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.
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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".vanhees71 said: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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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:Many articles these years claim that they have derived it.
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.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".
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I agree completely.vanhees71 said:I must admit that I never understood what MW is good for nor how it interprets quantum states.
Many interacting observers - yes, but many worlds? What is the explanatory value and how it helps us forward?
/Fredrik
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Is there any non-minimal interpretation of QM for which you do understand what is it good for?vanhees71 said:I must admit that I never understood what MW is good for nor how it interprets quantum states.
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Every observer with his or her own world. :-)Fra said: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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Not own worldMathematicalPhysicist said:Every observer with his or her own 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
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The "one common world" is the one which needs proof of its existence, otherwise it's as always assumed that it exists.Fra said:Not own worldEvery 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
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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.

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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.MathematicalPhysicist said:The "one common world" is the one which needs proof of its existence, otherwise it's as always assumed that it exists.
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
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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.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.
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It's strange for a mathematician to be lacking in a precise definition of the term "continuous". :-)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.
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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.WernerQH said:It's strange for a mathematician to be lacking in a precise definition of the term "continuous". :-)
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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.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 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
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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.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
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
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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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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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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: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.
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.
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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?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.
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