Born Rule in Many Worlds Derived?

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Discussion Overview

The discussion revolves around the derivation of Born's rule within the context of the Many Worlds interpretation (MWI) of quantum mechanics. Participants explore the implications of deriving Born's rule, its status as a postulate, and the interpretations of quantum states, particularly in relation to observable phenomena and the nature of reality.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Exploratory

Main Points Raised

  • Some participants argue that Born's rule is a fundamental postulate of quantum theory and does not require derivation.
  • Others suggest that deriving Born's rule could resolve significant issues within the Many Worlds interpretation, potentially favoring it over other interpretations.
  • One participant expresses skepticism about the explanatory value of the Many Worlds interpretation and questions its ability to relate quantum states to observable facts.
  • There is a discussion about the nature of discrete events in quantum mechanics, with some arguing for a continuous evolution perspective while others advocate for recognizing granularity in quantum processes.
  • Several participants express confusion or disagreement regarding the utility of Many Worlds and its interpretation of quantum states, with calls for clearer explanations of its implications.
  • Some participants propose alternative interpretations, such as the collapse hypothesis and Bohmian mechanics, while noting that these may not necessarily offer advantages over minimal interpretations.
  • There are discussions about the concept of a "one common world" and the need for proof of its existence, with suggestions that it may be an assumption rather than a derived principle.

Areas of Agreement / Disagreement

Participants generally express disagreement on the necessity and implications of deriving Born's rule, as well as the validity and utility of the Many Worlds interpretation. The discussion remains unresolved with multiple competing views presented.

Contextual Notes

Participants highlight limitations in understanding the relationship between mathematical formalism and observable phenomena, as well as the assumptions underlying various interpretations of quantum mechanics.

Is it?

  • Yes

    Votes: 1 10.0%
  • No

    Votes: 9 90.0%

  • Total voters
    10
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Many articles these years claim that they have derived it.Wonder what your thoughts on this problem are.
 
For me there's no need to derive Born's rule, because it's simply a fundamental postulate of quantum theory.
 
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vanhees71 said:
For me there's no need to derive Born's rule, because it's simply a fundamental postulate of quantum theory.
It's just some people argue that it's almost MW's last problem and if it's derived,MW would be "over the other interpretations".
 
I must admit that I never understood what MW is good for nor how it interprets quantum states. For me physical theory must clearly relate the mathematical formalism the theory is expressed into observable facts in Nature. I've not seen any convincing interpretation except the minimal statistical interpretation, i.e., a flavor of the Copenhagen Interpretations, where the state is just providing probabilities via Born's Rule (in the general sense for both pure and mixed states) for the outcome of measurements given a preparation procedure.
 
Adrian Lee said:
Many articles these years claim that they have derived it.
It surely depends what the derivation is based on. For a long time I too believed that Born"s rule ought to be derivable from Schrödinger's equation. But whenever I studied promising articles, the proof contained an innocent looking assumption that was equivalent to Born's rule (if it wasn't just shrouded in mathematIcs). Now I'm convinced that it is an independent ingredient of QM and even more important than the wave function. (What's observable can always be expressed using operators.)
Adrian Lee said:
It's just some people argue that it's almost MW's last problem and if it's derived,MW would be "over the other interpretations".
I don't consider MW an interpretation at all. It claims that Schrödinger's equation and continuous evolution is all there is to quantum theory. I can't believe that discrete events like the clicks of a Geiger counter are tricks played on us by our senses while the underlying reality evolves continuously. MWI glosses over the discrepancy with nothing but hand waving.
 
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This apparently discrete events are just rapid continuous dynamics, at least according to standard quantum theory.
 
You mean there is continuous evolution from 5, 4, 3, ... down to 0 undecayed atoms? I think there is some actual granularity that theoreticians should not conceal just because differential equations are easier to work with.
 
vanhees71 said:
I must admit that I never understood what MW is good for nor how it interprets quantum states.
I agree completely.

Many interacting observers - yes, but many worlds? What is the explanatory value and how it helps us forward?

