What pains me the most, is that this mailing list had I think the most influential and best thinkers of this century and we're left with that... this list had (and still has for those not in the mind bending dead state) hal finney, wei dai, jurgen Schmidhuber, Russell Standish, Saibal Mitra, Jason Resch, Terren Suydam, Telmo Menezez, Brent Meeker, Bruno Marchal and all of the nice non troll and truth seeking humans in this reality that I forgot, happy new year, happy new day to be alive to you all and happy discovering of this mind bending reality. I really love you all, even the ones who triggers that bad feelings in me.
> If you propose God, then I totally agree.
>>the question of list moderation would not be relevant at this time if one very recent list member didn't think page after page of nothing but "(:>)" characters was an intelligent rebuttal, and ALL scientific questions of the form "what is the nature of X?" can be answered by simply saying "X does not exist".
> Of course, given that consciousness is all there is. Why would you waste time talking about things that don't exist ?
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You can continue cancer research. But is just like playing World of Warcraft in order to get the legendary gear.
@Alan. You can do cancer research. But since that research is not based on fundamental ideas about reality, it will be just guesswork: Just try 1000 different drugs and cross fingers that one might work. Instead, if people would actually understand consciousness, they would cure cancer in 1 week.
How do you expect you can properly fix a car if you don't know how it function ? You just do guesswork, you give it a few kicks and maybe it starts. This is how present-day science works given that it doesn't work based on fundamentals, namely based on the working of consciousness. Sure, you can keep doing research this way: kick it till it works. And you might save a few lives. But if you were start from fundamentals, then you would know exactly what you were doing and you will save 8 billion lives. Not that it would matter at that point, given that at that level of development we will manipulate consciousness to such a degree that we will not even need bodies anymore.
On Saturday, January 4, 2025 at 9:53:59 AM UTC-7 Cosmin Visan wrote:How do you expect you can properly fix a car if you don't know how it function ? You just do guesswork, you give it a few kicks and maybe it starts. This is how present-day science works given that it doesn't work based on fundamentals, namely based on the working of consciousness. Sure, you can keep doing research this way: kick it till it works. And you might save a few lives. But if you were start from fundamentals, then you would know exactly what you were doing and you will save 8 billion lives. Not that it would matter at that point, given that at that level of development we will manipulate consciousness to such a degree that we will not even need bodies anymore.About 60 years ago I met a fellow with your philosophy, a Master of Yoga, an adept at "Traditional Science", author of several books, who claimed with great authority that the problem of cancer had been "solved". He never got cancer but died of a heart failure around age 80 in 2008. AG
I just opened a topic a while back about the definition of the word "useful" that you keep abusing. Let's remind you:Useful = whatever increases happiness.Useless = whatever doesn't increase happiness.My philosophy, I guarantee you 100%, increases happiness, so is useful.Getting cured of cancer might still let you depressed, so cancer cure is useless.
It depends what kind of person you are. If you are a depressed person, curing you of cancer will not do any good. On the contrary, if you would have died you would havd gotten a chance at happiness in the next life.
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> Moderation is inappropriate where Trump physics is endorsed. AG
Please assure me that I will be kept on the list whether you go not open to the public or public I approve your choices in advance
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0o1
Thank you In this dismal world in a rainy day you bring mirth and a giggle Thank you thank you for your interesting arguments
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On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN.
And please don't offer your BS that you've answered it repeatedly. Such a claim would be blatent lie. Finally, I know what you haven't offered the answer. It's really simple. You don't want to admit the Emperor has no clothes, as such an admission might trigger a coronary when you realize you've been preaching a lie these many years. AG0o1
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About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
On 1/4/2025 1:11 PM, Alan Grayson wrote:
Basically it boils down to two things. One, they think the Schoredinger equation is sufficient to described measurement so long as the world can separate into independent copies for each eigenvalue of the measurement. Exactly how this separation proceeds and how it is originated is sort of hand wavy, but they're sure it can be squared. Second, they want everything to be deterministic. So having all but one of the world's go away would require randomness per the Born rule. At one time they thought the Born rule was already implict in the Schoredinger equation. But since everything happens it's not so clear what it means that probabilities are equal to the squared amplitude. Probability of what? Not probability of a value happening. Probability of finding oneself in a particular world? How does the probability amplitude of a quantum event get to apply some kind of "weight" to you or to a world? One my say "That's just the way it is. If it's probabilistic then it must follow Born's rule by Gleanson's theorem." But then that's assuming it's probabilistic, not just Schroedinger's equation...in which case why not just bite the bullet and says it's the probability that a particular world exists.
On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN.
--
Brent
--And please don't offer your BS that you've answered it repeatedly. Such a claim would be blatent lie. Finally, I know what you haven't offered the answer. It's really simple. You don't want to admit the Emperor has no clothes, as such an admission might trigger a coronary when you realize you've been preaching a lie these many years. AG0o1
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> since everything happens it's not so clear what it means that probabilities are equal to the squared amplitude. Probability of what? Not probability of a value happening. Probability of finding oneself in a particular world?
> If it's probabilistic then it must follow Born's rule by Gleanson's theorem." But then that's assuming it's probabilistic not just Schroedinger's equation.
> ...in which case why not just bite the bullet and says it's the probability that a particular world exists.
This has been proposed before - by my friend Duraid Madina, where he
forked the list into a moderated one. It did not fare well. Nobody
moved to the new list, it was as dead as a doornail. He is now working
on other things in his life
So sadly, we have to deal with trolls by ignoring them. It wouldn't be
so bad if people kept things on-topic, but even then it seems we can't
help ourselves.
Every 4 years, this list gets dominated by discussion
of the US election, as does every other internet discuss fora. For us
non Americans, who have absolutely no influence on the outcome, it
does get a tad tedious.
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> Moderation is inappropriate where Trump physics is endorsed. AGAbout a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
> his answer to energy requirements for these new worlds seems weak, that energy is somehow globally conserved while the energy in particular branches can decrease,
> How could gravity be included as if it's something different from curvature of spacetime, which is caused by stress-energy tensor?
