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watsonea4
I'm having a bit of a brain fart. I am a very casual student of quantum psychics/mechanics so I will not claim any sort of knowledge, but I'm sure there's a principle basically stating that you cannot assume anything about anything unless you're observing it. I thought it was the Heisenberg uncertainty principle, but I couldn't find a layman description that really stated it like that, so I didn't want to misspeak when I referenced it. I'd like to find the exact verbiage if possible.


Thank you!
BigDumbWeirdo
QUOTE (watsonea4+Dec 17 2007, 11:46 AM)
I'm having a bit of a brain fart. I am a very casual student of quantum psychics/mechanics so I will not claim any sort of knowledge, but I'm sure there's a principle basically stating that you cannot assume anything about anything unless you're observing it. I thought it was the Heisenberg uncertainty principle, but I couldn't find a layman description that really stated it like that, so I didn't want to misspeak when I referenced it. I'd like to find the exact verbiage if possible.


Thank you!

Well, the Heisenberg Uncertainty principle says that the precision with which you know one attribute of a particle is inversly proportionate to the precision with which you know other attributes. So the more precisely you measure it's speed, the less precisely you can measure it's trajectory.
What you're referring to seems to be to be the most basic tenent of skepticism, a quality that is virtually required in anyone attempting to do theoretical or experimental physics. Others on this site might be able to help more, however. Look for answers from the following (this list is not complete,)
Dallas
AlphaNumeric
mr_homm
rpenner
Euler
BenTheMan,
and check out this site:
Wikipedia - Uncertainty Principle
mr_homm
I think the principle involved is simply the "Copenhagen interpretation," which among other things states that if you measure a particle and find that it is in state A,you MUST NOT assume that a particle was actually already in the state A before you measured it. In other words, the state of a particle is indefinite prior to observation, contrary to classical physics. This was the core point to which Einstein objected, because he saw it as denying the objective reality of events.

Hope that helps!

--Stuart Anderson
dawn
watsonea4, all,

I agreed mr_homm well stated.

As you see I am not on the list plus new on this forum resulting from a much needed break, but may I interject something for your consideration. Not to take away anything said above please take a note of this.

I would use caution using the term observer because of bias. I believe you would be hard pressed to make a real distinction between a passive observer (looking into the sky through a telescope) and an active observer like someone who might deliberately manipulate (it does happen in experiment's) and then takes note of what happens using what we call adjustments.

So using "observer" should not always be taken to mean a conscious being (our interaction collapsing a wave function).

It just as well designate a recording device or measuring instrument, or even something like different layers of the earths, which were existing before us. I am keenly aware of the philosophical implications this can bring, I choose not to travel this road.

Something to think about dealing with your research on observation using the uncertainty theory as a consideration.

dawn
e52rgr75@ms.com
I have a question on my mind. Sorry if I have breached any kind of protocol, but this is my first time on a message board of any kind.

What would happen to an object that could move, all directions instantaneously canceling out all relative motion between itself and everything else in the universe?

And know I'm not talking about blowing something up. Its the cancellation of all relative motion that important.
BigDumbWeirdo
QUOTE (dawn+Dec 17 2007, 03:14 PM)
I am keenly aware of the philosophical implications this can bring, I choose not to travel this road.

I don't see much in the way of philosophical implications, if you truly understand the act of observation, (which you seem to.)
It's not so much observation as it is interference. You're slamming the particle against a film, or bombarding it with photons or electrons, not merely "looking at it" the way most people think of it. I've never seen any evidence to suggest that it's not this interference which is responsible for wave-function collapse, although I would be interested in seeing such evidence.
I don't understand why there are so many works out there like What the Bleep Do We Know!? that so obviously misinterpret wave-function collapse as somehow requiring an intelligent person to achieve. There have been many experiments in the lab (A simple example of one would be the double slit experiment with a sheet of cardboard covering the readout which displays which slit the particle passed through) which demonstrate that such is not the case...
Ron
QUOTE (BigDumbWeirdo+Jan 11 2008, 04:40 PM)
I don't see much in the way of philosophical implications, if you truly understand the act of observation, (which you seem to.)
It's not so much observation as it is interference. You're slamming the particle against a film, or bombarding it with photons or electrons, not merely "looking at it" the way most people think of it. I've never seen any evidence to suggest that it's not this interference which is responsible for wave-function collapse, although I would be interested in seeing such evidence.
I don't understand why there are so many works out there like What the Bleep Do We Know!? that so obviously misinterpret wave-function collapse as somehow requiring an intelligent person to achieve. There have been many experiments in the lab (A simple example of one would be the double slit experiment with a sheet of cardboard covering the readout which displays which slit the particle passed through) which demonstrate that such is not the case...

Hi BDW, Dawn,
I think Dawn was making a subtle yet important point to others less acquainted with this stuff than you. I see your 'garbage' as just that also, but there are many (too many in my opinion) that try to muddle the Copenhagen interpretation with philosophy, and I also will not travel that road!
Peace,
Ron
Good Elf
Hi Mr Homm, BigDumbWeirdo, Dawn, Ron, e52rgr75@ms.com et al,

The idea of the Copenhagen Interpretation seems "out of date" in the light of non-local effects... how can entanglement occur between two photons if they do not have a "state" before either one of them is actually detected? The fact that they are entangled before they are detected must be telling us the two particles have a history. Are we saying that the two photons become entangled only when we read one of them? If "no" then they are always entangled right from the start and so they have pre-existing quantum states before they were detected... a history. If "yes" then how did these two particles become entangled without incurring a "history"? Any quantum particle with a "history" violates the primary quantum postulate that quantum particles are indistinguishable. If you can tell them apart then Bohr is wrong about quantum states.

Comments welcome!

Cheers
BigDumbWeirdo
QUOTE (Good Elf+Jan 14 2008, 02:03 AM)
Hi Mr Homm, BigDumbWeirdo, Dawn, Ron, e52rgr75@ms.com et al,

The idea of the Copenhagen Interpretation seems "out of date" in the light of non-local effects... how can entanglement occur between two photons if they do not have a "state" before either one of them is actually detected? The fact that they are entangled before they are detected must be telling us the two particles have a history. Are we saying that the two photons become entangled only when we read one of them? If "no" then they are always entangled right from the start and so they have pre-existing quantum states before they were detected... a history. If "yes" then how did these two particles become entangled without incurring a "history"?  Any quantum particle with a "history" violates the primary quantum postulate that quantum particles are indistinguishable. If you can tell them apart then Bohr is wrong about quantum states.

Comments welcome!

Cheers

It has been my understanding that there is a mechanism in String Theory which explains entanglement in terms which are completely compatible with the Copenhagen Interpretation, however I have never been given an explanation of what that mechanism is or how it works. I have also never seen corroboration of such a claim, so while I trust the source, I'm not completely sure he wasn't in error on this point. I would welcome input from mr_homm or AlphaNumeric in this point.
mr_homm
Hi everybody,

OK, here's the post about the Copenhagen interpretation that I promised to BDW some days ago. I'm going to talk about my opinions here, so this should not be taken as an authoritative pronouncement about standard practices! Also, I've been working on this in spare moments for a couple of days now, and it has grown lllooonnnggg, so I'm going to post it in installments. Today I'll post the first part, which is a general introduction and discussion of the uncertainty principle. Tomorrow I'll post about the uncertainty principle, then next about the Copenhagen interpretation, and finally how my point of view on both of them together fits into the big picture. By the way, some of this material is reworked from posts I made a year or so ago in the circular polarization thread, so if you've read that you may recognize some of this. On the other hand, most of it is new, so I'm not just recycling old stuff to fluff up my post count. wink.gif

I'll talk about both the uncertainty principle and the Copenhagen interpretation, because I think that they both miss the mark in similar ways. My aim is to give a psychological critique of the philosophical formulations of these ideas. The basic theme here is "classical prejudice," expectations that are held firmly and unconsiously by physicists, simply because they are human beings who live in and experience the classical face of the world every day.

It is a truism that it is difficult to be radical enough in quantum theory. Both the uncertainty principle and the Copehnagen interpretation attempt to be extremely radical by removing certainty and definiteness from the universe altogether in order to account for the predictions of quantum theory. This is certainly a radical departure from the tight determinism of classical physics, but I submit that it was the wrong radical departure.

It was, paradoxically, the most conservative radical departure available to Bohr and Heisenberg, because it conserved the classical concepts and meanings of position and momentum, or in general of the state of motion of an object. Rather than revising these classical concepts, a limitation was placed on them; in the case of the uncertainty principle, complementary variables cannot both be precisely measured at once, and in the case of the Copenhagen interpretation, the state of motion of an object becomes definite only upon observation. Both state, in effect, that there is something you cannot know: the variable you did not measure, or the state of the system prior to measurement. Neither denies the classical meaning of these pieces of information, but both deny them a definite value.

Although from a modern perspective, it is possible to regard these interpretations as conceptually conservative, they were in their time amazingly bold revisions, considering that classical deterministic physics had been extremely successful for centuries. The concepts of classical physics are every physicist's comfort zone, because they correspond immediately to our everyday experience, and because they form the backbone of our education. There is a limit to how far even the boldest thinkers can move out of their comfort zones; Bohr and Heisenberg arranged their interpretations to conserve the meaning of the classical concepts at the expense of limiting what can be regarded as determinate. Today, we have lived with quantum mechanics for a century, and the comfort zone has expanded somewhat.

So much for the psychological basis for Bohr's and Heisenberg's interpretations of quantum mechanics; now let's look at the philosophical tools available to them and how these tools were used to build up their interpretations step by step. Like every other well-trained European academic of the early 20th century, both Bohr and Heisenberg had a solid grounding in philosophy, and would have been aware of the ideas of phenomenology (theory of preception), epistemology (theory of knowledge) and ontology (theory of existence). Both the uncertainty principle and the Copenhagen interpretation arise by the process of taking phenomenology very literally (if you did not look at it, you did not see it), applying this to epistemology (if you did not see it, you do not know it), and projecting the result into ontology via a universal principle (if you cannot in principle ever know it, then saying it exists is nonsensical).

