Why does decoherence not fully solve the measurement problem?

[conway]

For reasons which will not be immediately obvious to you, it turns out that those particular "forbidden transitions" turn out to not have an oscillating dipole moment. It's just one of those things.

I am perfectly well aware of how to break down the multipole expansion of a charge distribution, oscillating or not. It is basic spectroscopy. So on this point, I think you are correct and your model will get these selection rules correct, because you are using the atomic eigenstates, which automatically build in the correct description of angular momentum conservation.

Good insight. I think when I wrote "for reasons which will not be immediately obvious (to you)", what I meant was the reasons were not obvious to me. I just remember evaluating dipole moments for some special cases and having them all come out to zero.\

I still don't understand why you resist accepting the basic antenna premise. You know how to calculate the dipole moments, you know the antenna formulas, and they clearly come out pretty close. Are you saying you think they come out close but not close enough? I haven't sketched out the argument for the B coefficients but I can do that if you want.

The reason I can't do the Rabi calculation is that you still don't accept the premise that if the atomic antenna is absorbing energy, then the p state is growing at the expense of the s state. It's like you accept the calculation of the oscillating dipole moment but deny the fact that Maxwell's equations should apply.

 

[collinsmark]

Hello conway,

I took quite a lot of flak yesterday for suggesting that the pure eigenstates of a hot gas in thermal equilibrium were an artifact of the Copenhagen interpretation. I claimed that it is just as consistent with experiment to assume that all the atoms are in a superposition of eigenstates. I haven't seen anyone post an experiment which shows how you can distinguish these two descriptions. So I'm thinking it might be a nice gesture is someone would acknowledge that I might have been correct on this small point.

I'm not sure anyone is claiming that all the atoms in a hot gas in thermal equilibrium are all in pure energy eigenstates (at least I don't think anybody is claiming this).

Personally, I agree with you that a given atom, that hasn't just released a photon, is far more likely to be in some sort of superposition of energy eigenstates at any given time. Even if the atom is mostly in a eigenstate, there is likely at least a little superposition of other eigenstates, as long as some sort of perturbation has taken place. So yes, in my opinion, I acknowledge you are correct on this.

I think the objection is only in terms of your claim that an electron radiates energy merely by being in a superposition of energy eigenstates.

The way I understand the standard theory is as such. Suppose an atom is prepared into a superposition of two energy eigenstates, say a linear combination of one s and one p, and if then left in a vacuum isolated chamber, it will remain in that superposition state for some time. During this time it will not radiate any energy at all (regardless of the fact that the wave-function's expectation value is oscillating). Then suddenly it will emit a photon which has an energy which is exactly the excitation energy from the s state to the p state (whichever two states were in the superposition). Immediately after the emission, the electron is an energy eigenstate (the s state, in this example). Of course if the atom were then perturbed, by being bumped into another atom, it would go back into some sort of superposition of states (not necessarily like it was before, and not necessarily a superposition of just two energy eigenstates).

The amount of time that the atom remains in the superposition of states (before emitting the photon) is a probabilistic function of the relative amounts of the eigenstates in the superposition. A 90% s and 10% p will statistically last longer in the superposition state than a 50-50% combination. The extra energy that can be thought of as "boosting" the energy up to the p state, such that a photon with the right energy can be emitted, is a function of the quantum fluctuations in the zero-point vacuum energy (that might be a very bad way to put it). Perhaps I should reword that. There is a probability that the electron might be found in the p rather than s state, and that probability determines the statistical lifetime of the superposition state. (It has been said that in QM, there really is no such thing as spontaneous emissions and that all emissions can be thought of as stimulated emissions -- the spontaneous emission case is really just a special case of stimulated emission, where the emission was stimulated by the zero-point vacuum energy.)

The point of all of that, is when it comes to electromagnetic radiation of an electron in a superposition of states, it's either all or nothing. Either the atom remains in the superposition -- radiating nothing, or it emits a photon which has an energy equal to the difference in energy between the two energy eigenstates in the superposition. The ratio of the relative eigenstates in the superposition has no bearing on the photon's energy (well, assuming that the two energy eigenstates are both at least present to some degree) -- it only has an impact on the amount of time it takes for the superposition state to decay. Or in the case of stimulated emission, it affects the probability that stimulated emission will occur.