> I'm pretty sure Carroll said energy is conserved in the MWI,
@Alan you wouldn't ask such question if you would understand that energy doesn't exist. "Energy" is just an idea in consciousness. All these theories that people create are just random guesses. They work until they don't. Wondering where the energy goes and so on is pointless, for the trivial reason that you go beyond what that guess covered and you are back to square 1 of making another guess.
> you wouldn't ask such question if you would understand that energy doesn't exist.
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On Sun, Jan 5, 2025 at 12:44 AM Bruce Kellett <bhkel...@gmail.com> wrote:On Sun, Jan 5, 2025 at 7:46 AM John Clark <johnk...@gmail.com> wrote:About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.I watched this video, but it is not as comprehensive as Carroll's book "Something Deeply Hidden".However, something came up in the question period that might warrant a comment. Talking about the Born rule, Carroll justifies it by saying that if you measure the spin of 1000 unpolarized particles, you get 2^1000 different UP-DOWN sequences. However, the vast majority of these sequences will show proportions of UP vs DOWN close to the Born rule prediction of 50/50. In the limit, if such a limit makes sense, the proportion of sequences that show marked deviations from the Born Rule proportions will form a set of measure zero, and can be ignored.That is just the law of large numbers at work, and is all very well if the amplitudes are such that the Born probabilities are equal to 0.5. But it is easy to rotate your S-G magnets so that the Born probabilities are quite different, say, 0.9-Up to 0.1-DOWN. Now take 1000 trials again. According to Everett, you necessarily get the same 2^1000 sequences of UP-DOWN that you had before. The law of large numbers will then tell you that the majority of these will have approximately a 50/50 UP/DOWN split, which is grossly in violation of the Born rule result of a 90/10 split. In other words, MWI. or Everettian QM. has a problem reproducing the Born rule. It works in the simple case of equal probabilities, but fails miserably once one departs substantially from equal probabilities.BruceDavid Z Albert mentions that if you define a measurement operator that just tells you the *fraction* of spin-up vs. spin-down in a large sequence of identical measurements, then even without any collapse assumption, in the limit as # measurements goes to infinity the wavefunction will approach an eigenstate of this operator that matches the probability that would be predicted by the Born rule. See his comments on p. 238 of The Cosmos of Science at https://books.google.com/books?id=_HgF3wfADJIC&lpg=PP1&pg=PA238#v=onepage&q&f=false"Then, even though there will actually be no matter of fact about what h takes the outcomes of any of those measurements to be, nonetheless, as the number of those measurements which have already been carried out goes to infinity, the state of the world will approach (not as a merely probabilistic limit, but as a well-defined mathematical epsilon-and-delta-type limit) a state in which the reports of h about the statistical frequency of any particular outcome of those measurements will be perfectly definite, and also perfectly in accord with the standard quantum mechanical predictions about what the frequency out to be."
On 1/4/2025 1:11 PM, Alan Grayson wrote:
On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN.
You think it absurd that you didn't exist in the past and after a finite time you will no longer exist?? Most people, and physicists, think that's the case.Basically it boils down to two things. One, they think the Schoredinger equation is sufficient to described measurement so long as the world can separate into independent copies for each eigenvalue of the measurement. Exactly how this separation proceeds and how it is originated is sort of hand wavy, but they're sure it can be squared. Second, they want everything to be deterministic. So having all but one of the world's go away would require randomness per the Born rule. At one time they thought the Born rule was already implict in the Schoredinger equation. But since everything happens it's not so clear what it means that probabilities are equal to the squared amplitude. Probability of what? Not probability of a value happening. Probability of finding oneself in a particular world? How does the probability amplitude of a quantum event get to apply some kind of "weight" to you or to a world? One my say "That's just the way it is. If it's probabilistic then it must follow Born's rule by Gleanson's theorem." But then that's assuming it's probabilistic, not just Schroedinger's equation...in which case why not just bite the bullet and says it's the probability that a particular world exists.
Because to me in itself, only one world is absurd... as absurd that my life is finite and preceeded by an infinite time in the past and infinite time in the future...
It's just improbable, which is quite different from absurd. Every hand of bridge I've been dealt was improbable, but I never considered one absurd.I know reality doesn't have to please me, but one world theory is as absurd as absurd can be imo. Only a theory about information where everything exists seems lesz absurd, yeah there is a gazillion things in it, so there is also in one world, thing is with MW like things, there is an explanation for you to be, you're one of the possibilities... in one world, you're one possibilities realised whatever that means against all not realised whatever that means, the realised thing is the absurd.
Quentin
-- All those moments will be lost in time, like tears in rain. Roy Betty, Rutger Hauer
Brent
And please don't offer your BS that you've answered it repeatedly. Such a claim would be blatent lie. Finally, I know what you haven't offered the answer. It's really simple. You don't want to admit the Emperor has no clothes, as such an admission might trigger a coronary when you realize you've been preaching a lie these many years. AG
0o1
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@Brent. "An absurd conclusion implies an absurd argument."
You clearly missed your Logic 1.0.1. class.
On Sunday, 5 January 2025 at 00:07:36 UTC+2 Brent Meeker wrote:
On 1/4/2025 10:27 AM, 'Cosmin Visan' via Everything List wrote:
> I just opened a topic a while back about the definition of the word
> "useful" that you keep abusing. Let's remind you:
>
> Useful = whatever increases happiness.
> Useless = whatever doesn't increase happiness.
>
> My philosophy, I guarantee you 100%, increases happiness, so is useful.
> Getting cured of cancer might still let you depressed, so cancer cure
> is useless.
An absurd conclusion implies an absurd argument.
