Difference betweem Many Worlds and Consistent Histories?

In summary: What you argue is that if you want ontological wavefunction without collapse you have to accept either DeWitt/Deutsch type MWI or Bohm?Both are deterministic.
  • #1
ThisIsMyName
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Can some help me out?

It seems both postulate:

Ontological wavefunction of the whole universe
No collapse
Both are deterministic
Both use decoherence

So what's different about them?
 
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  • #2
First, CH does not postulate that wave function is ontological. Second, CH is not deterministic.
 
  • #3
Demystifier said:
First, CH does not postulate that wave function is ontological. Second, CH is not deterministic.

Thanks for being the only one out of over 100 people reading this topic to answer:)

According to what I've read Hawking believe in a "Consistent Histories" Everettian type interpretation.
Where only a few worlds become "real", while hte rest are just possibilities.
Then you got the CH of Gellman and Hartle, this too seems to say the wavefunction is ontological.

What you argue is that if you want ontological wavefunction without collapse you have to accept either DeWitt/Deutsch type MWI or Bohm?
 
  • #4
ThisIsMyName said:
Thanks for being the only one out of over 100 people reading this topic to answer:)

According to what I've read Hawking believe in a "Consistent Histories" Everettian type interpretation.
Where only a few worlds become "real", while hte rest are just possibilities.
Then you got the CH of Gellman and Hartle, this too seems to say the wavefunction is ontological.

What you argue is that if you want ontological wavefunction without collapse you have to accept either DeWitt/Deutsch type MWI or Bohm?
There aren't many people here who know the consistent histories approach. I don't know it well enough myself to give a good answer to those questions. (I've been thinking that I should read this more carefully for a couple of years now, but it has never reached the top of my "to do" list since I first skimmed it). Regarding your last point, I think that what you would have to accept if you decide to view the state vector as ontological, in the version of QM that's based on the most popular set of axioms, is a different type of MWI. One that doesn't throw out the Born rule, like Everett did, and that relies on decoherence to tell us which worlds are "interesting" in the sense that they can contain conscious observers.

Isn't CH just the ontological interpretation that's based on a slightly different set of axioms for QM? (It's been too long since I skimmed that article, so I don't even remember what it's based on. Unfortunately I don't have time to read about it or get deeply involved in a discussion about it now). I like to think of a "theory" as defined by its axioms rather than by its predictions, and if CH is based on different axioms, it's a different theory in my book (but probably equivalent to standard QM in the sense that it makes the same predictions). So maybe CH and the MWI I'm talking about should be thought of as very similar interpretations of two different but equivalent theories.

But again, I hardly remember anything about the CH, so don't take what I said about it too seriously. I'm serious about the MWI though.
 
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  • #5
ThisIsMyName said:
What you argue is that if you want ontological wavefunction without collapse you have to accept either DeWitt/Deutsch type MWI or Bohm?
Yes.

Concerning CH, I would say it is a variant of the Copenhagen interpretation (CI), in the sense that QM only says what are the probabilities of different measurement outcomes. However, the difference is the following. If you perform many measurements at different times on the same system, CH treats it as a single measurement - the measurement of the whole history of the system. For that reason you do not need the collapse of the wave function in CH. CH says what is the probability of a given history.
 
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1. What is the main difference between Many Worlds and Consistent Histories?

The main difference between Many Worlds and Consistent Histories is the interpretation of quantum mechanics. Many Worlds suggests that all possible outcomes of a quantum event exist in parallel universes, while Consistent Histories proposes that only one outcome is actualized and the others do not exist.

2. Which interpretation is more widely accepted in the scientific community?

Currently, the Many Worlds interpretation is more widely accepted by the scientific community, as it is seen as a more straightforward and mathematically elegant explanation of quantum mechanics. However, Consistent Histories is also gaining traction and has its own proponents.

3. How do these interpretations explain the phenomenon of wave-particle duality?

Both Many Worlds and Consistent Histories explain wave-particle duality by suggesting that particles exist as both waves and particles simultaneously, and it is the act of observation that collapses the wave function and determines the particle's state.

4. Can Both Many Worlds and Consistent Histories coexist?

Yes, Many Worlds and Consistent Histories can coexist as they are simply different interpretations of the same quantum phenomena. Some scientists believe that both interpretations may be valid in different contexts or at different scales.

5. Are there any experiments that can distinguish between Many Worlds and Consistent Histories?

At this time, there are no known experiments that can definitively distinguish between Many Worlds and Consistent Histories. However, ongoing research and advancements in technology may lead to new experiments that could potentially provide evidence for one interpretation over the other.

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