This is experimentally verifiable. It can be performed with a trip to the Radio-Shack(TM), and a purchase of a small neon bulb, a current limiting resistor, and a diffraction grating or prism. I'm guessing the cost of the experiment materials might be under around $15. Attach one of the resistor's leads to one lead of the neon bulb. Plug the spare leads into a nearby wall socket. Use the diffraction grating or prism to view the spectrum. You'll notice that the only light is in very, very narrow bands in the spectrum. The difference between these bands corresponds to certain excitation energies between different energy eigenstates of neon.

If an electron, in a state of superposition between two energy eigenstates were to continuously radiate (such as gradually becoming less of p and more of s), the resulting spectrum would be more continuous, and you wouldn't see the discrete bands. But continuous (broader) bands are not observed in the $15, Radio-Shack(TM) experiment. The observed data show the radiated bands are very, very narrow.

(All this of course hinges on accepting the idea that E = h \nu, but that's been quite well established going back to 1905.)

[Edit: Sometimes it is advantageous to approximate atoms as only being in pure energy eigenstates, if one is not concerned about position and momentum, and if nearly all of the measured interactions only deal with energy. In QM, what you measure is what you get -- if you measure energy, the wave-function appears to collapse to to an energy eigenstate. If you measure position, the wave-function appears to collapse to a position eigenstate (which resembles a Dirac delta function, and is necessarily a superposition of energy eigenstates). But if nearly all the interactions of the experiment involve energy, and the measurements involve energy, then approximating everything as only being in pure energy eigenstates is often useful. It certainly simplifies things a lot. On the other hand, this approximation can mislead students into believing that atoms only occur in pure energy eigenstates. It is common for 1st year chemistry students to mistakenly believe that electrons in atoms only occur in these well defined electron orbitals or clouds (represented by the energy eigenstates), and that's it. We know that the shape is quite different (and time varying) when things are in superposition. But the misconception still persists. In all fairness though, even if it is a misconception, it still holds up pretty well as an approximation if the only thing that is of any concern is energy.]

 

[conway]

Hi Mark

Thanks for taking the time and effort to write such a detailed explanation of the emission process. You deserve some credit for being the first one to step up to the challenge of identifying an experiment which refutes my point of view. I’m sorry to have to tell you that I can’t agree with your refutation. I’ll try to explain why.

First of all, I am glad that you agree that atoms can be in a superposition of energy states, and that those superpositions will often (as in the s-p case) lead to an oscillating charge distribution (not to quibble but you call it an “expectation value”). I think you are onside with Spectracat so far.

What I am only beginning to grasp is that both you and Spectracat, while allowing the charge distribution to oscillate, do not allow the electron to radiate as an antenna. I find this perspective utterly baffling, and consider it to be the worst of both worlds vis-a-vis the Schroedinger versus the Born interpretations. (I hope this is neutral enough: I’m going to refrain henceforth from calling them “my wave interpretation versus your Copenhagen interpretation.) You retain the “quantum leap” of the old Bohr atom even though the Schroedinger atom makes it unnecessary by allowing for an orderly passage between eigenstates via time-evolution.

You say: “I think the objection is only in terms of your claim that an electron radiates energy merely by being in a superposition of energy eigenstates.” Correct; and this claim is in fact the central pillar of my worldview. I sink or swim with it.

You further state: “The point of all of that, is when it comes to electromagnetic radiation of an electron in a superposition of states, it's either all or nothing. Either the atom remains in the superposition -- radiating nothing, or it emits a photon which has an energy equal to the difference in energy between the two energy eigenstates in the superposition.” Again, hits at the crux of my worldview: in my picture, the antenna is radiating continuously, so long as the superposition persists. The amount of energy radiated is arbitrary: in the absense of the external field, it will radiate all the available energy (one-half a quanta for a 50-50 superposition) until it stabilises in the ground state; in the presence of an ambient field, it will either emit or absorb energy as the as the phase of the driving field leads or lags the phase of the oscillating charge.

I have shown that with my model I can easily estimate the emission rates (the Einstein A coefficient) by a simple ballpark calculation. I can do the B coefficients as well if anyone is interested. So my model does not claim to give different results than the standard model.