Brent
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On Saturday, January 4, 2025 at 8:06:38 PM UTC-7 Alan Grayson wrote:
On Saturday, January 4, 2025 at 2:11:02 PM UTC-7 Alan Grayson wrote:
On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN. And please don't offer your BS that you've answered it repeatedly. Such a claim would be blatent lie. Finally, I know what you haven't offered the answer. It's really simple. You don't want to admit the Emperor has no clothes, as such an admission might trigger a coronary when you realize you've been preaching a lie these many years. AG
I watched it. I can't say I fully understand it or believe it. I'll probably watch it again. I do know that lately I am less impressed with the cat experiment, as I recall a recent comment by Brent; that there's no operator which has Alive and Dead as its eigenvalues. This, IMO, means that the cat's wf isn't a valid quantum wf. AG
You're misinterpreting what I wrote. I meant that being alive is a superposition of a bazillion of different wave functions so it is impossible to formulate a measurement operator which will return just one of two values that actually correspond to Alive and Dead. In other words the exist a range of states that count as alive, some of which are dying, and a range of states that would count at dead, but some of which are recovering. It doesn't mean there is no WF of the cat. I means that alive and dead are only well defined in the extreme cases because the cat has many intermediate states which we can't account for in our measurement operator.
If the cat's wf isn't a valid wf in QM, which is now my belief, does the same apply to Decayed and Undecayed? That is, what is the operator which has Decayed and Undecayed as it eigenvalues? AG
Another question relates to the superposition which involves the Environment. Carroll claims the observer is contained in this superposition as part of the Environment without experience it's in such a state. Is this the origin of the Many Worlds in the MWI? If so, this seems independent of S's equation, and follows directly from the quantum definition of the wf as a linear sum of eigenvalues. AG
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On Sat, Jan 4, 2025 at 7:18 PM Brent Meeker <meeke...@gmail.com> wrote:
> since everything happens it's not so clear what it means that probabilities are equal to the squared amplitude. Probability of what? Not probability of a value happening. Probability of finding oneself in a particular world?
It's not just epistemological when it includes the whole world whether anybody else knows it or not. QBism is actually an epistemological interpretation which considers different wave functions for different people depending on what they know.Yes. That wasn't so unclear was it.> If it's probabilistic then it must follow Born's rule by Gleanson's theorem." But then that's assuming it's probabilistic not just Schroedinger's equation.No. If Many World is correct then ontological randomness can not exist but epistemological randomness certainly can and certainly does. Even in classical physics epistemological randomness exists whenever you lack the information needed to make an exact prediction, that's why you can't predict a coin flip or a roulette wheel .
Laplace's demon, which has knowledge of all initial conditions and has infinite computational capacity, does not need to think about "worlds" but can just contemplate how the quantum wave function of the entire universe evolves. Unfortunately we are not as smart or as knowledgeable as Laplace's demon, so we need to talk about worlds.
For example: a box with Schrodinger's cat inside it, the environment, and you, are all quantum objects entangled together, so there are not 3 separate wave functions but only one. After one hour there is a 50% chance of the cat surviving, that means the quantum wave consists of { (a live cat, the environment the live cat is in, and you observing the live cat) + ( a dead cat, the environment the dead cat is in, and you observing the dead cat) } . After one hour you are either in the dead cat environment or the live cat environment with a 50-50 probability, but you lack the information needed to know which one and will only obtain it when you open the box.
> ...in which case why not just bite the bullet and says it's the probability that a particular world exists.
You have to explain when the worlds split; which amounts to the same thing.Because then you have to explain why Schrodinger's equation suddenly stops working.
Measurement doesn't even have to include me or anybody else. The cat example just obfuscates the question. The measurement is done when the detector detects the atomic decay. A cleaner version has a clock stopped by the detection. Then it's clear that the Schroedinger equation applied to the whole system is separating the world when the detection is made. Exactly how this separation proceeds is somewhat hand wavy but I can see that it will eventually make different orthogonal worlds, only one of which we see. Carroll once joked that non-Everettians needed to explain the disappearing worlds. I don't see that as taking anymore explanation than he gives for them being orthogonal. What he fails to explain is how probabilities are realized in these worlds. As Bruce pointed out, except for 50-50 cases the overwhelming number of worlds find QM to be empirically falsified; so branch counting doesn't work. It appears that the Born rule adds another axiom; it's not just the Schroedinger equation.And then you have to explain exactly what a "measurement" is and why Schrodinger's equation treats you very differently than any other quantum object.
Incidentally, the very first post sent to the Everything List was sent by the late great Hal Finney (he was cryonically frozen in 2014 and became Alcor's 128'th patient); his message was sent on January 16, 1998 and entitled "Infinite universe and many worlds".
John K Clark See what's on my new list at Extropolis
fhf
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On Sun, Jan 05, 2025 at 04:47:00PM -0800, Brent Meeker wrote:
>
> What he fails to explain is how probabilities are realized in these worlds. As
> Bruce pointed out, except for 50-50 cases the overwhelming number of worlds
> find QM to be empirically falsified; so branch counting doesn't work. It
> appears that the Born rule adds another axiom; it's not just the Schroedinger
> equation.
>
> Brent
>
Bruce's argument is too coarse. He is assuming that all worlds have
equal representation in the original experimental preparation, whereas
the preparation process can clearly set things up such that there is
90% up 10% down in the original sample, after which measurement is
performed. "Branch counting" can easily explain something like the
90/10 Stern Gerlach case.
Where things fail is explaining something like the violation of Bell's
inequality. I originally thought I had an answer to that, but after
surface from the rabbit hole of maths, I realised I had to think again
:).
On Sun, Jan 5, 2025 at 12:44 AM Bruce Kellett <bhkel...@gmail.com> wrote:
On Sun, Jan 5, 2025 at 7:46 AM John Clark <johnk...@gmail.com> wrote:About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
I watched this video, but it is not as comprehensive as Carroll's book "Something Deeply Hidden".
However, something came up in the question period that might warrant a comment. Talking about the Born rule, Carroll justifies it by saying that if you measure the spin of 1000 unpolarized particles, you get 2^1000 different UP-DOWN sequences. However, the vast majority of these sequences will show proportions of UP vs DOWN close to the Born rule prediction of 50/50. In the limit, if such a limit makes sense, the proportion of sequences that show marked deviations from the Born Rule proportions will form a set of measure zero, and can be ignored.