/Fredrik
 
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  • #10
vanhees71 said:
I must admit that I never understood what MW is good for nor how it interprets quantum states.
Is there any non-minimal interpretation of QM for which you do understand what is it good for? :wink:
 
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  • #11
Well, yes. I've an idea, e.g., what's behind the idea of the collapse hypothesis (as an attempt to explain dynamically, how the preparation in a quantum state comes about) or Bohmian mechanics (as a nonlocal deterministic interpretation of the quantum state) although I don't think that these examples have in any sense any advantages in comparison to the more agnostic minimal interpretation, which just states the meaning of the quantum state for the purpose of describing the objective observations made in the lab without any attempt of further "metaphysical" explanations.
 
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  • #12
Fra said:
I agree completely.

Many interacting observers - yes, but many worlds? What is the explanatory value and how it helps us forward?

/Fredrik
Every observer with his or her own world. :-)
 
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  • #13
MathematicalPhysicist said:
Every observer with his or her own world. :-)
Not own world 😶 Every observer with its own subjectively inferred imperfect expectation of the one common world.

Observer equivalence is the special case of observer democracy where all the observers evolved their views to be in tune as analogous to a Nash equilibrium. Once in tune, the views asymptotically exhibits the symmetries the traditional pardigm sees as timeless constraints.

/Fredrik
 
  • #14
Fra said:
Not own world 😶 Every observer with its own subjectively inferred imperfect expectation of the one common world.

Observer equivalence is the special case of observer democracy where all the observers evolved their views to be in tune as analogous to a Nash equilibrium. Once in tune, the views asymptotically exhibits the symmetries the traditional pardigm sees as timeless constraints.

/Fredrik
The "one common world" is the one which needs proof of its existence, otherwise it's as always assumed that it exists.
 
  • #15
I heard once from someone that the axiom that through two points passes one unique straight line follows from some variational principle/s.
So the axiom of one common world might follow from some other principle/s or we might abandon it.
I guess one can use some sort of possible worlds modal logics for QT.
Tried typing google for Quantum Modal Logic... I don't know if it exists but nice term like all quantum something.
:oldbiggrin:
 
  • #16
MathematicalPhysicist said:
The "one common world" is the one which needs proof of its existence, otherwise it's as always assumed that it exists.
The only meaning I assign to the "one common world" is "what you get from all physical observers that are in causal contact with each other". Exactly what this is in detail - the microstructure of observers and their relations - is of course what the whole game of inference is about. It´s also necessarily moving target as I think the inference process itself helps to form and a self-organisation will take place. There will never be a complete answer, because the more complex and observer gets, it´s ability to encode more complex relations increase. The ambition is IMO just to understand the abductive inference mechanisms here.

In the research I see implied from this "interpretation" is to identify the most sensible mathematical model for this, and to investigate - in the limit of low complexity of observers - how many options there is. There is some hope that the options are limited, andn that predictions may come out. The hope is that - for any given complexity bound - there may be some uniqe rules that would represent a relation of worldviews that are "optimally" compressed. Like represented by some unique mathematics. But we do not just want to find the mathematics, we also want to understand in deeper WHY its the right one.

So the vision is that once observers interact, their common reality emerges asymptotically. An idea is that, the communication implies a universal unavoidable negotiation driving evolution. So the emergent patterns here should match the particle zoo and their relations. If it does not, then the interpretation is a failure.

/Fredrik
 
  • #17
WernerQH said:
You mean there is continuous evolution from 5, 4, 3, ... down to 0 undecayed atoms? I think there is some actual granularity that theoreticians should not conceal just because differential equations are easier to work with.
Its not much different from the continuous evolution of a discrete number of corona viruses from 0, to 1,2,3,4, to a huge number.
 
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  • #18
A. Neumaier said:
Its not much different from the continuous evolution of a discrete number of corona viruses from 0, to 1,2,3,4, to a huge number.
It's strange for a mathematician to be lacking in a precise definition of the term "continuous". :-)
 
  • #19
WernerQH said:
It's strange for a mathematician to be lacking in a precise definition of the term "continuous". :-)
This is a physics forum, so I use the term consistent with physics usage. But I presume that the evolution of viruses is governed primarily by classical mechanics, which is continuous even in the mathematical sense.
 
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  • #20
WernerQH said:
You mean there is continuous evolution from 5, 4, 3, ... down to 0 undecayed atoms? I think there is some actual granularity that theoreticians should not conceal just because differential equations are easier to work with.
I think what's effectively continuous and what is not is observer-dependent. A binary state always has a discrete transition, but if can consider the probability for the transition of the same state by observing the context as well, it can be almost continous. But the latter description contains MORE information and thus requires a sufficiently complex observer.

