • #68
Yes, that's the theoretical formulation, but in practice you must work with finite samples and do a corresponding statistical analysis to ensure that the predicted probabilities agree with the measured "frequencies". Practice shows that in the here discussed experiments, which probe the foundations of QT concerning entanglement, violation of Bell's inequalities, etc. this can be done with FAPP arbitrarily high accuracy. That together with the fact that also all other considered loopholes are closed (sometimes even in one and the same experiment) makes me believe that the distinction between finite samples and the infinite theoretical ensembles are not at the heart of the interpretational problems.
 
  • #69
vanhees71 said:
Yes, that's the theoretical formulation, but in practice you must work with finite samples and do a corresponding statistical analysis to ensure that the predicted probabilities agree with the measured "frequencies". Practice shows that in the here discussed experiments, which probe the foundations of QT concerning entanglement, violation of Bell's inequalities, etc. this can be done with FAPP arbitrarily high accuracy. That together with the fact that also all other considered loopholes are closed (sometimes even in one and the same experiment) makes me believe that the distinction between finite samples and the infinite theoretical ensembles are not at the heart of the interpretational problems.
This is unrelated. You were making claims about Ballentine's interpretation, which were wrong.
 
  • Like
Likes physika and PeterDonis
  • #70
I quoted Ballentine verbatim. Where can this be wrong? Here it is again from the RMP by Ballentine:

Untitled.png


It's an ensemble of single electrons being prepared by a procedure (to be specified for each state). So why do you claim it's wrong?
 
  • #71
vanhees71 said:
I quoted Ballentine verbatim. Where can this be wrong? Here it is again from the RMP by Ballentine:

View attachment 339207

It's an ensemble of single electrons being prepared by a procedure (to be specified for each state). So why do you claim it's wrong?
The quote is not wrong. Your statements are. You write "for a single elctron the state represents". Ballentine clearly says that the state represents the infinite abstract ensemble. You are wrong when you claim that Ballentine says what you say. He does not. Thr two of you use different interpretations. Yours is a Copenhagen interpretation in the way Bohr uses it.
 
  • Like
Likes weirdoguy and PeterDonis
  • #72
martinbn said:
Yours is a Copenhagen interpretation in the way Bohr uses it.
No, vanhees71's interpretation is not a Copenhagen interpretation, independent of whether he adheres exactly to Ballentine or not.
 
  • #73
But he says that the preparation procedure refers to a single electron. A bit later he even emphasizes that the so defined ensembles are different from preparing a bunch of electrons at once. I think it's pretty clear that the preparation procedure must relate to single electrons, if you want to strictly define an ensemble of "equally prepared single electrons", and as far as I understand him Ballentine precisely states this. The statistical interpretation is anyway very close to Copenhagen a la Bohr. Here's the precise quote from Ballentine:

Untitled2.png

Again in I the preparation procedure refers to single systems. Concerning the properties of the system described by the so prepared state it provides only the statistical properties and thus only refers to ensembles of such prepared single systems.
 
  • #74
gentzen said:
No, vanhees71's interpretation is not a Copenhagen interpretation, independent of whether he adheres exactly to Ballentine or not.
Why not? Where does he differ?
 
  • #75
vanhees71 said:
But he says that the preparation procedure refers to a single electron. A bit later he even emphasizes that the so defined ensembles are different from preparing a bunch of electrons at once. I think it's pretty clear that the preparation procedure must relate to single electrons, if you want to strictly define an ensemble of "equally prepared single electrons", and as far as I understand him Ballentine precisely states this. The statistical interpretation is anyway very close to Copenhagen a la Bohr. Here's the precise quote from Ballentine:

View attachment 339219
Again in I the preparation procedure refers to single systems. Concerning the properties of the system described by the so prepared state it provides only the statistical properties and thus only refers to ensembles of such prepared single systems.
The statistical interpretation falls in group (I) from the quote, and yours in group (II).
 