That is just the law of large numbers at work, and is all very well if the amplitudes are such that the Born probabilities are equal to 0.5. But it is easy to rotate your S-G magnets so that the Born probabilities are quite different, say, 0.9-Up to 0.1-DOWN. Now take 1000 trials again. According to Everett, you necessarily get the same 2^1000 sequences of UP-DOWN that you had before. The law of large numbers will then tell you that the majority of these will have approximately a 50/50 UP/DOWN split, which is grossly in violation of the Born rule result of a 90/10 split. In other words, MWI. or Everettian QM. has a problem reproducing the Born rule. It works in the simple case of equal probabilities, but fails miserably once one departs substantially from equal probabilities.
Bruce
David Z Albert mentions that if you define a measurement operator that just tells you the *fraction* of spin-up vs. spin-down in a large sequence of identical measurements,
then even without any collapse assumption, in the limit as # measurements goes to infinity the wavefunction will approach an eigenstate of this operator that matches the probability that would be predicted by the Born rule. See his comments on p. 238 of The Cosmos of Science at https://books.google.com/books?id=_HgF3wfADJIC&lpg=PP1&pg=PA238#v=onepage&q&f=false
--
"Then, even though there will actually be no matter of fact about what h takes the outcomes of any of those measurements to be, nonetheless, as the number of those measurements which have already been carried out goes to infinity, the state of the world will approach (not as a merely probabilistic limit, but as a well-defined mathematical epsilon-and-delta-type limit) a state in which the reports of h about the statistical frequency of any particular outcome of those measurements will be perfectly definite, and also perfectly in accord with the standard quantum mechanical predictions about what the frequency out to be."
Jesse
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On Sun, Jan 5, 2025 at 5:35 PM Bruce Kellett <bhkel...@gmail.com> wrote:
On Mon, Jan 6, 2025 at 9:14 AM Jesse Mazer <laser...@gmail.com> wrote:On Sun, Jan 5, 2025 at 12:44 AM Bruce Kellett <bhkel...@gmail.com> wrote:On Sun, Jan 5, 2025 at 7:46 AM John Clark <johnk...@gmail.com> wrote:About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
I watched this video, but it is not as comprehensive as Carroll's book "Something Deeply Hidden".
However, something came up in the question period that might warrant a comment. Talking about the Born rule, Carroll justifies it by saying that if you measure the spin of 1000 unpolarized particles, you get 2^1000 different UP-DOWN sequences. However, the vast majority of these sequences will show proportions of UP vs DOWN close to the Born rule prediction of 50/50. In the limit, if such a limit makes sense, the proportion of sequences that show marked deviations from the Born Rule proportions will form a set of measure zero, and can be ignored.
That is just the law of large numbers at work, and is all very well if the amplitudes are such that the Born probabilities are equal to 0.5. But it is easy to rotate your S-G magnets so that the Born probabilities are quite different, say, 0.9-Up to 0.1-DOWN. Now take 1000 trials again. According to Everett, you necessarily get the same 2^1000 sequences of UP-DOWN that you had before. The law of large numbers will then tell you that the majority of these will have approximately a 50/50 UP/DOWN split, which is grossly in violation of the Born rule result of a 90/10 split. In other words, MWI. or Everettian QM. has a problem reproducing the Born rule. It works in the simple case of equal probabilities, but fails miserably once one departs substantially from equal probabilities.
Bruce
David Z Albert mentions that if you define a measurement operator that just tells you the *fraction* of spin-up vs. spin-down in a large sequence of identical measurements, then even without any collapse assumption, in the limit as # measurements goes to infinity the wavefunction will approach an eigenstate of this operator that matches the probability that would be predicted by the Born rule. See his comments on p. 238 of The Cosmos of Science at https://books.google.com/books?id=_HgF3wfADJIC&lpg=PP1&pg=PA238#v=onepage&q&f=false
"Then, even though there will actually be no matter of fact about what h takes the outcomes of any of those measurements to be, nonetheless, as the number of those measurements which have already been carried out goes to infinity, the state of the world will approach (not as a merely probabilistic limit, but as a well-defined mathematical epsilon-and-delta-type limit) a state in which the reports of h about the statistical frequency of any particular outcome of those measurements will be perfectly definite, and also perfectly in accord with the standard quantum mechanical predictions about what the frequency out to be."
But then Albert goes on to say that there are all sorts of reasons why this simple theory cannot be the answer to the origin of the Born rule. I have pointed out one of the most cogent of these. If you perform similar measurements on N identically prepared systems (say z-spin measurements on systems prepared in an x-spin-left state), then according to Everett, you get all 2^N possible sequences of UP/DOWN spins. This exhausts the possibilities for the outcome of N trials, and, significantly, you must get exactly the same 2^N sequences whatever the amplitudes of the initial superposition might be. So you get these 2^N sequences if the amplitudes are equal, and also if the amplitudes are in the ratio 0.9/0.1. This behaviour is incompatible with the Born rule, and hence with ordinary quantum mechanics.
You do get all these sequences but this tells us nothing about what their relative probabilities/frequencies are. I assume as an extension of his analysis, if we did repeated experiments where on each trial we performed exactly N measurements and this was repeated over many trials (approaching infinity), then you could define a measurement operator that would tell you the fraction with any specific N-sequence (for example, for N=3 there would be an operator giving the fraction of trials with result 000, likewise other operators for 001 and 010 and 011 and 100 and 101 and 110 and 111). If you had a setup where the relative probability of these sequences was not uniform according to the Born rule,
then if the number of trials with that setup goes to infinity, it will presumably likewise be true that the state approaches the eigenstate of this operator with the frequency predicted by the Born rule, without ever actually invoking the Born rule.
Albert would presumably say that this still doesn't resolve the measurement problem because it doesn't give an outcome on any particular trial, only a sort of aggregate over many trials, but this is different from the criticism you are making. Even if we do use the Born rule in the above scenario, it's still true that each of the specific outcomes that are possible for a given trial with N measurements (eg the outcomes 000, 001, 010, 011, 100, 101, 110, and 111) will occur in the long term, but that doesn't mean they are equiprobable.
--
Jesse
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Thus, the operator that Albert talks about does not give the relative probabilities for each sequence.
Actually, Albert is talking about the case where there is only one outcome for each measurement.