For the uncertainty principle, the process looks like this: If you measure the position of a particle, then quantum mechanics says you cannot also measure its momentum. Therefore, if you know its position, you cannot know its momentum. Therefore, it makes no sense to say it even has a definite value of momentum. For the Copenhagen interpretation, the process looks like this: If you measure a particle for the first time at time t, then it is logically impossible for you to have measured it at an earlier time. Therefore, you do not know what state it was in prior to time t. Therefore, if you first measure a particle at time t, you can never know its state prior to t. Therefore, since you cannot even in principle know its state prior to t, it makes no sense to say that it was in a definite state then.

I have done my best here to show that the uncertainty principle and the Copenhagen interpretation are bold, logical, and appealing ideas. They are refreshing, with a sense of blowing old cobwebs away. But -- there is always a "but" -- that does not mean they are the only or even the best solution.

Now let's pass on to how I look at things, starting with the uncertainty principle. To me, the uncertainty principle is just a very bad name for a fundamental fact, and the fact is that the universe contains exactly half the information that we classically expect it to contain. Where we would expect two independent pieces of information (such as position and momentum) there is only one, which we can measure as position or as momentum.

(This reminds me of an anecdote about ancient astronomy: for centuries, the morning star and the evening star were thought to be two different planets. Eventually people realized that you never saw them together, and that there was really one planet, Venus. Venus is sometimes the morning star and sometimes the evening star, and at other times, it is in a different area of its orbit, and it is neither. Position and momentum are like that: two extreme aspects of one deeper thing, which also has many other aspects that are neither position nor momentum, but some mixture of the two that we usually don't think about.)

We are merely spoiled by growing up in the luxury of a large scale, high energy part of the universe. With large objects, you don't need to measure the position all that precisely in order for the error in measurement to be very small relative to the size of the object, and with large momenta, you don't need to measure the momentum all that precisely in order for the error in measurement to be very small relative to the momentum of the object. When we measure position to a (low) classical accuracy, we force a small quantity of the object's information to be position information, but there is still a lot of information left, so we go ahead and measure the momentum as well and we don't notice. Similarly, when we measure momentum, we slightly reduce the avaiable amount of position information and don't notice. And so, since we are living in the world of large objects, we expect to be able to "have our cake and eat it too." The universe is not "hiding" information from us; rather, we are falsely expecting to get information that is not really there. That's why hidden variable interpretations of quantum mechanics are simply silly.

I can explain this best with a parable: we are like a rich man who has so much money that every time he pulls money out of his wallet, there is still money in the wallet, so he has always dollars in his hand and dollars in his wallet. Now he becomes poor and has only one dollar. When he pulls it out, he is puzzled because there is now not a dollar in his wallet anymore. Where did it go? Shouldn't there be a dollar in his hand AND a dollar in his wallet? That's the way it always worked when he was rich! He puts the dollar back, and now he doesn't have a dollar in his hand. Again, he is puzzled; where did the dollar in his hand go? There is some kind of weird "uncertainty principle" that only shows up when you are poor: you can have the dollar in your wallet or the dollar in your hand, but not both. How strange. The universe must be hiding the other dollar from him. Perhaps if he pulls it out gently enough, he will find that there is still a dollar in his wallet too ... no, it didn't work.

The rich man seems very silly, not to understand that a single dollar cannot be in two places at once, but all he is doing is going by his own experience: all his life he has been so rich that there were always many dollars in his wallet and in his hand, and so the either/or behavior of the single dollar never became obvious to him.

Physics is in the same position. We have always previously measured large objects consisting of many particles, and containing plenty of information. There was always enough information in the object to let us specify its position and momentum very accurately, never noticing that there was any conflict between the two measurements. But when we measure a single particle, it has only a single piece of information describing it. Should we choose to look at this information as position? Then the object gives us all the information it has, and it gives it to us in the form of position. It does not have any more information to give, so we cannot also ask its momentum. Similarly, if we choose to look at the information as momentum, we cannot then ask about position. The dollar is either in the wallet or in the hand, and it can't be both places at once, and there are not any "hidden dollars."

My way of expressing it may be a bit unusual, but my opinion is really pretty much in line with the mainstream opinion in physics regarding the uncertainty principle. I just think that people don't take the principle far enough. Calling it "uncertainty" invites misinterpretation, even among physicists. We simply have to get over the idea that there is an unlimited amount of information out there to be measured. The emphasis placed on measurement in most explanations of the uncertainty principle is also very misleading, because it makes the principle into a measurement issue. It is not; it is an information issue. It should really be called the "limited information principle."

It applies to many other measurements besides position and momentum -- any "noncommuting pair of observables" is really one piece of information with two classical faces. The principle also works just the same for any particle. There are even experiments that measure properties of particles indirectly without interacting with the particle at all, and it still turns out that you can't beat the uncertainty principle. There are many different experimental ways of measuring position and momentum (and other pairs of variables), and they all fail in apparently different ways, but all obey the uncertainty principle.

When you see repeated failures, when every experiment fails in its own way, but all fail by the same degree, you start to suspect very strongly that something deeper is going on. Either there is a conspiracy by the universe to make each experiment fail, and by some vast coincidence we are cheated out of knowing both position and momentum, or else there is no conspiracy and no coincidence at all, and the experiments fail, each in its own way, because they are trying to do the impossible: measure information that isn't there. In that case, there is no mystery -- of course they fail, and of course each fails differently because each tries differently to do the impossible.

More later.

--Stuart Anderson
Majkl
QUOTE (mr_homm+Jan 23 2008, 05:41 AM)

When you see repeated failures, when every experiment fails in its own way, but all fail by the same degree, you start to suspect very strongly that something deeper is going on. Either there is a conspiracy by the universe to make each experiment fail, and by some vast coincidence we are cheated out of knowing both position and momentum, or else there is no conspiracy and no coincidence at all, and the experiments fail, each in its own way, because they are trying to do the impossible: measure information that isn't there. In that case, there is no mystery -- of course they fail, and of course each fails differently because each tries differently to do the impossible.

More later.

--Stuart Anderson

In my opinion things are not so much deeper yet no simpler if instead of particles one would search for connections which would be waves and their resonances or oscilations. I also think each different approach to catch the ghost particles fails on the same level. Its like trying to shoot the target from all possible angles which doesnt make any difference to the result except the "exploded" pieces observed. From certain angles you scratch it and from others you shoot right through. Additionaly you are certain you are hitting just one and the same target. Then you discover that when you hit the target next to it affects the first one. You decide to shoot at both simultaneously. You discover that a third one is now being affected. There is no other conclusion than they are directly connected by something else or one of their sub-phases. So are they peaks of the similar or the same wave or compund wave or thus "wavy continuum" or are they discrete and are connected through some kind of hyper-dimensional folded-space?
bm1957
My very simple interpretation of the Uncertainty Principle has always been based on the premise that you need to measure over a period of time to know the momentum accurately but you need to measure at a precise time to know the position accurately at that time. As you approach instantaneous measurement you lose momentum information because it isn't defined at a single instant; as you approach measurement over an infinite time (which would give the most accurate momentum, if it didn't change) you lose position information because the position is no longer defined (assuming the momentum isn't zero).

This is easier to see if you think about the time-energy uncertainty; to know the energy accurately the frequency must be well defined, and this requires the energy state to be maintained for long enough that the cycle completes, otherwise measurement of the frequency is difficult.

But then, my simple interpretation could be based upon any number of misconceptions I hold!
Good Elf
Hi BigDumbWeirdo, mr_homm, bm1957, Majkl, Ron, Dawn, e52rgr75@ms.com et al,

I am impressed with the treatment so far that mr_homm has provided and I do not disagree with any of it. I would like to add an additional perspective to this issue of the Uncertainty Principle and indicate that "uncertainty" is not really what this story is actually about and it is based on a unacknowledged genesis from an earlier age of Fourier Transforms and the way these conjugate variable interact with an underlying "exactitude" which is not immediately extracted from the quantum treatments which are derived from the operation of the instruments of an earlier era. You just know this is going to be controversial since I will always present these points because they are able to throw another light on the issue than the conventional treatment which has been "sanitized" by decades of formalized storytelling in order that doubt and a fixed approach has been instilled in more than one generation of "torch bearers"... My account will not be as "sanitized" nor formalized... this is because nobody is telling this story ... not even to me... wink.gif
QUOTE (mr_homm (Stuart Anderson)+)
When we measure position to a (low) classical accuracy, we force a small quantity of the object's information to be position information, but there is still a lot of information left, so we go ahead and measure the momentum as well and we don't notice. Similarly, when we measure momentum, we slightly reduce the avaiable amount of position information and don't notice. And so, since we are living in the world of large objects, we expect to be able to "have our cake and eat it too." The universe is not "hiding" information from us; rather, we are falsely expecting to get information that is not really there. That's why hidden variable interpretations of quantum mechanics are simply silly.
Here is a document I have found in another place that shows that the relationships between space and time or energy and momentum and other conjugates form "exact pairs" that are interrelated. This interrelationship provides more than the simple discrete relationships if you include additional dimensional aspects to the problem such as additional "holographic information". Have you ever wondered where Heisenberg got his idea for the Uncertainty Principle? Well here it is...
QUOTE
Fourier_Transforms_and_Uncertainty.

...In other words, the probability amplitude distributions of two conjugate variables are simply the (suitably scaled) Fourier transforms of each other. We saw previously that the dispersions (variances) of two density distributions that comprise a Fourier transform pair satisfy the inequality (2), so the variances of the probability amplitude distributions of conjugate observables in quantum mechanics satisfy such an inequality. Thus Heisenberg's uncertainty principle for conjugate pairs of observables follows directly from the fact that those observables are essentially the Fourier transforms of each other.

