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... but by different frogs, right?Dmitry67 said:the key concept of MWI is that both possibilities are observed.
... but by different frogs, right?Dmitry67 said:the key concept of MWI is that both possibilities are observed.
Demystifier said:... but by different frogs, right?
ueit said:The issue is different in MWI where all reality is supposed to somehow emerge from a wavefunction. Decoherence does not explain this.
Quantum decoherence gives the appearance of wave function collapse and justifies the framework and intuition of classical physics as an acceptable approximation: decoherence is the mechanism by which the classical limit emerges out of a quantum starting point and it determines the location of the quantum-classical boundary
As a consequence, the system behaves as a classical statistical ensemble of the different elements rather than as a single coherent quantum superposition of them. From the perspective of each ensemble member's measuring device, the system appears to have irreversibly collapsed onto a state with a precise value for the measured attributes, relative to that element.
Dmitry67 said:Well, as your claim contradicts with Wiki:
Quantum decoherence gives the appearance of wave function collapse and justifies the framework and intuition of classical physics as an acceptable approximation: decoherence is the mechanism by which the classical limit emerges out of a quantum starting point and it determines the location of the quantum-classical boundary
As a consequence, the system behaves as a classical statistical ensemble of the different elements rather than as a single coherent quantum superposition of them. From the perspective of each ensemble member's measuring device, the system appears to have irreversibly collapsed onto a state with a precise value for the measured attributes, relative to that element.
the burden of proof is yours
ueit said:To clarify this issue, can you point me at a set of postulates that define MWI so I can refer to them?
jnorman said:a small quibble, inre: "B. An unbound neutron has a half-life of perhaps 15 minutes."
a single neutron does not have a half-life.
Demystifier said:A. Even in standard QFT, vacuum fluctuations do NOT produce virtual particles. The vacuum is an eigenstate of the operator of the number of particles, so there are no particle fluctuations in the vacuum. What fluctuates in the vacuum is the value of field. Virtual particles are something different, they are artefact of a specific mathematical method of treating interactions, based on perturbation method. If you use some other method, such as numerical path integration on the lattice, then nothing analogous to virtual particles exists. For more details see e.g. Secs. 9.3. and 9.4. in
http://xxx.lanl.gov/abs/quant-ph/0609163 [Found.Phys.37:1563-1611,2007]
Dmitry67 said:Ha! This is the most interesting thing: while other interpretations have additional postulates (wave, guiding a particle inside, mysterious collapse and special role of measurement, offer and normal wave, etc) MWI does not have any additional postulates. It is a NULL interpretation - there are no any additional assumptions.
(Common misconseption that MWI postulates splitting and the existence of the parralel worlds)
Just take wavefunction, and shut up and calculate. If you wonder what observers would see - use quantum decoherence.
There are many blah blah around MWI - universes et cetera, but parralel worlds is merely a consequence of QD.
Dmitry67 said:Ha! This is the most interesting thing: while other interpretations have additional postulates (wave, guiding a particle inside, mysterious collapse and special role of measurement, offer and normal wave, etc) MWI does not have any additional postulates. It is a NULL interpretation - there are no any additional assumptions.
Just take wavefunction, and shut up and calculate.
If you wonder what observers would see - use quantum decoherence.
Count Iblis said:You do need to define a preferred basis.
ueit said:1 I didn't ask for "additional postulates", but for the set of postulates that define MWI.
2 You cannot calculate anything from the wavefunction unless you specify what the relationship between this wavefunction and our observation is. For example, in the Copenhagen interpretation (CI) you use Born postulate to calculate the probability of finding a particle in a certain volume of space. As you see I have used words like "particle", "volume of space" that have a very clear meaning here (CI assumes the existence of the classical world). If you only have the wavefunction how are you supposed to recognize in it anything that looks like a 3D world? How do you calculate the probabilities of anything?
3 What does "observer" mean in MWI? How do I recognize such an entity only looking at a wavefunction?
I have already explained it to you, but let me try again. MWI requires frogs, but there is no any mathematical theory of frogs within MWI. On the other hand, the additional equations that BI contains are nothing but a mathematical theory of frogs. Moreover, BI seems to be the simplest possible mathematical theory of frogs consistent with MWI.Dmitry67 said:And yes, I know that there is a duality between BI and MWI. But can I ask, what makes BI so attractive to you?
No. Feynman diagrams have nothing to do with paths or branches. To understand this, I suggest you to see a mathematical derivation of Feynman diagrams from first principles. For pedagogical purposes, I suggest you to see this within CLASSICAL (not quantum) mechanics (Refs. 52, 53).DrChinese said:As I understood it, the probabilities include terms for many paths (or branches), actually I guess an infinite number.