Its tempting to think that there is always a suffiently complex observer that can have maximal knowledge, and that this would be the "correct" description, but this will not explain the action of the non-maximal systems! It instead leaves us with a silly situation with the wave function of the whole universe. Something no one can compute or fine tune.

/Fredrik
 
  • #21
In quantum theory the evolution of the state (statistical operator) is described by a partial differential equation and thus is continuous. So are the probabilities and related expectation values concerning discrete variables like "the number of infected people" in a epidemics/pandemics simulation.
 
  • #22
Of course. Averages evolve continuously and deterministically. This may have a soothing effect on some physicists. But it doesn't make discontinuities and randomness go away. We should not be misled by Schrödinger's equation to think that physical evolution is necessarily continuous and deterministic. There's ample evidence that it is fundamentally random and discontinuous. After all, it's called quantum theory, and it describes the behaviour of atoms.
 
  • #23
The dynamics of quantum theory is continuous (even smooth) and it's causal. At the same time it's probabilistic and indeterministic. This is no contradiction to the fact that it describes, among all other known "things", atoms.
 
  • #24
"Dynamics" is a classical concept. Schrödinger's equation alone does not fully describe quantum processes. I'd say you are so habituated to quantum theory that you can't perceive the contradiction any more. :-)
 
  • #25
I identified two facets of the discussion here, not sure which one Werner was after but... on the second facet

vanhees71 said:
In quantum theory the evolution of the state (statistical operator) is described by a partial differential equation and thus is continuous. So are the probabilities and related expectation values concerning discrete variables
I think such infinite and uncountable amounts of information is likely a fiction that works well for describing atomic phenomena from the perspective of a dominant classical environment.

In symbolic math, one can easily imagine anything, but whenever you try to actually solve, and compute something, one is typically constrained to fixed precision and fixed information processing capacity. The problem is one asks not just for a description of a small subsystem, but a betting method for action in an unknown environment. Then the non-dominant agent is I think, intutively, certainly saturated with information, and has to resort to lossy retention, and make the right choices to be successful. The latter is the scenariou of inside observers (cosmology) and also to find explanatory improvements of unification of interactions, even from the perspective of classical reality.

/Fredrik
 
  • #26
To the contrary! If you have a small subsystem coupled to a macroscopic "environment", you don't have control and thus "trace out" the environment, i.e., we average over a lot of unknown degrees of freedom to effectively describe the "relevant observables" of the subsystem.

Even in cosmology, all we can do is to observe local observables and then extrapolate to the "universe as a whole" assuming the cosmological principle, which is amazingly successful.
 
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  • #27
Is the Born rule derived in any interpretation?! And why do physicists (at least some) obsess about it? What is the need to have a minimal number of postulates?
 
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  • #28
Right. Schrödinger's equation by itself is not enough; we need the Born rule to obtain measurable quantities from the wave function. Accordingly it is not derivable from Schrödinger's equation. But it seems that MWI supporters disagree and prefer to think that Schrödinger's equation is all that quantum theory is about.

What people have qualms about is how unitary evolution and "measurements" fit together. Schwinger's action principle that led to the closed time-path formalism allows direct calculation of observable quantities. It smoothly joins unitary evolution and the Born rule in one formalism.
 
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  • #29
WernerQH said:
Right. Schrödinger's equation by itself is not enough; we need the Born rule to obtain measurable quantities from the wave function. Accordingly it is not derivable from Schrödinger's equation. But it seems that MWI supporters disagree and prefer to think that Schrödinger's equation is all that quantum theory is about.
Isn't that about the time evolution only? MWI says that the evolution of the state is given by the Schrödinger's equation, no collapse. It doesn't say that there are no other accpects of QM. At least that is how I always understood it.
WernerQH said:
What people have qualms about is how unitary evolution and "measurements" fit together. Schwinger's action principle that led to the closed time-path formalism allows direct calculation of observable quantities. It smoothly joins unitary evolution and "measurements" in one formalism.
 
  • #30
martinbn said:
Isn't that about the time evolution only? MWI says that the evolution of the state is given by the Schrödinger's equation, no collapse. It doesn't say that there are no other accpects of QM. At least that is how I always understood it.
The other aspects are the other universes, or branches thereof. The central puzzle is: How does the wave function relate to the real world that we perceive around us?
 

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