Of course, this attribute of Fourier transform pairs is purely mathematical, and has no a priori applicability to pairs of observables such as position and momentum, or time and energy. The physical content of quantum mechanics is based on the two relations
  E =h-bar * w p = h-bar K
where E is energy, p is momentum (in one dimension), h-bar is Planck's (reduced) constant, w is the frequency with units second^-1, and k is the wave number with units meter^-1. These relations were introduced in the early 1900's by Planck, Einstein, and deBroglie to account for non-classical phenomena such as cavity radiation and the photo-electric effect, both of which depend on the particle-like behavior of entities that had previously been modeled as waves, as well as phenomena involving wave-like behavior of material particles. These are the relations that associate the familiar observables of energy, momentum, space, and time, with the frequency domain. Indeed in terms of the characteristic time t = 1/w and distance D = 1/k the above relations can be written as
  tE = Dp = h-bar
which already clearly reveals the conjugacy of time and energy, and of distance and momentum. In view of this, it isn't surprising to find that the product of the dispersions of two conjugate observables (such as position and momentum) cannot be less than one quanta of action, represented by h-bar .

In a sense, there is also a conjugacy between space and time - two observable that had been regarded as disjoint and independent prior to the early 1900s. In special relativity the inertial space and time intervals dx and dt between two events are components of a single invariant spacetime interval ds between those events. These intervals are related according to the Minkowski metric, which can be written in the form
{dx/dt + ds/dt}{dx/dt -ds/dt} = 1/c^2

This can be regarded as an "uncertainty relation" for space and time. In general, physics was based, prior to 1900, on the premise that h-bar and 1/c^2 were both zero. With the advent of quantum mechanics and special relativity, it was realized that they both have non-zero values, although they are extremely small in terms of ordinary units.

http://www.mathpages.com/home/kmath488/kmath488.htm

Please note that the reference is to h-bar (reduced Planck's Constant h/4π) not to Planck Length or other units that have become very popular recently... that is an aside.

Now looking at the equation for de Broglie's Matter Wavelength we can see that it relates strongly to Special Relativity and the Lorentz Transformation but considered at low velocity (low energy).
User posted image
In fact it describes the wavelength of particles as v -> 0 and as v -> C. More obviously the dynamics of particles with mass as v -> 0 is the low velocity limit of Special Relativity and as you can see λ -> ∞ as v -> 0. This phenomenon can be seen in BEC's which is a unique window on the interaction of matter and Bose Einstein Statistics in confined spaces.

Regarding the situation where m -> 0 and is subject to any force the acceleration will initially approach infinity (eg. photons). Simply an extension of the equations which relate the mass to the acceleration. Naturally as soon as this action occurs to any particle with finite (non-vanishing mass) the wavelength of any particle that was initially at rest will shrink to approach zero (but never quite reaches it). In the limit of course these events will happen. Big accelerators can hide this low velocity structure of matter and though we "know" that it there we think it can be ignored.. This behavior of inertia-less particles is one reason responsible for photons never moving at less than the speed of light. In the case of light the velocity will reach C but the wavelength will not reach 0 because E = hf.... Where for light f =C/λ. The conjugacy property described above "prevents" λ -> 0 by a factor h.

Now if there is an actual fixed reciprocal relationship between these variables but why is this not seen? Instead we "see" only the simple clicks of the detector providing the detection of events along a plane as shown in this treatment...


QUOTE (->
QUOTE
Fourier_Transforms_and_Uncertainty.

...In other words, the probability amplitude distributions of two conjugate variables are simply the (suitably scaled) Fourier transforms of each other. We saw previously that the dispersions (variances) of two density distributions that comprise a Fourier transform pair satisfy the inequality (2), so the variances of the probability amplitude distributions of conjugate observables in quantum mechanics satisfy such an inequality. Thus Heisenberg's uncertainty principle for conjugate pairs of observables follows directly from the fact that those observables are essentially the Fourier transforms of each other.

Of course, this attribute of Fourier transform pairs is purely mathematical, and has no a priori applicability to pairs of observables such as position and momentum, or time and energy. The physical content of quantum mechanics is based on the two relations
  E =h-bar * w p = h-bar K
where E is energy, p is momentum (in one dimension), h-bar is Planck's (reduced) constant, w is the frequency with units second^-1, and k is the wave number with units meter^-1. These relations were introduced in the early 1900's by Planck, Einstein, and deBroglie to account for non-classical phenomena such as cavity radiation and the photo-electric effect, both of which depend on the particle-like behavior of entities that had previously been modeled as waves, as well as phenomena involving wave-like behavior of material particles. These are the relations that associate the familiar observables of energy, momentum, space, and time, with the frequency domain. Indeed in terms of the characteristic time t = 1/w and distance D = 1/k the above relations can be written as
  tE = Dp = h-bar
which already clearly reveals the conjugacy of time and energy, and of distance and momentum. In view of this, it isn't surprising to find that the product of the dispersions of two conjugate observables (such as position and momentum) cannot be less than one quanta of action, represented by h-bar .

In a sense, there is also a conjugacy between space and time - two observable that had been regarded as disjoint and independent prior to the early 1900s. In special relativity the inertial space and time intervals dx and dt between two events are components of a single invariant spacetime interval ds between those events. These intervals are related according to the Minkowski metric, which can be written in the form
{dx/dt + ds/dt}{dx/dt -ds/dt} = 1/c^2

This can be regarded as an "uncertainty relation" for space and time. In general, physics was based, prior to 1900, on the premise that h-bar and 1/c^2 were both zero. With the advent of quantum mechanics and special relativity, it was realized that they both have non-zero values, although they are extremely small in terms of ordinary units.

http://www.mathpages.com/home/kmath488/kmath488.htm

Please note that the reference is to h-bar (reduced Planck's Constant h/4π) not to Planck Length or other units that have become very popular recently... that is an aside.

Now looking at the equation for de Broglie's Matter Wavelength we can see that it relates strongly to Special Relativity and the Lorentz Transformation but considered at low velocity (low energy).
User posted image
In fact it describes the wavelength of particles as v -> 0 and as v -> C. More obviously the dynamics of particles with mass as v -> 0 is the low velocity limit of Special Relativity and as you can see λ -> ∞ as v -> 0. This phenomenon can be seen in BEC's which is a unique window on the interaction of matter and Bose Einstein Statistics in confined spaces.

Regarding the situation where m -> 0 and is subject to any force the acceleration will initially approach infinity (eg. photons). Simply an extension of the equations which relate the mass to the acceleration. Naturally as soon as this action occurs to any particle with finite (non-vanishing mass) the wavelength of any particle that was initially at rest will shrink to approach zero (but never quite reaches it). In the limit of course these events will happen. Big accelerators can hide this low velocity structure of matter and though we "know" that it there we think it can be ignored.. This behavior of inertia-less particles is one reason responsible for photons never moving at less than the speed of light. In the case of light the velocity will reach C but the wavelength will not reach 0 because E = hf.... Where for light f =C/λ. The conjugacy property described above "prevents" λ -> 0 by a factor h.

Now if there is an actual fixed reciprocal relationship between these variables but why is this not seen? Instead we "see" only the simple clicks of the detector providing the detection of events along a plane as shown in this treatment...


Single slit diffraction - Uncertainty Principle
... Click to enlarge...

In the Heisenberg uncertainty relation, the momentum of a particle cannot be known with any greater accuracy than h/∆x where h is Planck's constant and ∆x is the uncertainty in spatial position. The more you localize its spatial position, the less certain you become about its momentum. An optical illustration for this is the diffraction of light though a slit.

How it works:
For a laser beam, the transverse momentum is pretty well known (i.e. it's zero) but you have no localization of its spatial x coordinate. You can localize it spatially, by passing the beam through a slit, but by doing this you become uncertain about your x momentum. The more you localize spatially by closing down the slit, the more uncertain becomes the momentum. This manifests itself in a broadening of the diffraction pattern in the x direction which means that you've given the photons some momentum ∆px that wasn't there before (see figure 1).

figure 1. Schematic illustration of single slit diffraction

User posted image
... Click to enlarge...

http://www.fas.harvard.edu/%7Escdiroff/lds...AnalogofUP.html

Here we see that the scattering of "particles" including photons and electrons obey this simple relationship and result in the Single and Double Slit/Pinhole Diffraction Effect where an event is registered along a flat plane such as a screen when using light or a Cadmium Sulphide Screen (alternatively a photon detector array may be used). The detector will register a click or no click (nothing in between... no half clicks). According to standard theory this scattering is in accord with this equation ...
∆E ∆t ≥ h/4π
This is an inequality signifying the digital nature of this phenomenon. This coupling indicates that there are no equalities here between Euler functions but there is a loss of data indicated by the product in the errors being greater than h_bar... the reduced Planck's Constant. What I would like to say is there is far more data in the spatial region of that single speck recorded on the screen than what is currently seen by such primitive detectors. Replace the simple plane detector with a thick sensitive translucent photographic emulsion and repeat the experiment and then you will see that this planar information does not contain just a simple record of the brightness on that plane but now contains information of all illuminated visible space in the dark room illuminated by the source laser... it is now a Hologram and you can prove this information is there by simply illuminating this film with a laser of the same wavelength. The entire room and not just the one dimensional data along the pattern is recovered. Replace the screen with a plate and the information is recorded as a series of in depth fringes in the hologram and not just "random noise". The information is actually really there. It is not a simple function as shown by Heisenberg's Equation above it is an harmonic function encoded in depth in the space and what the photodetector or the screen has done is simply "project" this information onto a surface losing the phasor information in the process. This "amplitude" is the same "amplitude" computed by Feynman's Many Path QED (Quantum Electrodynamics) Analysis. Now where did this additional information come from? Well it comes directly from the theory of Fourier Transforms and this plane that is being investigated is a transform plane which can only be described by complex numbers.

