Re: [New post] Why Probability in Quantum Mechanics is Given by the Wave Function Squared

2014-07-25 Thread Platonist Guitar Cowboy
Thanks for posting, Brent. Fine topics to dig into when one takes the time.

And if we never take the time for these things, how can we ever expect to
derive proper energetic eigenvalues for hydrogen like stuff in the wave
we're surfing on, independent of distracting deadlines?

The hard answer nobody wants to face is: we don't. And the result is we die
as lesser men. For only idiots wait for the right wave, blinking in the
sun. A proper surfer of the fundamental just goes when it's time, surfs
that one right wave, and simultaneously leaves the idiots waiting for the
wave in his wake... forever. Timeless cojones. Not even a contest.

The gender ghost haunts this statement mumbling something about exclusion,
but I just destroyed it before it could finish the sentence.

No time for vain attention sinks or these kinds of silly ghosts. They will
be crushed as they have dangerous property of propagating tedious boredom
broadcast waves, a highly contagious, prevalent, virulent disease of our
time. We shouldn't engage this nonsense; just kill it, walk away, and not
bother to even contemplate looking back.

The wave pushes forward regardless, and laughs at time's ridiculous
routines and dead lines. Born (squared tude) again. PGC


On Thu, Jul 24, 2014 at 8:24 PM, meekerdb meeke...@verizon.net wrote:

  On 7/24/2014 11:09 AM, David Nyman wrote:

  On 24 July 2014 18:40, meekerdb meeke...@verizon.net wrote:

 This may clarify (or provoke) discussion of Moscow vs. Washington.  It's
 interesting that Carroll and Sebens use FPI and Sean says it increases his
 confidence in Everett's MWI.  But in his penultimate paragraph he
 essentially lays out an endorsement of Fuchs QBism, which is generally seen
 as the instrumentalist alternative to MWI.


 Brent, could you possibly summarise what you see as the essential
 distinction between the CS and Fuchs alternatives for dummies?


 I'd need to study CS's paper a little, I just read Sean's blog summary.
 But Fuch's quantum Bayesianism says that the collapse of the wave function
 is just like the collapse of a classical probability distribution when we
 learn the value of the random variable.  It's purely epistemic.  It's a
 sort of instrumentalism.

 Brent

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Re: [New post] Why Probability in Quantum Mechanics is Given by the Wave Function Squared

2014-07-25 Thread Bruno Marchal


On 24 Jul 2014, at 19:40, meekerdb wrote:

This may clarify (or provoke) discussion of Moscow vs. Washington.   
It's interesting that Carroll and Sebens use FPI and Sean says it  
increases his confidence in Everett's MWI.  But in his penultimate  
paragraph he essentially lays out an endorsement of Fuchs QBism,  
which is generally seen as the instrumentalist alternative to MWI.



The universal machine does that too.

Eventually all mode of existence are psychological, as you can guess  
by interpreting physics as the inside view of the arithmetical FPI  
undetermined machine. The observable (roughly the []p  p ( p)  
hypostases (with p sigma_1) are mental, or machine self- 
referencial modalities.


We just don't know yet if those dreams glue enough to determine a  
multiverse or a multi-multiverse, has filtered from what at the start  
his a giant web of (machine) dreams emulated in arithmetic.


Nice post. I like Born, even when wrong. I appreciate the Born- 
Einstein dialog.


Nice way to call the Copenhagen theory: the theory of disappearing  
universes, it is already closer to the brain filtration of realities,  
or consciousness differentiation.


Bruno




Brent


 Original Message 
Subject:	[New post] Why Probability in Quantum Mechanics is Given by  
the Wave Function Squared

Date:   Thu, 24 Jul 2014 15:21:04 +
From:   Sean Carroll donotre...@wordpress.com
To: meeke...@verizon.net


New post on Sean Carroll


Why Probability in Quantum Mechanics is Given by the Wave Function  
Squared

by Sean Carroll
One of the most profound and mysterious principles in all of physics  
is the Born Rule, named after Max Born. In quantum mechanics,  
particles don't have classical properties like position or  
momentum; rather, there is a wave function that assigns a  
(complex) number, called the amplitude, to each possible  
measurement outcome. The Born Rule is then very simple: it says that  
the probability of obtaining any possible measurement outcome is  
equal to the square of the corresponding amplitude. (The wave  
function is just the set of all the amplitudes.)


Born Rule:

The Born Rule is certainly correct, as far as all of our  
experimental efforts have been able to discern. But why? Born  
himself kind of stumbled onto his Rule. Here is an excerpt from his  
1926 paper:




That's right. Born's paper was rejected at first, and when it was  
later accepted by another journal, he didn't even get the Born Rule  
right. At first he said the probability  
wasequal to the  
amplitude, and only in an added footnote did he correct it to being  
the amplitude squared. And a good thing, too, since amplitudes can  
be negative or even imaginary!