On 1/4/2025 11:45 PM, Alan Grayson wrote:
On Saturday, January 4, 2025 at 8:06:38 PM UTC-7 Alan Grayson wrote:
On Saturday, January 4, 2025 at 2:11:02 PM UTC-7 Alan Grayson wrote:On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN. And please don't offer your BS that you've answered it repeatedly. Such a claim would be blatent lie. Finally, I know what you haven't offered the answer. It's really simple. You don't want to admit the Emperor has no clothes, as such an admission might trigger a coronary when you realize you've been preaching a lie these many years. AGI watched it. I can't say I fully understand it or believe it. I'll probably watch it again. I do know that lately I am less impressed with the cat experiment, as I recall a recent comment by Brent; that there's no operator which has Alive and Dead as its eigenvalues. This, IMO, means that the cat's wf isn't a valid quantum wf. AG
You're misinterpreting what I wrote. I meant that being alive is a superposition of a bazillion of different wave functions so it is impossible to formulate a measurement operator which will return just one of two values that actually correspond to Alive and Dead. In other words the exist a range of states that count as alive, some of which are dying, and a range of states that would count at dead, but some of which are recovering. It doesn't mean there is no WF of the cat. I means that alive and dead are only well defined in the extreme cases because the cat has many intermediate states which we can't account for in our measurement operator.
If the cat's wf isn't a valid wf in QM, which is now my belief, does the same apply to Decayed and Undecayed? That is, what is the operator which has Decayed and Undecayed as it eigenvalues? AGNo, for a simple particle or atom the decayed and undecayed states are well enough know that we can create measurement operators.
Another question relates to the superposition which involves the Environment. Carroll claims the observer is contained in this superposition as part of the Environment without experience it's in such a state. Is this the origin of the Many Worlds in the MWI? If so, this seems independent of S's equation, and follows directly from the quantum definition of the wf as a linear sum of eigenvalues. AG
Eigenvalues of what...of the Schroedinger equation (including a measurement interaction).
Brent
On 1/4/2025 11:45 PM, Alan Grayson wrote:
You're misinterpreting what I wrote. I meant that being alive is a superposition of a bazillion of different wave functions so it is impossible to formulate a measurement operator which will return just one of two values that actually correspond to Alive and Dead. In other words the exist a range of states that count as alive, some of which are dying, and a range of states that would count at dead, but some of which are recovering. It doesn't mean there is no WF of the cat. I means that alive and dead are only well defined in the extreme cases because the cat has many intermediate states which we can't account for in our measurement operator.
On Saturday, January 4, 2025 at 8:06:38 PM UTC-7 Alan Grayson wrote:
On Saturday, January 4, 2025 at 2:11:02 PM UTC-7 Alan Grayson wrote:
On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN. And please don't offer your BS that you've answered it repeatedly. Such a claim would be blatent lie. Finally, I know what you haven't offered the answer. It's really simple. You don't want to admit the Emperor has no clothes, as such an admission might trigger a coronary when you realize you've been preaching a lie these many years. AG
I watched it. I can't say I fully understand it or believe it. I'll probably watch it again. I do know that lately I am less impressed with the cat experiment, as I recall a recent comment by Brent; that there's no operator which has Alive and Dead as its eigenvalues. This, IMO, means that the cat's wf isn't a valid quantum wf. AG
On Sun, Jan 5, 2025 at 6:36 PM Bruce Kellett <bhkel...@gmail.com> wrote:
On Mon, Jan 6, 2025 at 10:21 AM Jesse Mazer <laser...@gmail.com> wrote:On Sun, Jan 5, 2025 at 5:35 PM Bruce Kellett <bhkel...@gmail.com> wrote:On Mon, Jan 6, 2025 at 9:14 AM Jesse Mazer <laser...@gmail.com> wrote:On Sun, Jan 5, 2025 at 12:44 AM Bruce Kellett <bhkel...@gmail.com> wrote:On Sun, Jan 5, 2025 at 7:46 AM John Clark <johnk...@gmail.com> wrote:About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
I watched this video, but it is not as comprehensive as Carroll's book "Something Deeply Hidden".
However, something came up in the question period that might warrant a comment. Talking about the Born rule, Carroll justifies it by saying that if you measure the spin of 1000 unpolarized particles, you get 2^1000 different UP-DOWN sequences. However, the vast majority of these sequences will show proportions of UP vs DOWN close to the Born rule prediction of 50/50. In the limit, if such a limit makes sense, the proportion of sequences that show marked deviations from the Born Rule proportions will form a set of measure zero, and can be ignored.
That is just the law of large numbers at work, and is all very well if the amplitudes are such that the Born probabilities are equal to 0.5. But it is easy to rotate your S-G magnets so that the Born probabilities are quite different, say, 0.9-Up to 0.1-DOWN. Now take 1000 trials again. According to Everett, you necessarily get the same 2^1000 sequences of UP-DOWN that you had before. The law of large numbers will then tell you that the majority of these will have approximately a 50/50 UP/DOWN split, which is grossly in violation of the Born rule result of a 90/10 split. In other words, MWI. or Everettian QM. has a problem reproducing the Born rule. It works in the simple case of equal probabilities, but fails miserably once one departs substantially from equal probabilities.
Bruce
David Z Albert mentions that if you define a measurement operator that just tells you the *fraction* of spin-up vs. spin-down in a large sequence of identical measurements, then even without any collapse assumption, in the limit as # measurements goes to infinity the wavefunction will approach an eigenstate of this operator that matches the probability that would be predicted by the Born rule. See his comments on p. 238 of The Cosmos of Science at https://books.google.com/books?id=_HgF3wfADJIC&lpg=PP1&pg=PA238#v=onepage&q&f=false
"Then, even though there will actually be no matter of fact about what h takes the outcomes of any of those measurements to be, nonetheless, as the number of those measurements which have already been carried out goes to infinity, the state of the world will approach (not as a merely probabilistic limit, but as a well-defined mathematical epsilon-and-delta-type limit) a state in which the reports of h about the statistical frequency of any particular outcome of those measurements will be perfectly definite, and also perfectly in accord with the standard quantum mechanical predictions about what the frequency out to be."