You can find this information about the way a pinhole camera or camera obscura will process information from coherent light reading this article here...
Optical Methods in Experimental Mechanics. Part 15: Fourier Optical Processing.
User posted image
... Click to enlarge...
So we can readily see that while these variables are conjugate they are actually "exact relationships" and they can be examined in detail provided the the photons are all absorbed in such a way to decode the complex information from the waveform as "depth" in the plane. I would also add that the Fourier Transform in this sense is a repeatable process that is it's own reciprocal and is not an approximation as some linear methods can be.

This works because of Canonical Typicality and the property of locality (not inherently part of standard Quantum Theory) where the variables have a relationship to teach each other and are not distributed "statistically" at all when the information is gathered in the way described. Obviously the detector is criitical in this process... Simple photodetectors just cannot record this data.
QUOTE
Canonical Typicality
Sheldon Goldstein, Joel L. Lebowitz,
Roderich Tumulka, and Nino Zanghi
December 27, 2005
Abstract
It is well known that a system, S, weakly coupled to a heat bath, B, is described
by the canonical ensemble when the composite, S + B, is described by
the microcanonical ensemble corresponding to a suitable energy shell. This is
true both for classical distributions on the phase space and for quantum density
matrices. Here we show that a much stronger statement holds for quantum systems.
Even if the state of the composite corresponds to a single wave function
rather than a mixture, the reduced density matrix of the system is canonical, for
the overwhelming majority of wave functions in the subspace corresponding to
the energy interval encompassed by the microcanonical ensemble. This clarifies,
expands and justifies remarks made by Schrodinger in 1952.
http://www.math.rutgers.edu/~oldstein/papers/can.pdf

The next surprise about This Heisenberg Relationship is it can be circumvented by certain methodologies. This paper tells the story...
Protective Measurements by Yakir Aharonov and Lev Vaidmana
or this commentry...
Comment on"Protective measurements and Bohm's trajectories" byY.Aharonv, B.G.Englr, M.O.Suly, A.Drezt
These have a practical aspect aside from locality and Canonical Typicality....
"Protective" measurements in quantum mechanics... with animations
There are arguments possible to counter these claims but there have been no proofs to show that these claims are false "so far". Nevertheless a test of these theories should be made.

These are experimentally derived phenomena and also indicate the true underlying nature of this "holographic information" and the potential fact that quantum particles can have a history without having the wave function collapse.
User posted image
... Click to enlarge...
Shows fine static standing wave fringing in a Holographic Image (no lens needed) and when illuminated by a laser of the same frequency restores the entire three dimensional relationships "globally". These fringes are as exact as it can be while each flash of light still indicates the collapse of the state these tiny pinpoints of light are actually signaling "much more data" than initially seen. I would also like to point out that the Quantum Zeno Effect also is another application of these processes leading to extracting more information than many are publicly saying about them.
http://en.wikipedia.org/wiki/Quantum_Zeno_effect
(ps: warning on this page but the information is correct)
This effect is definitely confirmed in experiment where a photon state is reset over and over and is one of the prime mechanisms in the practical science of Circuit QED. You need only look them up in the literature and you will actually find hundreds of references to all these topics and none of them say "a spade is a spade".

Sometimes we listen to the stories and we assume they are true just because they give the right answers. However they do not give the whole answer. What sometimes is not apparent is a theory can have a limited range of application and then you need to open up and allow that wider vista to to be revealed.

Cheers

PS: Watch for typos ... they will be there somewhere.
mr_homm
This isn't the next installment of my opinion piece, just a quick reply to the people who have posted in response to my first installment.

@Majkl

The quantum field theory approach treats the particles as just disturbances in a fundamental field. In the same way that an individual particle has various quantum states and can be excited to a higher state by adding energy, the field has states which represent numbers of particles, and by adding energy to the field, you can excite it to a higher level, which increases the number of particles. From this point of view, particles aren't things, they are actions of the field, so it suddenly makes sense to think of them as connected to the field even at points that are separated in space. This seems rather similar to the idea you expressed.

@bm1957

There's nothing wrong with your understanding of uncertainty, I'm only emphasizing a different perspective on things. You are looking at it from the point of view of practical limitations on what we can measure, which is of course important. I am trying to step back and take a "very big picture" view and ask why do these practical limitations always arise? Really, I'm thinking like a mathematician here, rather than a physicist. When a mathematician observes that something is true in many apparently different cases, he starts to smell a theorem somewhere, some unifying explanation that provides a deeper reason why all the individual cases must be true. To make a rather trivial analogy, suppose I try to look up the phone numbers of 10 old friends in a phone book, and each time, I fail to find the number. I suspect that each of my friends doesn't live in town anymore. Finally, I look at the cover for the phone book, and realize I've got the book for the wrong city. Suddenly all is clear, and each case no longer requires an individual explanation. The individual explanations are all still true (my friends really don't live in the town whose phone book I was looking at), but it's no longer a puzzle or even a coincidence, and the universal explanation is much more satisfying than all 10 of the individual explanations together. (In my experience, real insights always make you slap your forehead and go "Doh!" like Homer Simpson.)

@GoodElf

Thanks for you comments, and for adding much interesting material to the discussion. I won't respond in much detail to all of your points, because a lot of them are things I'm already discussing in my next installment, which is half written, and it seems inefficient to say most of the same things twice. So, I'm not snubbing your contribution at all, let me make that clear, it's just that most of the things I would normally have written in response to your points are already in the pipeline.

Thanks for bringing up Fourier transform pairs and uncertainty. This is one of the topics that I was going to find somewhat troublesome to introduce, and now it will be easy. Much of my opinion on the Copenhagen interpretation depends on thinking about these Fourier transforms and what they mean in terms of the space of states (more on that in my next post.) At the end of your quote on Fourier transforms and uncertainty, they bring up the similarity between the connection of time to space in special relativity and the connection between conjugate variables in quantum mechanics. This is another interesting point, and I already had included some discussion of this in my upcoming post. (I know that sounds like "I was just about to say that," but it's true.)

QUOTE
The conjugacy property described above "prevents" λ -> 0 by a factor h.

Well, that's not quite literally true. You can make λ go as close to 0 as you wish at the expense of losing track of the position, but it is basically true that bringing λ all the way to zero would require an experimental container of infinite size, so there is a practical limitation here. Also, the energy of the particle would diverge to infinity, so there's another practical limitation.

QUOTE (->
QUOTE
The conjugacy property described above "prevents" λ -> 0 by a factor h.

Well, that's not quite literally true. You can make λ go as close to 0 as you wish at the expense of losing track of the position, but it is basically true that bringing λ all the way to zero would require an experimental container of infinite size, so there is a practical limitation here. Also, the energy of the particle would diverge to infinity, so there's another practical limitation.

The detector will register a click or no click (nothing in between... no half clicks). According to standard theory this scattering is in accord with this equation ...
∆E ∆t ≥ h/4π

Most people focus all their attention on the two slits in this experiment, whereas I tend to think that the behavior of the detector is much more interesting. There's a whole long essay I could write about just that, but let's leave that for a later time.

QUOTE
This is an inequality signifying the digital nature of this phenomenon. This coupling indicates that there are no equalities here between Euler functions but there is a loss of data indicated by the product in the errors being greater than h_bar... the reduced Planck's Constant.

I'm not sure how this shows a digital nature, although the all or nothing response of the detector certainly does so. As you can probably guess from the first installment of my little essay, my position on this is going to be that there is no loss of information here, because there was never any information to lose. Of course, that's open to debate. Certainly the detector loses information, because it fails to record phase, as you mention a bit later. However, even with the phase information recorded, you would still find that ∆E ∆t ≥ h/4π, so this inequality is true even without any information loss.

In order to record the phase information, it is important to remember that absolute phase cannot be measured, only relative phase. Therefore, you need a phase reference, so you shine a reference laser onto the photographic plate along with the light from the two slits, so that the phase difference between the two beams can be detected. Of course, this is precisely the recipe for making a hologram, just as you said. Note that the information specifying the hologram is all available at the plane of the photographic plate, so it is not necessary to think of this information as being spread out through the volume of space occupied by the light.

I've started reading the Canonical Typicality paper, but so far I don't see the relevance. Perhaps it will become clear upon further reflection. At this point I am out of time for now, so I will have to follow up on your other links and comments in a later post. Next up: installment 2.

--Stuart Anderson
Good Elf
Hi Stuart,

Thanks for the points. Just answering some of those issues as you have placed them there.

QUOTE (mr_homm+)
QUOTE (Good Elf+)
The conjugacy property described above "prevents" λ -> 0 by a factor h.
Well, that's not quite literally true. You can make λ go as close to 0 as you wish at the expense of losing track of the position, but it is basically true that bringing λ all the way to zero would require an experimental container of infinite size, so there is a practical limitation here. Also, the energy of the particle would diverge to infinity, so there's another practical limitation.
Just mentioning the fact that E = hf where f -> 0 or even if f -> ∞ there is a fixed ration E/f between the energy and the frequency that equals h. Classical physics does not have this relationship and assumes energy can be varied independently of f.... This is like your poor man rich man analogy.
QUOTE (mr_homm+)
QUOTE (Good Elf+)
This is an inequality signifying the digital nature of this phenomenon. This coupling indicates that there are no equalities here between Euler functions but there is a loss of data indicated by the product in the errors being greater than h_bar... the reduced Planck's Constant.