It seems to me that you are not close at all.DrChinese said:OK. But there are contributions from some higher order branches that need to be considered, and they represent "something". We can't just ignore them. And I suppose these are usually thought of as virtual particles simply because they are mathematical artifacts (i.e. act mathematically like particles). They are NOT there when the smoke clears, but their presence IS felt. As something of a realist, I would expect you of all people to acknowledge that what appears in the formula must have some counterpart in nature.
Am I close?![]()
Dmitry67 said:I can understand how you can define a hidden preferred frame in flat spacetime. It is the same in LET (Lorentz Ether Theory, compatible with SR).
But how can you do the same for the black hole metric? Can you define a single frame common to space inside and outside the horizon?
ueit said:I am not sure what "pure QM" is supposed to be but the orthodox interpretation assumes the existence of a classical world with observers, instruments and all that. In BM you also work on a 3D space background so one does not need to explain it. The issue is different in MWI where all reality is supposed to somehow emerge from a wavefunction. Decoherence does not explain this.
ZapperZ said:Hum... then all I wanted to say is that, that is not condensed matter physics.
Dmitry67 said:yes, sure, I am MWI fan.
I don't see any problems with a frog.
the key concept of MWI is that both possibilities are observed.
Demystifier said:I have already explained it to you, but let me try again. MWI requires frogs, but there is no any mathematical theory of frogs within MWI.
Ilja said:Yes, I can. I have to modify the theory of gravity for this, but I have done this already before becoming a Bohm supporter. See ilja-schmelzer.de/glet.
Ilja said:But my main problem with MWI is that none of the possibilities has anything to do with the wave function. The wave function appears to be some linear combination of them, but every two states |a> and |b> are connected in such a way: |a> = |b> + (|a> - |b>). Thus, this linear decomposition defines no connection at all between the wave function and the particular branch.
I will calculate that when you calculate the probability distribution of prices per barrel next year starting from first principles of QM in the many-world interpretation.Dmitry67 said:I have a cosmological question to the BM supporters.
What is price per barrel next year?
I mean, it is definitely pre-coded at the time of the Big bang, right :) ? Laplace determinism is valid for any deterministic single=history theory...
That is a good point. Still, there is a set of physical laws, which are not completely independent, that explain BOTH chemistry and phases of the moon. BI is an attempt to do something similar for BOTH MWI and frogs. Moreover, the encouraging fact is that BI achieves that in a rather simple way.Dmitry67 said:So your question 'but how MWI explains the frogs?' is like 'I see that chemistry works well, but how chemistry explains the phases of the moon?'
Dmitry67 said:I see CI, for example, as a modern alchemistry: a description of the QM world based on some magical 'measurement devices' and 'knowledge of an observer about the system'.
MWI get rids of it like modern chemistry get rids of the phases of the Moon. So your question 'but how MWI explains the frogs?' is like 'I see that chemistry works well, but how chemistry explains the phases of the moon?'
Ilja said:Yes, I can. I have to modify the theory of gravity for this, but I have done this already before becoming a Bohm supporter. See ilja-schmelzer.de/glet.
Demystifier said:1. Feynman diagrams have nothing to do with paths or branches. To understand this, I suggest you to see a mathematical derivation of Feynman diagrams from first principles. For pedagogical purposes, I suggest you to see this within CLASSICAL (not quantum) mechanics (Refs. 52, 53).
2. It seems to me that you are not close at all.
Let me use an analogy. Consider a classical wave, say a wave on the surface of watter. It may have a complicated shape. Mathematically, it can be written as a Fourier sum of plane waves. But does it mean that plane waves are really there, that they are real? Not at all. Alternatively, it can also be written as a Taylor sum. But does it mean that particular terms in the Taylor expansion represent real objects? Again, not at all. All that makes a physical sense is the TOTAL function that describes the real wave. Particular terms in this or that expansion are nothing but a mathematical trick that simplifies calculations.
If it is still not clear to you, let me use an even simpler analogy. Assume that you have 1 apple. You can write it as
1=2+(-1)
Does it mean that you actually have 2 apples and -1 apple? Of course not. All you really have is 1 apple, and that's it.
Count Iblis said:What do the people opposed to MWI make of the thought experiment by David Deutsch in which you do a measurement and then forget the result of the measurement but not that the measurement was carried out, in such a way that the original wavefunction of the object is restored?