But then Albert goes on to say that there are all sorts of reasons why this simple theory cannot be the answer to the origin of the Born rule. I have pointed out one of the most cogent of these. If you perform similar measurements on N identically prepared systems (say z-spin measurements on systems prepared in an x-spin-left state), then according to Everett, you get all 2^N possible sequences of UP/DOWN spins. This exhausts the possibilities for the outcome of N trials, and, significantly, you must get exactly the same 2^N sequences whatever the amplitudes of the initial superposition might be. So you get these 2^N sequences if the amplitudes are equal, and also if the amplitudes are in the ratio 0.9/0.1. This behaviour is incompatible with the Born rule, and hence with ordinary quantum mechanics.
You do get all these sequences but this tells us nothing about what their relative probabilities/frequencies are. I assume as an extension of his analysis, if we did repeated experiments where on each trial we performed exactly N measurements and this was repeated over many trials (approaching infinity), then you could define a measurement operator that would tell you the fraction with any specific N-sequence (for example, for N=3 there would be an operator giving the fraction of trials with result 000, likewise other operators for 001 and 010 and 011 and 100 and 101 and 110 and 111). If you had a setup where the relative probability of these sequences was not uniform according to the Born rule, then if the number of trials with that setup goes to infinity, it will presumably likewise be true that the state approaches the eigenstate of this operator with the frequency predicted by the Born rule, without ever actually invoking the Born rule.
Albert would presumably say that this still doesn't resolve the measurement problem because it doesn't give an outcome on any particular trial, only a sort of aggregate over many trials, but this is different from the criticism you are making. Even if we do use the Born rule in the above scenario, it's still true that each of the specific outcomes that are possible for a given trial with N measurements (eg the outcomes 000, 001, 010, 011, 100, 101, 110, and 111) will occur in the long term, but that doesn't mean they are equiprobable.
The trouble that I have pointed to is that if every possible outcome occurs for each measurement, then the sequences are all present whatever the amplitudes in the wavefunction. so the sequences 000...,001...,010...,100...,011...,... etc are all equiprobable, whatever the wave function.
How do you get from "all present" to "equiprobable"? If you flip a pair of coins enough times you will surely get all the sequences HH, HT, TH and TT, but you could easily be using weighted coins that don't have 50/50 chances of landing heads and tails, in which case those 4 sequences won't occur equally often.Thus, the operator that Albert talks about does not give the relative probabilities for each sequence.
But he's talking very generally about any sort of operator that gives relative frequencies of different results of quantum experiments, so do you disagree that it's plausible this could be generalized to an operator that gives frequencies of different multi-measurement sequences in the way I described? Making N measurements in a row can itself be considered a type of repeatable experiment that has 2^N possible outcomes each time you perform it. And each of those 2^N outcomes would be assigned some probability by the Born rule, so you should be able to design an operator that gives you the frequency of any one of those 2^N outcomes, which may not be equiprobable depending on the experimental setup.
Albert's statement about the wavefunction converging to the correct eigenfunction of such an operator wasn't limited to cases where all outcomes are equiprobable, I can't say for sure but I'd expect his statement would cover this sort of case as well.
Actually, Albert is talking about the case where there is only one outcome for each measurement.
He doesn't specify that each "outcome" has to be a single spin measurement though. There's also another presentation of the same idea (apparently called 'Mittelstaedt’s theorem') starting on p. 13 at https://www.academia.edu/6975159/Quantum_dispositions_and_the_notion_of_measurement and it seems to be stated in a very general way, talking about an operator that gives "the relative frequency of the outcome a_k in a given sequence of N outcomes" without placing any conditions on an "outcome" only involving a single particle measurement.
Jesse
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On Sun, Jan 5, 2025 at 6:56 PM Brent Meeker <meeke...@gmail.com> wrote:
On 1/4/2025 11:45 PM, Alan Grayson wrote:
You're misinterpreting what I wrote. I meant that being alive is a superposition of a bazillion of different wave functions so it is impossible to formulate a measurement operator which will return just one of two values that actually correspond to Alive and Dead. In other words the exist a range of states that count as alive, some of which are dying, and a range of states that would count at dead, but some of which are recovering. It doesn't mean there is no WF of the cat. I means that alive and dead are only well defined in the extreme cases because the cat has many intermediate states which we can't account for in our measurement operator.
On Saturday, January 4, 2025 at 8:06:38 PM UTC-7 Alan Grayson wrote:
On Saturday, January 4, 2025 at 2:11:02 PM UTC-7 Alan Grayson wrote:
On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN. And please don't offer your BS that you've answered it repeatedly. Such a claim would be blatent lie. Finally, I know what you haven't offered the answer. It's really simple. You don't want to admit the Emperor has no clothes, as such an admission might trigger a coronary when you realize you've been preaching a lie these many years. AG
I watched it. I can't say I fully understand it or believe it. I'll probably watch it again. I do know that lately I am less impressed with the cat experiment, as I recall a recent comment by Brent; that there's no operator which has Alive and Dead as its eigenvalues. This, IMO, means that the cat's wf isn't a valid quantum wf. AG
In terms of our fuzzy ordinary language this may be true, but in classical mechanics we have the notion of a "macrostate" which is defined as some large set of microstates, can we do something similar in QM and just imagine classifying every possible position eigenstate
as either falling into the macrostate "live cat" or not being a member of that macrostate? (ignoring the practical difficulties of actually going through all the eigenstates and classifying them this way) If we had such a precise definition, could we then define an operator corresponding to the macrostate we had defined? The discussion at https://physics.stackexchange.com/questions/343380/how-is-a-macrostate-specified-in-quantum-statistics seems to indicate that macrostates in QM can be defined as density operators.
Jesse
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On 1/5/2025 7:29 PM, Jesse Mazer wrote:
But what's your assurance that position eigenstates are the ones that provide a binary alive/dead dichotomy? And position of what? Particles...that doesn't work because the particle positions don't define an eigenstate of the whole. It's a feature of QM that measurements are holistic. You have to know what "alive" means in order to measure it.