I'm not sure how this shows a digital nature, although the all or nothing response of the detector certainly does so. As you can probably guess from the first installment of my little essay, my position on this is going to be that there is no loss of information here, because there was never any information to lose. Of course, that's open to debate. Certainly the detector loses information, because it fails to record phase, as you mention a bit later. However, even with the phase information recorded, you would still find that ∆E ∆t ≥ h/4π, so this inequality is true even without any information loss.
What I mean there is if there was a ∆E that I could stipulate then there is an actual value for ∆t such that it equals h/4π as shown in that reference. This is because the Fourier Transform transform pair is an exact relationship not a statistical one related through Euler's relationships... a non-linear harmonic transform for each frequency. This means that the purely random nature of the association is not retained (if you like ... an enforced "locality" of the function around that particular ∆E). Interestingly this is not part of standard quantum theory where the second value need not have any value at all related to the first value... There is a "deep significance" here. This leads to these fine interference lines or cavities in the hologram. The photons pick their place in that actual physical space to be absorbed at an "antinode" in some function... a phasor. Whereas at the "nodes" the photons cannot be absorbed. This is not possible to determine in the case of a detector like a planar device that can only absorb "on the plane".
QUOTE (mr_homm+)
Note that the information specifying the hologram is all available at the plane of the photographic plate, so it is not necessary to think of this information as being spread out through the volume of space occupied by the light.
What this Holographic Information "means" is the Hologram can be made anywhere in the space and the plate will record all hte information about the interference pattern where ever it is relative to the photographic plate. Unlike a "simple detector" the Hologram records all the spatial information "including" the interference pattern from any relative commonly visible position. knowing that the actual photons travel directly from source to 'screen" with no deviations ... the path of least time this information about the distant parts of the room which may include the interference pattern must be recorded in "spatial interferences"... those little patterns in the plate that extends to every part of the "darkened room".

Waiting for the next installment...

Cheers
vkamath
Thanks m_homm for that excellent description and interesting analogies of the Uncertainty Principle. Without all the math, this is understandable to a layman to physics like myself.
I always thought until this point that the Uncertainty Principle was a "cop-out" in finding the position and momentum of a particle. But your description make it clear.
Looking forward to your second installment.

mr_homm
Here is the second installment. Sorry for being slow, but I've had less time to work on this than I expected.

There is more to say about the uncertainty principle, but first I must talk a bit about the Copenhagen interpretation. Unfortunately, this requires certain mathematical concepts to be crystal clear, so it will be necessary to set up some of these ideas before the main discussion can go forward.

I mentioned earlier that position and momentum are just the two classical aspects of a single piece of physical information, and that this piece of information had many other aspects as well, just as the planet Venus does other things when it is not being the morning or evening star. This is the central idea behind my position on the Copenhagen interpretation, and is also the other radical reinterpretation of physics to which I alluded earlier; it is the road Bohr and Heisenberg did not take.

Fundamentally, it comes down to taking "state space" literally, and thinking like a mathematician instead of like a physicist. To see what I mean by that, let's start with state space. Part of the basic mathematical formalism of quantum mechanics is that the state of a physical system can be described by a vector in an abstract space called a Hilbert space. This is basically just a vector space like ordinary three dimensional space, but may have infinitely many dimensions.

(The fact that it may be infinite dimensional shouldn't be a conceptual roadblock, because the "Hilbert basis theorem" shows that it acts pretty much like a finite dimensional space. You can set up a coordinate system on it and express vectors as series of numbers, just as you can express ordinary 3 dimensional vectors in terms of x, y, and z coordinates. There are just a lot more of them. Just about everything you would want to understand about Hilbert space, you can visualize by thinking about how it would look in 3 dimensions. Also, this is an abstract space, a mathematical construct, so it does not mean that the physical space of the universe is really infinite dimensional.)

To state my first mathematical point most concretely, let's look at a 2 dimensional map, for instance a map of Italy. I can draw a coordinate system on this map, with the origin at Rome, and the x axis pointing due east, and the y axis pointing due north. Then I can give the coordinates of another city, say Naples, as so many km E and so many km S. By giving you these numbers, have I given you the vector that points from Rome to Naples? NO. I have given you a description of the vector in this coordinate system. If I were to choose a different set of axes, still through Rome, but now with the x axis pointing due northeast and the y axis pointing due northwest, I could also give you coordinates for Naples, this time, so many km NE and so many km NW. This would also be a description of the same vector, but in a new coordinate system.

The idea here is that the vector is something real, and the coordinate system is something artificial which we add to the map in order to give coordinates to the vector. Both physicists and mathematicians are aware of this, of course, but physicists (at least in my experience) tend to have a bias in favor of working with coordinates and mathematicians have a bias in favor of working without them.

Why this should be so is another interesting philosophical sidelight to the discussion. "Noumenon" is the word philosophers use to describe the actual reality that lies behind our perceptions, and "phenomenon" describes the observable expression of the underlying noumenon. (For the genetically inclined, you may think of this as similar to the relation of genotype to phenotype.) Physicists have no access to the noumenon, because their theories all must eventually involve measurement of some kind, and these are part of the phenomenon, the appearance of reality. By building ever subtler theories, they hope to trap the noumenon in the web of all its phenomena. Mathematicians, on the other hand, create mathematical constructs by setting up postulates, and then deriving the consequences of those postulates. The postulates are by definition the ultimate reality (noumenon) of the mathematical structures, and the theorems are the phenomena. Mathematicians proceed from noumenon to phenomenon, and physicists (attempt to) proceed the other way.

This means that, to a mathematician, the underlying truth of a vector space comes from its postulates, and the vectors themselves are therefore real things (within the mathematical theory) that exist before a coordinate system is applied to the vector space. In contrast, to a physicist, the coordinate dependent measurements are prior, and from them the coordinate-free reality must be inferred. You can see this in how the theory of tensors is constructed in physical applications: the emphasis is all on how the changes of coordinates must work so that the physical meaning of the quantity will be the same in the new coordinate system as in the old one. Then anything whose appearance changes in the proper way when you change coordinates must be something with an invariant physical meaning; the stable reality is inferred from the way that the various appearances change. Mathematicians, on the other hand, define tensors by certain postulates about how they behave, and then later, when a coordinate system is applied to them, they can say that their abstract tensor looks one way in one coordinate system and another way in a different coordinate system, based on the postulates. They construct the coordinate change properties from the underlying reality instead of constructing the underlying reality from the coordinate change properties.

(By the way, this is all from personal experience. I majored in both Mathematics and Physics separately as an undergraduate. In fact, I simply told each department that I was majoring in their subject but never informed them that I was also majoring in the other one. Apparently I wasn't supposed to do this, because when I graduated, I got two separate diplomas and a rather petulant letter from a university bureaucrat telling me that I wasn't allowed to have done that, but it was now too late to stop me. wink.gif Anyway, this is the difference in emphasis between the mathematicians' approach and the physicists' approach, which I observed by doing the two majors side-by-side. I'm not saying that all mathematicians and all physicists think in these ways, just that there is a noticable degree of bias.)

Now, what does this have to do with the Copenhagen interpretation? My position is as follows: Both the Copenhagen interpretation and the uncertainty principle arise from the same interpretive error, and that error is our failure to recognize at a gut level that our state vector coordinate systems are not part of reality. The preference for coordinates over abstract vectors biases us towards making this mistake, and both our education in classical physics and our everyday experience reinforce that bias so strongly that it can be difficult to shake off the conviction that it is right. But it is a mistake nonetheless.

In detail then, what is this mistake? Let's first look at this mistake in the context of a very simple system, such as the map of Italy, then look at how a very similar, but subtler mistake was recognized and corrected by special relativity, and finally, proceed to the case of the Copenhagen interpretation, which fails to correct the mistake.

Suppose I show you my map of Italy upside down. Even with no text printed on it, you immediately know it is upside down, because it looks weird that way. But there is no inherent right way to map Italy. The peninsula itself does not come with a "this end up" arrow printed on the ground. The sense of weirdness comes entirely from our familiarity with seeing things one way and our unfamiliarity with seeing them any other way. We are disoriented (literally: the word "disoriented" originally meant that you didn't know which way was east) and it is hard to resist the urge to turn it the "right" way up in order to "see it better." The point here is that culturally based expectations can generate a quite strong sense that one of two ways is "right" or "real" and the other way is "wrong" or "fake." How much stronger than that, then, is the conditioning that we absorb from our entire education and our entire experience of the everyday world? It can be very difficult to force your mind to accept a new perspective.

When I turn the map right way up, Venice is directly above Rome, and Naples is 45 degrees down and to the right from Rome. Let's put a coordinate system on this map with the "y" axis pointing north and the "x" axis east. You could say that the vector from Rome to Venice was "pure" y, but the vector to Naples was a "superposition" of -y and x. Now suppose I turn the map 45 degrees counterclockwise, so that northeast is at the top, and I draw a new coordinate system on the map with the "y" line straight up the map (i.e. due northeast) and the "x" directly horizontal (due southeast). On this coordinate system, Venice does not appear to be directly above Rome, but somewhat above and to the left of it. In this coordinate system, you could say that the vector to Venice was now a mixture of -x and y, while the vector to Naples was now pure x.

What is this map discussion telling us? Three things: conditioned bias can give you a compelling but false feeling that one way is right, coordinate systems can be changed arbitrarily without affecting reality, and most importantly, the concepts of "pure" directions (due North, for instance) and "superposed" directions are an artifact of the coordinate system. The first point is obvious from experience, and the second point is just Alfred Korzybski's famous saying that "the map is not the territory." The third point is the one to keep in mind: the idea that some vectors are pure and others are superpositions is false. These concepts do not apply to the vectors themselves (the noumenon) but to their expressions in particular coordinate systems (the phenomenon). In fact, for any given vector, I can always just draw a coordinate system with one axis along that vector and the other axis perpendicular to it, to make the vector pure in that coordinate system. For every vector, there is a coordinate system in which it is pure (i.e. has only one nonzero component).

This discussion of the map may seem trivial, but that is intentional. I want to show what the error is in a simple case where it is extremely obvious that it is an error. For the map, it is completely clear that changing the coordinate system will not actually move the city of Naples! Who would think otherwise? The separation between the map and the reality, and between the vectors themselves and their coordinate system representations should also be completely clear in the map example. Finally, it should also be crystal clear that the the property of a vector being "pure" is not a feature of reality. Now we can turn to the next case, special relativity, in which all these same statements are widely acknowledged to be true, but are much less obvious than for the map.