Now let me address your counterexample of the neon lamp’s emmision spectrum. You believe that the continuously oscillating expectation value would give rise to a distributed spectrum. I’m understanding you see it as something like the Bohr atom where the orbit spirals inwards at higher and higher speeds; correct me if I’m wrong. In any case, this is not what the Schroedinger equation gives me. The frequency of charge oscillation is constant throughout the transition, and it is the difference of the ground state and excited state frequencies. Tell me if you need me to elaborate on this, because it should be quite straightforward from the expression for the wavefunction. The result is that my tiny antennas give exactly the same spectrum as your “quantum leaps”.

Finally: I really, really don’t like to invoke authority in these discussions. I think what’s wrong with physics these days is that everything is about what papers you can quote. People are throwing citations back and forth and there’s not that much actual physics being argued. I like to think my arguments should stand or fall on their merits and not on whom I can reference. But it is also a fact that starting in the 60’s a research group led by Jaynes did a lot of work to see just how far you could go using the combination of classical light and the quantum atom. I’m sure people here have vaguely heard of this, at least anecdotally. I wonder what people think they came up with if it wasn’t basically the kind of things I am talking about? I’ve never read any of their stuff myself but if they didn’t deal with my little atomic antennas, then I can’t imagine what they spent their time on.

 

[collinsmark]

Hello conway,

I've been thinking about this since my last post, and perhaps I have some insight that might help you if you decide to continue the theory you've been working on, partially involving atom's acting like antennae.

You've mentioned that antennae described in your model have an extremely high Q.

Let's consider a macroscopic, ideal antenna that has nearly infinitely high Q at certain frequencies. If you were to attach a signal generator to this antenna, it would only radiate power at these certain frequencies. Since it's an ideal antenna, at these frequencies it would radiate energy with 100% efficiency. But at any other frequencies, the power would be purely reactive, and it would transmit nothing. When the signal generator is not at one of these specific frequencies, the antenna does not radiate, but it does not draw any real power from the signal generator either (it's acting like an ideal capacitor or an ideal inductor; or perhaps like an open circuit). So the antenna is still 100% efficient. No power is ever wasted by the antenna.

The antenna can also be used for reception too. If the electromagnetic field around the antenna is exactly one of these frequencies, a voltage will be produced at the antenna terminals, which can be used to gather real power from the electromagnetic field. But if the field is at any other frequency, the thing is useless as a receiver.

Now let's shrink this infinite Q, ideal antenna down to the size of an atom, and bring up the superposition of the s and p eigenstates. Let's also accept the relationship of E = h \nu. Suppose the tuned frequencies of the antenna conform to \nu = E/h and the energy E corresponds to the excitation energies of the atom between the ground state and excited states.

If the electron was in an excited energy eigenstate, it would have enough energy to produce one of the tuned frequencies of the antenna and emit a quantum of energy. But as soon as it did so, the available energy would drop according to E = h \nu, and the available energy would correspond to a lower energy eignenstate, where another quantum of energy might be emitted (at a different tuned frequency), until eventually the energy reaches the ground state.

Now let's imagine that the electron is in a superposition of states. Suppose it is in a superposition between its ground state and the first excited state. Would it be able to radiate this extra exited energy to other atoms around it? No! Because the available energy isn't enough to correspond to one of the antenna's tuned frequencies (via \nu = E/h). The energy just stays in the atom. The atom does not radiate! Just like in the case when it was bigger, the antenna doesn't transmit any energy, but it doesn't draw any energy from the atom either. Could the atom receive just enough energy (via the antenna) to get to one of the tuned frequencies? Not exactly, but it could go past the amount by receiving the right quanta of energy, in which case it would simply be in a superposition of different energy eigenstates (although now it could release a particular quantum of energy).

The point of all of this is that even using your semi-classical model where atoms act like high Q antenna, the atom will still only radiate energy having specific quanta. This is almost just like photons. And it sort of agrees with some experimental evidence.

Of course, once again, it all hinges on E = h \nu.

So I believe that if you continue your theory, you'll ether have to abandon the idea that electrons/atoms continuously radiate energy merely by being in a superposition of states, or abandon E = h \nu as well as Einstein's photoelectric effect (and perhaps anything in quantum mechanics that is based on such results).