On Sun, Jan 5, 2025 at 6:56 PM Brent Meeker <meeke...@gmail.com> wrote:
On 1/4/2025 11:45 PM, Alan Grayson wrote:
You're misinterpreting what I wrote. I meant that being alive is a superposition of a bazillion of different wave functions so it is impossible to formulate a measurement operator which will return just one of two values that actually correspond to Alive and Dead. In other words the exist a range of states that count as alive, some of which are dying, and a range of states that would count at dead, but some of which are recovering. It doesn't mean there is no WF of the cat. I means that alive and dead are only well defined in the extreme cases because the cat has many intermediate states which we can't account for in our measurement operator.
On Saturday, January 4, 2025 at 8:06:38 PM UTC-7 Alan Grayson wrote:
On Saturday, January 4, 2025 at 2:11:02 PM UTC-7 Alan Grayson wrote:
On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN. And please don't offer your BS that you've answered it repeatedly. Such a claim would be blatent lie. Finally, I know what you haven't offered the answer. It's really simple. You don't want to admit the Emperor has no clothes, as such an admission might trigger a coronary when you realize you've been preaching a lie these many years. AG
I watched it. I can't say I fully understand it or believe it. I'll probably watch it again. I do know that lately I am less impressed with the cat experiment, as I recall a recent comment by Brent; that there's no operator which has Alive and Dead as its eigenvalues. This, IMO, means that the cat's wf isn't a valid quantum wf. AG
In terms of our fuzzy ordinary language this may be true, but in classical mechanics we have the notion of a "macrostate" which is defined as some large set of microstates, can we do something similar in QM and just imagine classifying every possible position eigenstate
Brent
On 1/4/2025 11:21 PM, Quentin Anciaux wrote:
You think it absurd that you didn't exist in the past and after a finite time you will no longer exist?? Most people, and physicists, think that's the case.
Le dim. 5 janv. 2025, 01:18, Brent Meeker <meeke...@gmail.com> a écrit :
On 1/4/2025 1:11 PM, Alan Grayson wrote:
Basically it boils down to two things. One, they think the Schoredinger equation is sufficient to described measurement so long as the world can separate into independent copies for each eigenvalue of the measurement. Exactly how this separation proceeds and how it is originated is sort of hand wavy, but they're sure it can be squared. Second, they want everything to be deterministic. So having all but one of the world's go away would require randomness per the Born rule. At one time they thought the Born rule was already implict in the Schoredinger equation. But since everything happens it's not so clear what it means that probabilities are equal to the squared amplitude. Probability of what? Not probability of a value happening. Probability of finding oneself in a particular world? How does the probability amplitude of a quantum event get to apply some kind of "weight" to you or to a world? One my say "That's just the way it is. If it's probabilistic then it must follow Born's rule by Gleanson's theorem." But then that's assuming it's probabilistic, not just Schroedinger's equation...in which case why not just bite the bullet and says it's the probability that a particular world exists.
On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN.
Because to me in itself, only one world is absurd... as absurd that my life is finite and preceeded by an infinite time in the past and infinite time in the future...
It's just improbable, which is quite different from absurd. Every hand of bridge I've been dealt was improbable, but I never considered one absurd.I know reality doesn't have to please me, but one world theory is as absurd as absurd can be imo. Only a theory about information where everything exists seems lesz absurd, yeah there is a gazillion things in it, so there is also in one world, thing is with MW like things, there is an explanation for you to be, you're one of the possibilities... in one world, you're one possibilities realised whatever that means against all not realised whatever that means, the realised thing is the absurd.
Brent
----
Quentin
-- All those moments will be lost in time, like tears in rain. Roy Betty, Rutger Hauer--
Brent
--And please don't offer your BS that you've answered it repeatedly. Such a claim would be blatent lie. Finally, I know what you haven't offered the answer. It's really simple. You don't want to admit the Emperor has no clothes, as such an admission might trigger a coronary when you realize you've been preaching a lie these many years. AG0o1
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Le lun. 6 janv. 2025, 00:41, Brent Meeker <meeke...@gmail.com> a écrit :
On 1/4/2025 11:21 PM, Quentin Anciaux wrote:
You think it absurd that you didn't exist in the past and after a finite time you will no longer exist?? Most people, and physicists, think that's the case.
Le dim. 5 janv. 2025, 01:18, Brent Meeker <meeke...@gmail.com> a écrit :
On 1/4/2025 1:11 PM, Alan Grayson wrote:
Basically it boils down to two things. One, they think the Schoredinger equation is sufficient to described measurement so long as the world can separate into independent copies for each eigenvalue of the measurement. Exactly how this separation proceeds and how it is originated is sort of hand wavy, but they're sure it can be squared. Second, they want everything to be deterministic. So having all but one of the world's go away would require randomness per the Born rule. At one time they thought the Born rule was already implict in the Schoredinger equation. But since everything happens it's not so clear what it means that probabilities are equal to the squared amplitude. Probability of what? Not probability of a value happening. Probability of finding oneself in a particular world? How does the probability amplitude of a quantum event get to apply some kind of "weight" to you or to a world? One my say "That's just the way it is. If it's probabilistic then it must follow Born's rule by Gleanson's theorem." But then that's assuming it's probabilistic, not just Schroedinger's equation...in which case why not just bite the bullet and says it's the probability that a particular world exists.
On Saturday, January 4, 2025 at 1:46:26 PM UTC-7 John Clark wrote:
> Moderation is inappropriate where Trump physics is endorsed. AG
About a month ago Sean Carroll uploaded a very good video explaining the Many Worlds theory, but it's over an hour long so I know there's about as much chance of a dilettante such as yourself of actually watching it is there is of you reading a post of mine if it's longer than about 100 words.
John K Clark See what's on my new list at Extropolis
Sure, I'll watch it. But I am still waiting for your reply to my question, posed around 10 times, why, based on S's equation, every thing that can happen, MUST HAPPEN.
Because to me in itself, only one world is absurd... as absurd that my life is finite and preceeded by an infinite time in the past and infinite time in the future...