In special relativity, there are various puzzling effects, such as mass increase, time dilation, length contraction, and shifts in simultaneity. These are all aspects of the general Lorentz transformation, which is basically a coordinate transformation. What was new in special relativity was that the coordinate system encompassed both space and time. Instead of viewing the world as having three spatial dimensions and a separate time dimension, the space and time dimensions were treated as parts of a single whole called "spacetime." This is a profound difference, in that it allows for the direction of time to change. Out of the entire 4 dimensional spacetime, one direction is singled out to be time, and three other directions are chosen to form the three space axes, x, y, and z. When an observer begins to move, the direction of time is altered for that observer, so that his time axis is now a different line in spacetime, and the three dimensional slice of spacetime that looks like space to him also changes.

There are many similarities to the map of Italy example here, and also some important differences. The direction of the time axis may change in spacetime, just as the direction of the y axis may change on the map. Also, just as on the map, but even more so, we have a strong feeling that one of these axis choices is "more right" than the other. For instance, suppose observer A stands on the shore, while observer B on a ship goes 100km north in one day. Imagine (if you can) drawing a line through the 4 dimensional spacetime from observer A today to observer B tomorrow. From A's point of view, there is a change of both position and time, so this vector would appear as a mixture of space and time displacements. From B's point of view, with his space coordinate system attached to the ship, he has stayed at the origin of his coordinate system the whole time, but aged one day, and so to him the same spacetime vector from A today to B tomorrow would appear to be purely a change of time. This vector is B's time axis. Clearly, A and B disagree on whether the same physical vector is or is not pure time. Since the vector cannot really be different from itself, the disagreement can only be the result of using different coordinate systems. This means that the concept of being pure time cannot be attached to the vector itself, but only to its expression in a particular coordinate system. The direction of time is therefore not a feature of reality.

However, it is hard to shake off the feeling that observer A is "really" right about the direction of time, just as it is hard to get over wanting to turn the map so that north is straight up. In fact, it is much harder with relativity than with the map because we experience time so very differently from space that it is quite a stretch of the imagination to see how they could be aspects of one and the same thing. This is a point where special relativity differs from the map of Italy: there is no inherent difference between the x and y axis directions. You could walk in the x direction or in the y direction just by choosing to do so. You cannot walk in the time direction, so time really is essentially different from space. Also, for the map you can choose the directions of x and y at will, but in relativity you cannot choose the directions of time and space. They appear to be chosen for you in some way. The choice varies as your velocity varies, but you have no direct control over it. By changing your velocity, you can cause a certain change of coordinates specified by the Lorentz transformation, but that is as much control as you have. The combination of lack of ability to choose the coordinates for yourself, coupled with the very different perceptions we have of time and space, make it much more difficult to accept that they are parts of the same whole.

In special relativity we can see that there is a real difference between time and space, in the sense that one of the 4 coordinates behaves quite differently from the other three. However, which exact direction in spacetime is the time axis depends on who is looking and how they are moving. This reminds me of the old latin saying, mors certa sed hora in certa (death is certain, only the hour is uncertain). The vector from A today to B tomorrow is prefectly certain, and the distinction between time and space is also perfectly certain, but exactly how much of that vector is space and how much is time is uncertain, because it varies with the observer's motion. It should be clear now how this is like the coordinate system on the map of Italy: there is a strong bias towards looking at things in the usual way and regarding that as the "right" way; the concept of a vector being "pure" is misapplied, because it applies to the coordinate system choice, not to the vector itself; and finally, all of the confusion in both cases stems from mistaking the coordinate system for a part of reality, which it is not. Arguments about whether the vector from A today to B tomorrow is "really" pure time or not are just as silly as arguments about whether the direction from Rome to Naples is "really" pure x or not, and for the exact same reason.

Classical physics assumed that time and space were completely independent of each other, which is the same as saying that the choice of time axis is fixed and can never vary. This is a clear case of confusing the coordinate system with reality. Special relativity cures this problem by correctly separating the coordinate system from the underlying spacetime, which therefore becomes a single 4 dimensional whole. This is not really any harder to understand than that tilting the map of Italy does not tilt the real Italy, but it is harder to accept because all of our experience is at such slow velocities that we are living within the same coordinate system all our lives. Since it is a permanent feature of our experience, it is very easy to mistake it for a permanent feature of the universe. The truth is that space is merely my three dimensional slice of spacetime that looks like space to me, and time is merely my line through spacetime that looks like time to me. One of the best things ever to happen to special relativity was the coining of the word "spacetime," because it forces space and time together into one thing on a verbal level, which helps anchor the somewhat slippery ideas of relativity to a nice graspable noun. Never underestimate the power of language: if you give something a name, people will immediately start to treat it as real. The word "spacetime" itself makes it easier to think about special relativity. If quantum mechanics had done the same thing with position and momentum, we would not now have either the uncertainty principle or the Copenhagen interpretation.

I'm afraid I must stop here for now, so that I can post this. Sorry it is so long, and sorry also that I still haven't got to the Copenhagen interpretation itself, but I felt is was important to make the argument clearly and in detail. You can probably already see where the trend is leading. I promise to finish the next installment ASAP.

More later.

--Stuart Anderson
meBigGuy
@ALL
I'm going to state some opinions with little scientific basis.

I have a problem with Copenhagen. I have a problem with long term superposition. I think Schrodinger's cat died, or didn't, long before anyone looked.

I have this notion that quantum effects are limited within regions of space-time. Kind of a quantum fuzziness. Think of fuzziness moving through time, but continually resolving itself. It's always fuzzy at the moment, but leaves a trail of "whatever happened". Everything at the quantum level is a mess of interacting probabilities ever changing in spacetime. The end effect is the illusion of stability, continuity, and consistency. Most of the time (on average?) the most probable things happen, so here we are in a stable reality.

Roger Penrose says some interesting things:
"Penrose hypothesised that the transition between macroscopic and quantum begins on the scale of dust particles, which could exist in more than one location for as long as one second "

@mr_homm
QUOTE
The direction of time is therefore not a feature of reality.

By this did you mean that the forward direction of time is not a feature of reality? There is forward and backward, and they are different. We experience time in a forward "cause and effect" sense probably due to our physical dependence on the Second law of thermodynamics.

Even if you buy into Cramer and Transactional interpretations, forward and backwards are different.

Looking forward to more from you. smile.gif
mr_homm
@meBigGuy:

I meant only that the direction of the time axis through spacetime can be skewed. So in that sense, the direction of time is changed, similarly to taking the y axis in my map example and turning it a few degrees away from notrh. What I said is literally true, because there are many different directions through spacetime that can be the time axis for different observers, but along each axis time does flow forward, never backward.

I think the miscommunication arose because I forgot and used the technical meaning of "direction" in a general interest discussion. The technical usage has the word "sense" for describing "forward or backward along a line" and "direction" for the orientation of the whole line in space. But everyday language uses the word "direction" for both of these ideas, and so the meaning was not clear. More formally, I should say that the Lorentz transformation varies the direction of the time axis, but cannot reverse the sense of time flow along that axis.

(Actually, if the relative speed is > c, then the sense of time flow for one observer would reverse relative to another observer. This is usually taken as one of the proofs that faster than light travel is impossible, since it would violate causality.)

About Cramer: I know this guy, very tangentially. He's a physics professor at the same university I work at, and many years ago when I was a student, I was the grader for his daughter Katherine's physics homework. She didn't go into physics herself, but into publishing, At the last time I heard, which was when I ran into her at a science fiction convention a few years back, she is one of the more important people in the science fiction publishing business. Her father is a science fiction writer as well as a physicist, so I suppose it runs in the family. I never had a class from him directly, but I've talked to him. He's a very interesting guy, full of interesting ideas, and he has the most distinctive laugh I've ever heard, which starts off like a loud donkey-bray, and then always ends in three rapid snorts. His transactional interpretation ideas are very interesting, but I haven't looked at them in a while, so they've gone a bit fuzzy in my memory. I don't recall them allowing for time reversal though, but I could be wrong.

As to Penrose, his idea (well, he has a LOT of ideas, but this particular one) is that any kind of interaction with a particle will collapse the wave function, and there are particles all over the place, so all the wave functions are collapsing all the time, which keeps the universe looking classical. So for him, the fate of Schrodinger's cat is already decided, since the molecules of the box itself function as an observer by interacting with the cat, collapsing the wave function immediately.

My take on it (see next installment, whenever I manage to finish it) will be a bit different, because in my opinion there was never any quantum fuzziness in the first place, nor any wave function collapse. These ideas are both artifacts of our clinging to a classical "coordinate system" in our description of the particles.

Thanks for an interesting discussion so far!

--Stuart Anderson
rmuldavin
Trying to follow the interesting discussion above, and note that Physorg.com recently posted an article "The Worlds lowest noise laser: Researchers outsmart quantum physics".

In trying to go beyond the article, I found this link:

http://www.aei.mpg.de/english/research/tea...Proj/index.html

The Index lists a number of projects worldwide that are attempting to measure gravity waves.

The Max Planck Institute for Gravitational Physics, is one of the participating members of the GEO600 ground based detector, with arms some 600 meters long. The article in Physorg shows a picture of a model that uses red laser and green laser said to get an improvement of three times.

It appears to my thinking that the authors make the claim that by distributing within the crystal that is excited by a red lase, green laser energy, the normally random "noise" is reduced since it is, maybe separated and and more concentrated.

Have not found any supporting essays. But since some String Theories I've read assign the EM forces as a transverse to the strings and Gravity forces longitudinal, I wonder if there is information as to how they would aim their device which is 600 meters long.

Is this another Michelson Morely Experiment that did not detect a difference for the speed of light?

Maybe an effort to get accurate 100 Hertz per second gravity waves at very low amplitudes?

Best, rm
rmuldavin
http://front.math.ucdavis.edu/author/R.Schnabel

Try this link to the author of the above GEO600, I just downloaded his and two other author's papers, it is 16 pages long, has many detail drawing.