[Edit: When I wrote the above, I was assuming that the antenna's tuned frequencies are somehow tied to the state that the electron happens to be in (superposition or not). Re-reading the above I seem to have left this out. If they were totally independent, the atom could release energy quanta corresponding to higher excited states (lower frequency spectra -- still quantized though) even though the electron was near the ground state. If you were to power a filament in a bulb, the radiation spectra would first behave as if the electrons were in a highly excited state, only to produce the lower state quanta wavelengths only when the gas became very hot -- totally backwards from experimental data! But that's not what I meant when I wrote the post. What I neglected to say was that the quanta that the electron can radiate or absorb would need to be tied to the state of the electron. Given that, the above post still holds, and the antenna-model atom would not continuously radiate merely by being in a state of superposition. Anyway, thinking about all this is just giving me a bad headache. Sorry conway, but I think you're on your own on this one.]

 

[conway]

SpectraCat, I hope I am not misrepresenting your last post when I say that you seemed to accept my characterisation of the superposition of s and p states as an oscillating charge distribution, but maintained that it would not radiate energy energy in a continuous way, antenna-style, while in that state:

Yes, there is a time dependent oscillation of the charge density in this picture. The oscillation will even also have a non-zero dipole component if you choose a single p-orbital for the expansion. However, as I said, in the absence of an external perturbation, such a superposition will persist forever with no change in the expansion coefficients for the eigenstates. This is basic stuff! Write out the expansion and show me the time-dependence of the coefficients for the superposition state.

And later you continue:

"As I said, it cannot lose energy in the continuous fashion you claim .. it can only lose discrete quanta of energy. This has been verified experimentally. That is part of the reason why the expansion coefficients (10% and 90%) are time stable in the self-consistent, verified, peer-reviewed description given by standard QM. "

And you conclude:

“Just to be completely clear, the vacuum fluctuations which give rise to spontaneous emission are considered external perturbations, so SQM correctly predicts emission from superposition states. They are time-stable until the instant that the fluctuation comes into being and perturbs them, at which point they can radiate .. as I mentioned before, this process is effectively instantaneous ... the system goes from excited atom directly to ground state atom + photon in the transition. This is not at all controversial, it is basic first-year QM. So get off your high-horse and support your model.”.

Surely you are not claiming that this is the Copenhagen interpretation? Unless I’m very wrong, I thought according to Copenhagen, the atoms were distributed between the discrete energy levels, all of them in pure eigenstates, no superpositions, and the photons are emitted instantaneously as the atom jumps between energy levels? Or is what you’ve called “SQM” different from what I think Copenhagen is?

It just doesn’t add up to me. I can see Copenhagen somehow trying to make do with time-stable eigenstates that instantaneoulsy jump from one level to another: I don’t like it but I suppose it’s consistent: the eigenstates are not antennas, so to get from one to the other they must make some magical transition. But I can’t see how SQM would allow superpositions of those eigenstates and then compel them to remain time-stable rather than simply allowing them to radiate according to Maxwell’s equations. Are you sure you’ve got it right?

 

[SpectraCat]

SpectraCat, I hope I am not misrepresenting your last post when I say that you seemed to accept my characterisation of the superposition of s and p states as an oscillating charge distribution, but maintained that it would not radiate energy energy in a continuous way, antenna-style, while in that state:
And later you continue:
And you conclude:
Surely you are not claiming that this is the Copenhagen interpretation? Unless I’m very wrong, I thought according to Copenhagen, the atoms were distributed between the discrete energy levels, all of them in pure eigenstates, no superpositions, and the photons are emitted instantaneously as the atom jumps between energy levels? Or is what you’ve called “SQM” different from what I think Copenhagen is?

It just doesn’t add up to me. I can see Copenhagen somehow trying to make do with time-stable eigenstates that instantaneoulsy jump from one level to another: I don’t like it but I suppose it’s consistent: the eigenstates are not antennas, so to get from one to the other they must make some magical transition. But I can’t see how SQM would allow superpositions of those eigenstates and then compel them to remain time-stable rather than simply allowing them to radiate according to Maxwell’s equations. Are you sure you’ve got it right?