The status of the Born Rule depends greatly on one's preferred  
formulation of quantum mechanics. When we teach quantum mechanics to  
undergraduate physics majors, we generally give them a list of  
postulates that goes something like this:


Quantum states are represented by wave functions, which are vectors  
in a mathematical space called Hilbert space.

Wave functions evolve in time according to the Schrödinger equation.
The act of measuring a quantum system returns a number, known as the  
eigenvalue of the quantity being measured.
The probability of getting any particular eigenvalue is equal to the  
square of the amplitude for that eigenvalue.
After the measurement is performed, the wave function collapses to  
a new state in which the wave function is localized precisely on the  
observed eigenvalue (as opposed to being in a superposition of many  
different possibilities).
It's an ungainly mess, we all agree. You see that the Born Rule is  
simply postulated right there, as #4. Perhaps we can do better.


Of course we can do better, since textbook quantum mechanics is an  
embarrassment. 
There are other formulations, and you know that my own favorite is  
Everettian (Many-Worlds) quantum mechanics. (I'm sorry I was too  
busy to contribute to the active comment thread on that post. On the  
other hand, a vanishingly small percentage of the 200+ comments  
actually addressed the point of the article, which was that the  
potential for many worlds is automatically there in the wave  
function no matter what formulation you favor. Everett simply takes  
them seriously, while alternatives need to go to extra efforts to  
erase them. As Ted Bunn argues, Everett is just quantum mechanics,  
while collapse formulations should be called disappearing-worlds  
interpretations.)


Like the textbook formulation, Everettian quantum mechanics also  
comes with a list of postulates. Here it is:


Quantum states are represented by wave functions, which are vectors  
in a mathematical space called Hilbert space.

Wave functions evolve in time according to the Schrödinger equation.
That's it! Quite a bit simpler -- and the two 

Re: [New post] Why Probability in Quantum Mechanics is Given by the Wave Function Squared

2014-07-25 Thread Bruno Marchal


On 24 Jul 2014, at 20:24, meekerdb wrote:


On 7/24/2014 11:09 AM, David Nyman wrote:

On 24 July 2014 18:40, meekerdb meeke...@verizon.net wrote:

This may clarify (or provoke) discussion of Moscow vs. Washington.   
It's interesting that Carroll and Sebens use FPI and Sean says it  
increases his confidence in Everett's MWI.  But in his penultimate  
paragraph he essentially lays out an endorsement of Fuchs QBism,  
which is generally seen as the instrumentalist alternative to MWI.


Brent, could you possibly summarise what you see as the essential  
distinction between the CS and Fuchs alternatives for dummies?


I'd need to study CS's paper a little, I just read Sean's blog  
summary.  But Fuch's quantum Bayesianism says that the collapse of  
the wave function is just like the collapse of a classical  
probability distribution when we learn the value of the random  
variable.  It's purely epistemic.  It's a sort of instrumentalism.


It would be purely epistemic if it made not the universe disappearing.  
But why postulate universe(s) at the start?  We know only that there  
are person(s), and some agreements on 0, 1, 2, 3, ...


Bruno





Brent

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http://iridia.ulb.ac.be/~marchal/



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Fwd: [New post] Why Probability in Quantum Mechanics is Given by the Wave Function Squared

2014-07-24 Thread meekerdb
This may clarify (or provoke) discussion of Moscow vs. Washington.  It's interesting that 
Carroll and Sebens use FPI and Sean says it increases his confidence in Everett's MWI.  
But in his penultimate paragraph he essentially lays out an endorsement of Fuchs QBism, 
which is generally seen as the instrumentalist alternative to MWI.


Brent


 Original Message 
Subject: 	[New post] Why Probability in Quantum Mechanics is Given by the Wave Function 
Squared

Date:   Thu, 24 Jul 2014 15:21:04 +
From:   Sean Carroll donotre...@wordpress.com
To: meeke...@verizon.net



WordPress.com
Sean Carroll posted: One of the most profound and mysterious principles in all of physics 
is the Born Rule, named after Max Born. In quantum mechanics, particles don't have 
classical properties like position or momentum; rather, there is a wave function that 
assigns a (co



   New post on *Sean Carroll*



http://www.preposterousuniverse.com/blog/?author=4  


   Why Probability in Quantum Mechanics is Given by the Wave Function Squared
   
http://www.preposterousuniverse.com/blog/2014/07/24/why-probability-in-quantum-mechanics-is-given-by-the-wave-function-squared/

by Sean Carroll http://www.preposterousuniverse.com/blog/?author=4

One of the most profound and mysterious principles in all of physics is the Born Rule 
http://en.wikipedia.org/wiki/Born_rule, named after Max Born. In quantum mechanics 
http://www.preposterousuniverse.com/eternitytohere/quantum/, particles don't have 
classical properties like position or momentum; rather, there is a wave function 
http://en.wikipedia.org/wiki/Wave_function that assigns a (complex) number, called the 
amplitude, to each possible measurement outcome. The Born Rule is then very simple: it 
says that the probability of obtaining any possible measurement outcome is equal to the 
square of the corresponding amplitude. (The wave function is just the set of all the 
amplitudes.)