Best, rm
Good Elf
Hi mr_homm,

QUOTE (mr_homm+)
About Cramer: I know this guy, very tangentially. He's a physics professor at the same university I work at, and many years ago when I was a student, I was the grader for his daughter Katherine's physics homework. She didn't go into physics herself, but into publishing, At the last time I heard, which was when I ran into her at a science fiction convention a few years back, she is one of the more important people in the science fiction publishing business. Her father is a science fiction writer as well as a physicist, so I suppose it runs in the family. I never had a class from him directly, but I've talked to him. He's a very interesting guy, full of interesting ideas, and he has the most distinctive laugh I've ever heard, which starts off like a loud donkey-bray, and then always ends in three rapid snorts. His transactional interpretation ideas are very interesting, but I haven't looked at them in a while, so they've gone a bit fuzzy in my memory. I don't recall them allowing for time reversal though, but I could be wrong.
Bit uncharitable to mention these matters ... people are usually "quite complex". What would you say about Stephen Hawking for instance? I find that many on this Forum are playing the man and not the ball. IMHO this is an error. I think you have Cramer at a distinct disadvantage don't you?

Fair comment about Roger Penrose but that is the ball game and we can all be right or wrong depending on what turns up in experiments. I am a journeyman in Physics so I just "read the signposts" and not go about pulling them down when they disagree with one's own "map". The problems of intense specialization and compartmentalization of information can result in a cloistered environment of mutually agreeing social gatherings. There are very few pronouncements nowadays about the direction of Physics regardless of the rapid developments that are occurring... none of that future is being foretold by the "futurologists". I also think that this changing vista is the direct result of experimental sciences and not so much theoretical sciences which have moved "out of the ballpark" into the unprovable and problematic. To me this indicates "something is rotten in the State of Denmark" (... Umm... the Copenhagen Interpretation rolleyes.gif ). We need to wait and see what is turning up since the Theoreticians are not providing a unified view of all these different physical situations and we all know they all can't be right at the same time.... If they are then we are doing the wrong set of experiments to find a resolution.

You have said nothing substantial about Cramer's Transactional Hypothesis which is the subject of the questions... what can you say about that and of course Wheeler-Feynman Absorber Theory on which it is based? This theory is a forerunner of Feynman's Many Paths QED Theory in which he shared a Nobel Prize. I don't think anyone has said that he was wrong ... It would take a "big man" to say that. Feynman was quite strongly committed to the interpretation of antiparticles as ordinary particles traveling back in time. I am sure that general time travel is not possible but without specific arguments I can't see why there are not reactions which send particles back in time since "arguably" this is experimentally seen and I believe experiment is the ultimate deciding step in Physics. All "theories" must toe the line right there... in the results of the experiments. Physicists who disagree with the Universe itself usually come off a poor second.

I would point out that time is quite "elastic" under certain conditions ... Consider the Delayed Choice Quantum Eraser Experiment (the fundamental concept was proposed by John Archibald Wheeler) the resolution of this is the recent experiment actually works and from our perspective this is the "future" influencing the "past". Even one experiment, properly carried out, is "enough" to put down all the nonsense. We may not control that past but it is indicating an anomaly of non-local behavior of which there are many examples. This is not just a "one off" experiment and is the result of a sequence of maturing ideas which are all "self supporting" as all properly designed experiments are. The methodology has stood up and it has been repeated. I for one despise the scorn placed on Experimental Physicists and support their purpose "ahead of the smarter Mathematical Physicists". There are a lot of politics there and I would not buy into that simply to stroke our egos. Quantum Theory is time symmetric even though nature is not. It is my understanding that it is a credible concept... at least to me.
http://arxiv.org/abs/quant-ph/9903047
http://en.wikipedia.org/wiki/Delayed_choice_quantum_eraser


Otherwise a very interesting discussion... please continue.

Cheers
meBigGuy

I found this on Wikipedia. I'd sure like to read his exact words.
QUOTE
As Heisenberg pointed out, being "observed" does not actually have to involve a human consciousness. What is actually required is that the "intrinsically undefined" photon, encounters a situation that results in its presence being manifested in the Universe in such a way that it is no longer "undefined."




@mr_homm
I'm really looking forward to your treatment of this. I see what you were referring to by direction of time. As to forward and backwards time, I lean towards Wheeler-Feynman. I can see no other way to resolve a five year photon trip to my eye with the fact that the transfer was instantaneous in the photon frame.

I still have issues at the wave-particle level.

When you you think about the two slit experiment from the perspective of a photon, which experiences no proper space or time, the entire path is just an instantaneous transfer of energy. So, anywhere you affect the results, you affect the whole path. This manefests itself in strange ways in our frame.

But, I have problems with respect to particles with mass. Electrons have proper time and space, and exhibit spin entanglement and the same 2 slit wavelike behaviors. What happens when you apply Wheelers Delayed choice thought experiment to electrons? Is there a delay due to electron proper time?

Maybe your theory will resolve all this for me smile.gif.


mr_homm
Hi Good Elf,

You said:
QUOTE (Good Elf+Jan 26 2008, 02:51 PM)
Hi mr_homm,
Bit uncharitable to mention these matters ... people are usually "quite complex".


Ouch! I was very surprised by this. It seems that I've given very much the wrong impression with my comments on Professor Cramer. I had no intention of dismissing either the man or his work; in fact I have great respect for him, which I thought showed in my comments! Apparently that did not come through. I have fond memories of the few times I spoke with him, and his distinctive laugh is tied up in those fond memories for me, so I mentioned it merely to make the reminiscence more concrete and personal. Also, the fact that he writes science fiction is decidedly a point in his favor as far as I am concerned; I certainly did NOT mean to imply that since he also writes science fiction, we do not need to take his theories seriously. On the contrary, the fact that he writes science fiction makes him more interesting, because he is willing to be an outside-the-box thinker. Really, the only reason I mentioned any of this is that it very seldom happens that someone mentioned in the context of physics is someone I actually have met. Since I thought it was interesting, I brought up some recollections I had of the man, which were intended as an anecdote and nothing more. In any event, my estimate of the man, whether good or bad, does not bear at all on my estimate of his theoretical work, which must speak for itself through experimental test.

QUOTE
What would you say about Stephen Hawking for instance?

Since I have not met him in person, I do not have any personal anecdotes to relate about him, so I would say nothing. On the other hand, if I had met him, there would undoubtedly be some detail about him that would stick in my mind afterwards, and no it would probably not be the obvious one. I usually remember little quirks people have, both because they are interesting and because they help me fix that person in my memory more solidly. They are a kind of mnemonic device for me.

QUOTE (->
QUOTE
What would you say about Stephen Hawking for instance?

Since I have not met him in person, I do not have any personal anecdotes to relate about him, so I would say nothing. On the other hand, if I had met him, there would undoubtedly be some detail about him that would stick in my mind afterwards, and no it would probably not be the obvious one. I usually remember little quirks people have, both because they are interesting and because they help me fix that person in my memory more solidly. They are a kind of mnemonic device for me.

I find that many on this Forum are playing the man and not the ball. IMHO this is an error. I think you have Cramer at a distinct disadvantage don't you?

I am not one of them, and I completely agree that it is an error. The ad hominem argument is basically an admission of defeat. However, in this case, I was playing neither the man nor the ball, but merely telling a story. Perhaps it could be said that I had Cramer at a disadvantage if I were in any conflict with him, but I am not. I will say no more in defending my comments.

QUOTE

Fair comment about Roger Penrose but that is the ball game and we can all be right or wrong depending on what turns up in experiments. I am a journeyman in Physics so I just "read the signposts" and not go about pulling them down when they disagree with one's own "map". The problems of intense specialization and compartmentalization of information can result in a cloistered environment of mutually agreeing social gatherings. There are very few pronouncements nowadays about the direction of Physics regardless of the rapid developments that are occurring... none of that future  is being foretold by the "futurologists". I also think that this changing vista is the direct result of experimental sciences and not so much theoretical sciences which have moved "out of the ballpark" into the unprovable and problematic.  To me this indicates "something is rotten in the State of Denmark" (... Umm... the Copenhagen Interpretation  rolleyes.gif  ). We need to wait and see what is turning up since the Theoreticians are not providing a unified view of all these different physical situations and we all know they all can't be right at the same time.... If they are then we are doing the wrong set of experiments to find a resolution.

I agree that there is a lot of specialization and very little overview, which poses a problem for anyone wanting to take a philosophical look at physics. I also agree that experiment must overrule theory.

QUOTE (->
QUOTE

Fair comment about Roger Penrose but that is the ball game and we can all be right or wrong depending on what turns up in experiments. I am a journeyman in Physics so I just "read the signposts" and not go about pulling them down when they disagree with one's own "map". The problems of intense specialization and compartmentalization of information can result in a cloistered environment of mutually agreeing social gatherings. There are very few pronouncements nowadays about the direction of Physics regardless of the rapid developments that are occurring... none of that future  is being foretold by the "futurologists". I also think that this changing vista is the direct result of experimental sciences and not so much theoretical sciences which have moved "out of the ballpark" into the unprovable and problematic.  To me this indicates "something is rotten in the State of Denmark" (... Umm... the Copenhagen Interpretation  rolleyes.gif  ). We need to wait and see what is turning up since the Theoreticians are not providing a unified view of all these different physical situations and we all know they all can't be right at the same time.... If they are then we are doing the wrong set of experiments to find a resolution.

I agree that there is a lot of specialization and very little overview, which poses a problem for anyone wanting to take a philosophical look at physics. I also agree that experiment must overrule theory.

You have said nothing substantial about Cramer's Transactional Hypothesis which is the subject of the questions... what can you say about that and of course Wheeler-Feynman Absorber Theory on which it is based?

This is because I know nothing substantial about it, so any opinion I had about it would be uninformed and therefore useless to meBigGuy. Also, I should point out that there were no questions about Cramer's Transactional Hypothesis in meBigGuy's post. He merely stated that it did not imply time reversal. Since I also was not asserting that time would reverse, there was no conflict, and so I posted the only relevant comment I could make, which was that as far as I knew, he was right. Thank you, however, for reminding me that it is an approach to physics which I have been meaning to find out more about. As of now, though, I have nothing useful to contribute on that topic, since I know next to nothing about it.