Yes, I am sure. You are confused about several things. There is no restriction in SQM or CI for "pure eigenstates". When you start from a system of pure eigenstates as is typical, then you can create superposition states IF AND ONLY IF a time dependent perturbation is present that can couple the levels .. that is a big part of what Rabi oscillations *are*. They describe the smooth oscillation of the superposition between the ground and excited states of a two-level system, at a frequency which depends only on the magnitude of the perturbing field. If the oscillations are going, and then the perturbing field is switched off, the system becomes "trapped" in whatever particular superposition it was in at that instant (say, the 90-10 example we have been discussing). This system will persist as a stable superposition state until it is perturbed somehow, say by a vacuum fluctuation to initiate spontaneous emission as I have described.

By playing clever tricks with photon phase and polarization, physicists can actually use this to create superpositions involving "dark states", which have no route to decay by photoemission, and thus can persist for arbitrarily long times. I have not studied these papers in detail, but I think the gist of the technique is they set the system into a Rabi oscillation using the optical excitation, and then quickly switch the light off when the phase of the Rabi oscillation corresponds with zero coefficient for the bright state. However the states are prepared, the important point for the current discussion is that, since the coefficients can't change after the field has been switched off, the system is stuck in that superposition state, and can't decay, because the dark states do not have any allowed routes back to the ground state. I can't see any hope of describing such a process using a classical antenna model for atomic absorption.

You are getting hung up on the oscillating charge density, because you are thinking about the system classically. There is nothing classical about it. Maxwell's equations in the classical form you are referring to do not apply ... you need to use the versions for quantized fields in order to properly describe the emission. I am not an expert in QFT, and I don't really know how to do that. However, I do understand the proper semi-classical description (classical fields, quantized electronic states), and I understand the phenomenology of spontaneous emission. That is what we need to address your example, as I have been saying.

An important point that you may be missing is that I am most emphatically *not* saying that superposition states will not radiate ... they will definitely radiate by spontaneous emission as follows. When the system is in a superposition state, the squared coefficients describe the probability that a measurement will cause the system to be "resolved" into the various component states due to decoherence. As I understand it, that is what happens when a vacuum fluctuation initiates spontaneous emission ... in the case of a superposition state, if the interaction "resolves" the system into the ground state, nothing happens .. it is already stable. However if the fluctuation perturbs the system into the excited state, then it can decay to the ground state via the emission of a single photon. Thus the probability of spontaneous emission from such a state is described by the normal Einstein A coefficient, multiplied by the probability of finding the system in the excited state.

Finally, in your reply to Collinsmark, you wrote:

You say: “I think the objection is only in terms of your claim that an electron radiates energy merely by being in a superposition of energy eigenstates.” Correct; and this claim is in fact the central pillar of my worldview. I sink or swim with it.

You are going to sink, because that picture is incorrect for quantum systems, as I have been trying to explain to you. Please, for both our sakes, write down the time-dependent wavefunction describing the two-state superposition of s and p states that *you* introduced as part of your system. Examine it carefully, and try to find the time dependence of the expansion coefficients .. you cannot, because it is not there. The time dependence has to be induced by an external perturbation ... research time-dependent perturbation theory a bit and hopefully you will be able to understand this a little better.

 

[conway]

Yes, I am sure. You are confused about several things. There is no restriction in SQM or CI for "pure eigenstates". When you start from a system of pure eigenstates as is typical, then you can create superposition states IF AND ONLY IF a time dependent perturbation is present that can couple the levels...

SpectraCat, I think I was trying to get onside with what you called "basic first-year QM". In this quote you refer to a system of pure eigenstates as "typical". So was I at least more or less correct in describing SQM's version of say, an hot gas in thermal equilbrium with radiation inside a box? So the gas molecules are distributed between the ground states and the excited states according to A*exp(-E/kt), with basically no atoms in a superposition?

You are getting hung up on the oscillating charge density, because you are thinking about the system classically. There is nothing classical about it. Maxwell's equations in the classical form you are referring to do not apply ... you need to use the versions for quantized fields in order to properly describe the emission. I am not an expert in QFT, and I don't really know how to do that.

But didn't I get pretty close to the correct emission rate with my ballpark calculation of radiation resistance for the short antenna?

However, I do understand the proper semi-classical description (classical fields, quantized electronic states)...

Are you talking here about the research led by Jaynes starting in the 1960's which I mentioned a couple of posts back? I have never read their papers but I can't imagine what they could have been doing unless it was just the type of things that I am talking about, calcuating radiation resistance for small antennas etc. Would that not be the proper semi-classical description?