*Born Rule:* \mathrm{Probability}(x) = |\mathrm{amplitude}(x)|^2.

The Born Rule is certainly correct, as far as all of our experimental efforts have been 
able to discern. But why? Born himself kind of stumbled onto his Rule. Here is an excerpt 
from his 1926 paper 
http://hermes.ffn.ub.es/luisnavarro/nuevo_maletin/Born_1926_statistical_interpretation.pdf:


Born Rule 
http://www.preposterousuniverse.com/blog/wp-content/uploads/2014/07/bornrule.jpeg

That's right. Born's paper was rejected at first, and when it was later accepted by 
another journal, he didn't even get the Born Rule right. At first he said the probability 
was equal to the amplitude, and only in an added footnote did he correct it to being the 
amplitude squared. And a good thing, too, since amplitudes can be negative or even imaginary!


The status of the Born Rule depends greatly on one's preferred formulation of quantum 
mechanics 
http://www.preposterousuniverse.com/blog/2014/05/29/quantum-mechanics-smackdown/. When 
we teach quantum mechanics to undergraduate physics majors, we generally give them a list 
of postulates that goes something like this:


1. Quantum states are represented by wave functions, which are vectors in a 
mathematical
   space called Hilbert space http://en.wikipedia.org/wiki/Hilbert_space.
2. Wave functions evolve in time according to the Schrödinger equation
   http://en.wikipedia.org/wiki/Schr%C3%B6dinger_equation.
3. The act of measuring a quantum system returns a number, known as the 
eigenvalue
   http://en.wikipedia.org/wiki/Eigenvalues_and_eigenvectors of the quantity 
being
   measured.
4. The probability of getting any particular eigenvalue is equal to the square 
of the
   amplitude for that eigenvalue.
5. After the measurement is performed, the wave function collapses to a new 
state in
   which the wave function is localized precisely on the observed eigenvalue 
(as opposed
   to being in a superposition of many different possibilities).

It's an ungainly mess, we all agree. You see that the Born Rule is simply postulated right 
there, as #4. Perhaps we can do better.


Of course we can do better, since textbook quantum mechanics is an embarrassment 
http://www.washingtonpost.com/blogs/wonkblog/wp/2013/02/07/quantum-mechanics-is-an-embarrassment/. 
There are other formulations, and you know that my own favorite is Everettian 
(Many-Worlds) quantum mechanics 
http://www.preposterousuniverse.com/blog/2014/06/30/why-the-many-worlds-formulation-of-quantum-mechanics-is-probably-correct/. 
(I'm sorry I was too busy to contribute to the active comment thread on that post. On the 
other hand, a vanishingly small percentage of the 200+ comments actually addressed the 
point of the article, which was that the potential for many worlds is automatically there 
in the wave function no matter what formulation you favor. Everett simply takes them 
seriously, while alternatives need to go to extra efforts to erase them. As Ted Bunn 
argues 

Re: [New post] Why Probability in Quantum Mechanics is Given by the Wave Function Squared

2014-07-24 Thread David Nyman
On 24 July 2014 18:40, meekerdb meeke...@verizon.net wrote:

This may clarify (or provoke) discussion of Moscow vs. Washington.  It's
 interesting that Carroll and Sebens use FPI and Sean says it increases his
 confidence in Everett's MWI.  But in his penultimate paragraph he
 essentially lays out an endorsement of Fuchs QBism, which is generally seen
 as the instrumentalist alternative to MWI.


Brent, could you possibly summarise what you see as the essential
distinction between the CS and Fuchs alternatives for dummies?

David

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Re: [New post] Why Probability in Quantum Mechanics is Given by the Wave Function Squared

2014-07-24 Thread meekerdb

On 7/24/2014 11:09 AM, David Nyman wrote:

On 24 July 2014 18:40, meekerdb meeke...@verizon.net 
mailto:meeke...@verizon.net wrote:

This may clarify (or provoke) discussion of Moscow vs. Washington. It's 
interesting
that Carroll and Sebens use FPI and Sean says it increases his confidence in
Everett's MWI.  But in his penultimate paragraph he essentially lays out an
endorsement of Fuchs QBism, which is generally seen as the instrumentalist
alternative to MWI.

Brent, could you possibly summarise what you see as the essential distinction between 
the CS and Fuchs alternatives for dummies?


I'd need to study CS's paper a little, I just read Sean's blog summary.  But Fuch's 
quantum Bayesianism says that the collapse of the wave function is just like the 
collapse of a classical probability distribution when we learn the value of the random 
variable.  It's purely epistemic.  It's a sort of instrumentalism.


Brent

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