QUOTE
This theory is a forerunner of Feynman's Many Paths QED Theory in which he shared a Nobel Prize.  I don't think anyone has said that he was wrong ... It would take a "big man" to say that.

Of course he was wrong. All current physical theories are wrong, since they all involve either GR or QM in some way, and these are in conflict. Therefore, none of the current theories can actually be correct.

QUOTE (->
QUOTE
This theory is a forerunner of Feynman's Many Paths QED Theory in which he shared a Nobel Prize.  I don't think anyone has said that he was wrong ... It would take a "big man" to say that.

Of course he was wrong. All current physical theories are wrong, since they all involve either GR or QM in some way, and these are in conflict. Therefore, none of the current theories can actually be correct.

Feynman was quite strongly committed to the interpretation of antiparticles as ordinary particles traveling back in time. I am sure that general time travel is not possible but without specific arguments I can't see why there are not reactions which send particles back in time since "arguably" this is experimentally seen and I believe experiment is the ultimate deciding step in Physics. All "theories" must toe the line right there... in the results of the experiments. Physicists who disagree with the Universe itself usually come off a poor second.

Since Feynman's interpretation of antiparticles is an interpretation rather than a new theory, it does not make any predicitions different from the standard ones. It is therefore not subject to experimental test, and so it is strictly optional. We can look at things this way if we choose to do so, if it is helpful in clarifying our understanding, or we can choose not to look at things this way if we prefer that instead. Similarly, the way of thinking about quantum mechanics that I have been presenting makes no physical predicitons different from standard theory; it is merely a way of looking at things which may or may not help make the theory "feel clearer." Of course I agree that where theories make physical predictions, experiment must be the final and only arbiter.

QUOTE

I would point out that time is quite "elastic" under certain conditions ... Consider the Delayed Choice Quantum Eraser Experiment (the fundamental concept was proposed by John Archibald Wheeler) the resolution of this is the recent experiment actually works and from our perspective this is the "future" influencing the "past". Even one experiment, properly carried out, is "enough" to put down all the nonsense.  We may not control that past but it is indicating an anomaly of non-local behavior of which there are many examples. This is not just a "one off" experiment and is the result of a sequence of maturing ideas which are all "self supporting" as all properly designed experiments are.  The methodology has stood up and it has been repeated. I for one despise the scorn placed on Experimental Physicists and support their purpose "ahead of the smarter Mathematical Physicists". There are a lot of politics there and I would not buy into that simply to stroke our egos. Quantum Theory is time symmetric even though nature is not. It is my understanding that it is a credible concept... at least to me.
http://arxiv.org/abs/quant-ph/9903047
http://en.wikipedia.org/wiki/Delayed_choice_quantum_eraser

Yes, the delayed choice quantum eraser is a fascinating experiment, and one that strongly constrains how we think about locality, causality, and many other aspects of quantum theory. As to the status of experimentalists, it has been my experience that every theoretical physicist I have met has been in awe of the experimental physicists for the massively complex and yet extremely precise equipment and procedures they develop. I have never yet met an experimentalist who was as impressed with the theoreticians as the theoreticians were with the experimentalists. The experimentalists, after all, have to understand the theory themselves well enough to design machinery to test it, and that level of understanding is often better than the understanding of some theoretical physicists. In addition to this, they must be masters of experimental design and experts with all sorts of hardware. I personally have a vast respect for anyone who has ever successfully designed and carried out a high precision physics experiment. It seems to me that experimentalists get short shrift in the popular physics books compared to theoreticians, because all the pragmatic and technical complexity of the experiments is essential to them, so it is impossible to convey to a nonspecialist what is going on. They simply cannot be "dumbed down" for the average reader the way theory can.

QUOTE (->
QUOTE

I would point out that time is quite "elastic" under certain conditions ... Consider the Delayed Choice Quantum Eraser Experiment (the fundamental concept was proposed by John Archibald Wheeler) the resolution of this is the recent experiment actually works and from our perspective this is the "future" influencing the "past". Even one experiment, properly carried out, is "enough" to put down all the nonsense.  We may not control that past but it is indicating an anomaly of non-local behavior of which there are many examples. This is not just a "one off" experiment and is the result of a sequence of maturing ideas which are all "self supporting" as all properly designed experiments are.  The methodology has stood up and it has been repeated. I for one despise the scorn placed on Experimental Physicists and support their purpose "ahead of the smarter Mathematical Physicists". There are a lot of politics there and I would not buy into that simply to stroke our egos. Quantum Theory is time symmetric even though nature is not. It is my understanding that it is a credible concept... at least to me.
http://arxiv.org/abs/quant-ph/9903047
http://en.wikipedia.org/wiki/Delayed_choice_quantum_eraser

Yes, the delayed choice quantum eraser is a fascinating experiment, and one that strongly constrains how we think about locality, causality, and many other aspects of quantum theory. As to the status of experimentalists, it has been my experience that every theoretical physicist I have met has been in awe of the experimental physicists for the massively complex and yet extremely precise equipment and procedures they develop. I have never yet met an experimentalist who was as impressed with the theoreticians as the theoreticians were with the experimentalists. The experimentalists, after all, have to understand the theory themselves well enough to design machinery to test it, and that level of understanding is often better than the understanding of some theoretical physicists. In addition to this, they must be masters of experimental design and experts with all sorts of hardware. I personally have a vast respect for anyone who has ever successfully designed and carried out a high precision physics experiment. It seems to me that experimentalists get short shrift in the popular physics books compared to theoreticians, because all the pragmatic and technical complexity of the experiments is essential to them, so it is impossible to convey to a nonspecialist what is going on. They simply cannot be "dumbed down" for the average reader the way theory can.

Otherwise a very interesting discussion... please continue.

Cheers


I still need to say one more thing about my unfortunate comments regarding Dr. Cramer. If you have looked at my posting history, you will know that I am extremely scrupulous about conducting myself politely and productively on these forums. Even though it was inadvertant, I seem to have given offense this time. For this I apologize to you, to everyone on the thread, and to Dr. Cramer. It is very important to me to conduct myself well, and I take it very seriously when it is pointed out to me that I have failed.. I am deeply embarassed to have given even the appearance of such loathsome behavior. It is clear to me now that I cannot entirely trust myself to post freely about speculative topics without giving offense, and so in the future I will confine myself to the Homework Help section, where I can make myself useful without danger of this happening again. However, I have promised a third installment of my opinion of the Copenhagen interpretation, and so I am committed to delivering that. Look for it in a few days; it may be a little slower in coming than the first two, because I'm feeling quite despondent just now, and my enthusiasm for the topic has dried up along with my self-respect. After that I will bow out of the discussion and return to something I know I can do (because it is my profession), helping people with their homework.

--Stuart Anderson
vkamath
QUOTE (mr_homm+)
For instance, suppose observer A stands on the shore, while observer B on a ship goes 100km north in one day. Imagine (if you can) drawing a line through the 4 dimensional spacetime from observer A today to observer B tomorrow. From A's point of view, there is a change of both position and time, so this vector would appear as a mixture of space and time displacements. From B's point of view, with his space coordinate system attached to the ship, he has stayed at the origin of his coordinate system the whole time, but aged one day, and so to him the same spacetime vector from A today to B tomorrow would appear to be purely a change of time. This vector is B's time axis. Clearly, A and B disagree on whether the same physical vector is or is not pure time. Since the vector cannot really be different from itself, the disagreement can only be the result of using different coordinate systems. This means that the concept of being pure time cannot be attached to the vector itself, but only to its expression in a particular coordinate system. The direction of time is therefore not a feature of reality.

However, it is hard to shake off the feeling that observer A is "really" right about the direction of time, just as it is hard to get over wanting to turn the map so that north is straight up. In fact, it is much harder with relativity than with the map because we experience time so very differently from space that it is quite a stretch of the imagination to see how they could be aspects of one and the same thing.


Thanks for the interesting discussion mr_homm.

With your example, from B's point of view he is moving only on the time axis. I would say even the passing of time is experienced only due to some motion on the ship. So if everything was perfectly still on the ship, then B would Not even be moving on the time axis. But this is not possible with B being a person with biological processes going on in his body.
So lets assume that instead of a person, B is a machine which records time but it is not a watch which generates its own events, instead it records events that happen outside. If B is moving through space and no events happen, it will not record time. Now B sees A moving towards it at a distance, it soon starts recording time and motion.

Doesn't that tell us that time does not exist, it is nothing but motion or events? Is that what you mean with your example?

Please consider my question as a sort of homework help. smile.gif
TRoc
Mr Homm,



I feel it necessary to post my opinion here. I have followed along with interest, but not had the time to post any response in this thread.


I read your comments concerning your personal history with Prof. Cramer, and I will say that in no way did I perceive them as derogatory. I hope that you will not take the post by Good Elf seriously, and let it effect your future actions here.


I can say, having probably the longest time spent conversing with GE on this Forum, that this is "typical", off the mark behavior. My opinion on his comment is simply that he felt threatened, in that you might have some objection to Cramer's work, and he was "hedging". He does this whenever someone points out an inconsistency in his approach. I do not recall having ever seen him admit a problem; what usually transpires is anything but productive. No doubt he will disagree with me here, but also, in his defense, he will likely apologize, and recant.


As a self-described "journeyman", GE, how do you maintain such arrogance? These statements that I see you make, like "I'm the only guy saying this", or "it's just me and Feynman who are aware of this" (I'm paraphrasing, not quoting), and then the "mafia" response to anyone who disagrees, is why I made the "Sinatra" remark in my last response to you. A change in behavior, and writing style, is in order, IMO. I've not seen any original predictions/ideas made by you, nor do I think that your "conglomerate" style revisions have less problems than the sources you are using. If anything, you create more problems with this style, than any of the individual interpretations had to begin with.


I, for one, am getting tired of seein