Please, for both our sakes, write down the time-dependent wavefunction describing the two-state superposition of s and p states that *you* introduced as part of your system. Examine it carefully, and try to find the time dependence of the expansion coefficients .. you cannot, because it is not there. The time dependence has to be induced by an external perturbation ... research time-dependent perturbation theory a bit and hopefully you will be able to understand this a little better.

It's true that the coefficients are not time dependent. But that's just because you derive those coefficients using an incomplete formula, i.e. Schroedinger's equation, that doesn't include a term for electromagnetic radiation, so your expression for the time evolution is only an approximation. The time variation of the coefficients comes in naturally when you include the effect of Maxwell's equations on the system.

 

[SpectraCat]

SpectraCat, I think I was trying to get onside with what you called "basic first-year QM". In this quote you refer to a system of pure eigenstates as "typical". So was I at least more or less correct in describing SQM's version of say, an hot gas in thermal equilbrium with radiation inside a box? So the gas molecules are distributed between the ground states and the excited states according to A*exp(-E/kt), with basically no atoms in a superposition?

Yes and no ... the *average* distribution is given by the Boltzman factors in terms of pure quantum states, but at any instant in time, there can certainly be atoms in superposition states, since there are time-dependent perturbations (i.e. the radiation fields), available to mix the states. Remember that the superposition states will decay due to spontaneous emission, they just won't do it as quickly as the pure excited states. (Note: I will have to classify my position on that last statement as "pretty darn sure but not certain" ... I think one really needs to use QFT to get the correct answer, and I am not facile enough with QFT to work out the answer without a significant amount of work that I don't have time for right now).

But didn't I get pretty close to the correct emission rate with my ballpark calculation of radiation resistance for the short antenna?

So what? I pointed out several other flaws with the physics of that model (which have been corroborated by others), so I am inclined to believe that it was just coincidental. I'd want to see a more detailed analysis, and a couple of other successful predictions before I am willing to accept that it was more than a coincidence.

Are you talking here about the research led by Jaynes starting in the 1960's which I mentioned a couple of posts back? I have never read their papers but I can't imagine what they could have been doing unless it was just the type of things that I am talking about, calcuating radiation resistance for small antennas etc. Would that not be the proper semi-classical description?

No, I am talking about the same semi-classical picture that is typically used in spectroscopy to derive formulae like the Rabi formula and Fermi's Golden rule for transition rates. You assume that the EM field is classical, with a continuous amplitude that represents the magnitude of the perturbation coupling the quantum states. It is much older than the 60's .. it dates back to Einstein and Dirac. I am unfamiliar with Jaynes' papers, but I will look then up when I have time.

It's true that the coefficients are not time dependent. But that's just because you derive those coefficients using an incomplete formula, i.e. Schroedinger's equation, that doesn't include a term for electromagnetic radiation, so your expression for the time evolution is only an approximation. The time variation of the coefficients comes in naturally when you include the effect of Maxwell's equations on the system.

Schrodinger's equation may be incomplete, but I don't agree that you can apply the classical versions of the Maxwell equations to this system .. at least not to get physically sensible results. However, if you are saying that theories incorporating quantum descriptions of Maxwell's equations such as QFT or QED can supply a better description of this problem, then by all means I agree with that statement. I have not worked through those derivations for myself for a rather long time, but as I recall it, what you get from those treatments is Einstein's A-coefficient for spontaneous emission. As I have said, that is why I feel justified using it in the context of our current discussion, and I believe I have interpreted it's significance correctly.

 

[Cthugha]

Are you talking here about the research led by Jaynes starting in the 1960's which I mentioned a couple of posts back? I have never read their papers but I can't imagine what they could have been doing unless it was just the type of things that I am talking about, calcuating radiation resistance for small antennas etc. Would that not be the proper semi-classical description?

In fact Jaynes did quite the opposite. The famous Jaynes-Cummings model (THE model of quantum optics) describes the interaction of a quantized two-level atom with a quantized cavity field mode and they tried to find out which differences occur compared to the semiclassical model. For example the semiclassical model can explain Rabi cycles of probabilities, but not stuff like revivals of population inversions after a collapse and vacuum Rabi splitting for single emitters in a cavity.