  • #76
martinbn said:
Why not? Where does he differ?
At many points. He accepts neither the role of classical concepts in Bohr's thinking, nor the collapse of the wavefunction as an update of knowledge in Heisenberg's thinking. And your claim
martinbn said:
The statistical interpretation falls in group (I) from the quote, and yours in group (II).
feels strange to me. When has vanhees71 ever asserted that "a pure state provides a complete and exhaustive description of an individual system (e.g., an electron)"?
 
  • #77
martinbn said:
The statistical interpretation falls in group (I) from the quote, and yours in group (II).
My interpretation falls in group I, because for me all the state describes concerning the properties of the systems prepared in a state are the statistical properties, which of course refer to an ensemble of equally prepared systems. I just say the same as what Ballentine says with different words.
 
  • #78
vanhees71 said:
he says that the preparation procedure refers to a single electron
What you actually mean here is that the phrase "single electron" occurs in the passage in question from Ballentine's book. But it occurs in the context of describing an ensemble, which, as Ballentine makes clear, is not the same thing as the real collection of real electrons that get prepared and measured in real experiements. So you are taking Ballentine out of context when you claim that his use of the phrase "single electron" means that he takes the quantum state or the preparation procedure to apply to real single electrons in real experiments. Read in context, that is not what he is saying.
 
  • #79
vanhees71 said:
I just say the same as what Ballentine says with different words.
Perhaps you think you do, but nobody else here appears to agree.
 
  • #80
But then you couldn't use the formalism to describe real-world experiments. That's for sure not what Ballentine implies.
 
  • #81
PeterDonis said:
Perhaps you think you do, but nobody else here appears to agree.
@gentzen obviously understands it as I mean it.
 
  • #82
vanhees71 said:
But then you couldn't use the formalism to describe real-world experiments.
Sure you can. Ballentine describes how: you treat the real world statistical sample as just that, a statistical sample from the abstract ensemble that the formalism describes. Then you use standard statistical techniques to see how well the statistical sample matches what you would expect from the abstract ensemble.
 
  • #83
That's what I also say the whole time, and you get this statistical sample by preparing single electrons (using Ballentine's example for the argument) repeatedly in the same way, i.e., with a preparation procedure referring to a quantum state. This is even emphsized by Ballentine himself in distinguishing it from preparing once a many-electron system, which of course, if repeated. forms another statistical sample, which is not the same as preparing many times a single electron:

Untitled3.png
 
  • #84
vanhees71 said:
you get this statistical sample by preparing single electrons
Yes.

vanhees71 said:
distinguishing it from preparing once a many-electron system, which of course, if repeated. forms another statistical sample, which is not the same as preparing many times a single electron
Yes.

vanhees71 said:
with a preparation procedure referring to a quantum state
The state can be taken to refer to the preparation procedure, but if you take the state this way, it refers to the preparation procedure as it applies to the ensemble, not as it applies to an actual single electron in an experiment. The state is part of the mathematical model, not part of what you compare the model's predictions to. The actual preparation you do in the experiment, and the actual electron you do the preparation on, are part of what you compare the model's predictions to.

In other words, the term "preparation procedure", without any context, is ambiguous. There is the actual preparation you do in the actual experiment, that prepares single electrons, repeatedly, and there is the abstract "preparation procedure" in the model, that prepares an abstract ensemble. These are two different things, and the state, which is also in the model, if it is taken to refer to a preparation procedure, refers to the second thing just described, not the first.
 
  • Like
Likes mattt, vanhees71, bhobba and 1 other person
  • #85
Yes, of course the math is the math the real world is the real world, but the math accurately describes the real world according to the observations. So the samples you prepare with a preparation procedure are described by the formalism correctly, i.e., they are proxies of the ensembles described by the used preparation procedure. In high-precision experiments you can make the samples to come as close as you wish to the ensembles by just "collecting enough statistics", i.e., by repeating the experiment sufficiently often.
 

Similar threads

Replies
309
Views
14K
Replies
3
Views
2K
Replies
91
Views
7K
Replies
2
Views
2K
Replies
49
Views
5K
Replies
199
Views
17K
Replies
14
Views
3K
Back
Top