It's just improbable, which is quite different from absurd. Every hand of bridge I've been dealt was improbable, but I never considered one absurd.I know reality doesn't have to please me, but one world theory is as absurd as absurd can be imo. Only a theory about information where everything exists seems lesz absurd, yeah there is a gazillion things in it, so there is also in one world, thing is with MW like things, there is an explanation for you to be, you're one of the possibilities... in one world, you're one possibilities realised whatever that means against all not realised whatever that means, the realised thing is the absurd.
BrentI understand your analogy with improbable bridge hands, but I think the difference lies in the nature of "improbable" versus "absurd" when we scale it to the entirety of existence. The improbability of any specific bridge hand exists within a defined framework with clear rules and outcomes—it is improbable, but not absurd because we understand the context.In the case of existence, a single-world theory suggests that out of infinite possibilities, only one outcome is "realized." This is not just improbable—it's a rejection of the inherent structure of possibility itself. Without a multiverse or some equivalent explanation, the realization of just one world feels like a singular, unexplained "bridge hand" with no deck, no dealer, and no game. It's the framework itself that becomes suspect.With a many-worlds or "everything exists" perspective, there is a structure that accounts for all possibilities, including the one where "I am." It doesn't feel absurd because existence is distributed across possibilities rather than being inexplicably concentrated into one. The absurdity for me isn't about odds; it's about the lack of explanatory context in a single-world view.Does that make sense?Quentin
On Sunday, January 5, 2025 at 2:25:42 PM UTC-7 Cosmin Visan wrote:@Alan you wouldn't ask such question if you would understand that energy doesn't exist. "Energy" is just an idea in consciousness. All these theories that people create are just random guesses. They work until they don't. Wondering where the energy goes and so on is pointless, for the trivial reason that you go beyond what that guess covered and you are back to square 1 of making another guess.You're a stupid prick. AG
On Sunday, 5 January 2025 at 23:03:50 UTC+2 Alan Grayson wrote:
On Sunday, January 5, 2025 at 2:00:46 PM UTC-7 Alan Grayson wrote:
On Sunday, January 5, 2025 at 1:49:59 PM UTC-7 John Clark wrote:
On Sun, Jan 5, 2025 at 2:45 PM Alan Grayson <agrays...@gmail.com> wrote:> his answer to energy requirements for these new worlds seems weak, that energy is somehow globally conserved while the energy in particular branches can decrease,It doesn't matter if Many Worlds is correct or not, we've known for a century that in an expanding universe, like the one we live in, energy is NOT conserved at the cosmological scale; photons of light gets stretched to the red end of the spectrum and red photons have less energy than blue photons. In fact, unlike classical physics or even special relativity, the very concept of conservation of energy is not rigorously defined in General Relativity. GR does have something called the "stress-energy tensor" that includes contributions from all non-gravitational fields and matter, but gravity is not included. If you're interested Sean Carroll goes into much more detail here:
John K Clark See what's on my new list at Extropolis
How could gravity be included as if it's something different from curvature of spacetime, which is caused by stress-energy tensor? I'm pretty sure Carroll said energy is conserved in the MWI, making it superior to the Copenhagan interpretations. AG
On Mon, Jan 06, 2025 at 12:44:05PM +1100, Bruce Kellett wrote:
> On Mon, Jan 6, 2025 at 12:02 PM Russell Standish <li...@hpcoders.com.au> wrote:
>
> On Sun, Jan 05, 2025 at 04:47:00PM -0800, Brent Meeker wrote:
> >
> > What he fails to explain is how probabilities are realized in these worlds. As
> > Bruce pointed out, except for 50-50 cases the overwhelming number of worlds
> > find QM to be empirically falsified; so branch counting doesn't work. It
> > appears that the Born rule adds another axiom; it's not just the Schroedinger
> > equation.
> >
> > Brent
> >
>
> Bruce's argument is too coarse. He is assuming that all worlds have
> equal representation in the original experimental preparation, whereas
> the preparation process can clearly set things up such that there is
> 90% up 10% down in the original sample, after which measurement is
> performed. "Branch counting" can easily explain something like the
> 90/10 Stern Gerlach case.
>
>
> No, that does not work, even if you make the extreme assumption that
> measurement is a process of discrimination between already existing worlds (a
> point of view for which we have no evidence whatsoever.)
> In Everettian many worlds, every outcome is realized on every trial. So after
> one trial, there are two branches; after two trials, 4 branches; and so on; so
> that after N trials, there are 2^N branches.
Why do you think that just because there are two outcomes (up/down,
say), there will be precisely two branches generated?
It can only be guaranteed if there is a fundamental symmetry in the
system between the two outcomes. That is when you get equal branches
for each outcome.
It is quite easy to concoct an example where 3 branches are up and 1
down, giving a 75/25 ratio. Just perform a second binary measurement
if the down measurement is observed in the first measurement, but just
record if an up was seen in either measurement, or not. This can be
easily generalised to any ratio representable by a finite binary
expansion.
Not sure if you can squeeze the Stern Gerlach experiment into that
role, but my hunch is maybe. Positions of magnets are limited to the accuracy of our rulers and protractors.
But I do suspect that pure branch counting does fail to describe more
complex scenarios, such as Bell inequality violating ones, but I
haven't seriously looked into it.
>> If Many World is correct then ontological randomness can not exist but epistemological randomness certainly can and certainly does.
> It's not just epistemological when it includes the whole world whether anybody else knows it or not.
> QBism is actually an epistemological interpretation
>> you have to explain why Schrodinger's equation suddenly stops working.
> You have to explain when the worlds split
> Measurement doesn't even have to include me or anybody else. The cat example just obfuscates the question. The measurement is done when the detector detects the atomic decay. A cleaner version has a clock stopped by the detection.
> I can see that it will eventually make different orthogonal worlds, only one of which we see. Carroll once joked that non-Everettians needed to explain the disappearing worlds.
> branch counting doesn't work.
> It appears that the Born rule adds another axiom; it's not just the Schroedinger equation.
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> I exist, consciousness exists. There's no question about that, for me.
> in your understanding, what does "to exist" mean ?
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