 

[conway]

Cthuga, I appreciate your input, but I don't understand it, especially your use of the phrase "just the opposite". You say they compare the quantized two-level atom with a quantized cavity field mode (call this A) to the semiclassical model (B). Are you saying they compared A to B and found B could explain some but not all? That's what I understand...that A is SQM and B is "semiclassical".

If I've understood that correctly, that I have to ask again: just what was the "semi-classical model" they used if not my little antennas with their radiation resistance etc? I'd really like to know.

 

[cesiumfrog]

Semiclassical here (regarding foundational QM) often refers to classical EM fields interacting with some quantum-mechanical particles. So it accounts for the wave-particle duality of the electron, but not for the particle duality of the photon.

The obvious first improvement of this model is called quantum electrodynamics (QED). This is obtained by quantising the EM field (thus accounting for creation and absorption of individual photons) and which basically results in perfect agreement with experiment (provided the number of electrons stays fixed).

In particular, semi-classical does not mean "little antennas with their radiation resistance". Such a model would be termed entirely classical, but it would be disparaged as ad-hoc (since, although one can perhaps come up with such a little classical model for any single experiment, you don't have a completely consistent a priori framework for modelling all experiments). Such a classical model even takes numerous results from standard QM as parameters (whilst standard QM obviously derives those itself from far fewer parameters), which contradicts justification for differing with standard QM.

Conway, since you seem reluctant to acknowledge photons, why don't you study the experiments that persuaded the community of their existence: Compton scattering (where photons bounce off a particle like ping-pong balls), the photoelectric effect (where some electrons accumulate escape-energy faster than could be explained by uniform irradiation, not to mention that if the light wavelength is lowered then electrons abruptly stop escaping regardless of energy availability), and single-photon sources (which have facilitated some elegant experiments in foundational QM, such as interference between photons emitted by different sources at different times)?

 

[conway]

Semiclassical here (regarding foundational QM) often refers to classical EM fields interacting with some quantum-mechanical particles. So it accounts for the wave-particle duality of the electron, but not for the particle duality of the photon.

The obvious first improvement of this model is called quantum electrodynamics (QED). This is obtained by quantising the EM field (thus accounting for creation and absorption of individual photons) and which basically results in perfect agreement with experiment (provided the number of electrons stays fixed).

In particular, semi-classical does not mean "little antennas with their radiation resistance". Such a model would be termed entirely classical, but it would be disparaged as ad-hoc (since, although one can perhaps come up with such a little classical model for any single experiment, you don't have a completely consistent a priori framework for modelling all experiments). Such a classical model even takes numerous results from standard QM as parameters (whilst standard QM obviously derives those itself from far fewer parameters), which contradicts justification for differing with standard QM.

Conway, since you seem reluctant to acknowledge photons, why don't you study the experiments that persuaded the community of their existence: Compton scattering (where photons bounce off a particle like ping-pong balls), the photoelectric effect (where some electrons accumulate escape-energy faster than could be explained by uniform irradiation, not to mention that if the light wavelength is lowered then electrons abruptly stop escaping regardless of energy availability), and single-photon sources (which have facilitated some elegant experiments in foundational QM, such as interference between photons emitted by different sources at different times)?

Cesiumfrog, it's hard for me to know what to make of all this. A week ago I would have never believed that a group like Jaynes et. al. could be the universally acknowledged leaders of the "semi-classical school" without having dealt with my "little antennas with their radiation resistance". When SpectraCat steadfastly maintained this all last week, I could only marvel at what I considered his ignorance or willful blindness, especially when he insisted he knew all about "semi-classical treatments". How, I wondered, can he believe he knows what he's talking about if he's never even heard of calculating the radiation resistance of the hydrogen atom to get the Einstein A coefficient?

Cesiumfrog, I know I'm going to disappoint you because I sense that you feel you are being patient with me, trying to gently guide me back onto the right path by shaking of the blinders that prevent me from seeing the light. The sad fact is that what you have told me today only reinforces my conviction, my dementia as FrameDragger so ably diagnosed it, that I know things that nobody else does, that I'm on the track of something really big. Because if Jaynes et al weren't dealing in my little antennas, then maybe I'm the first. Maybe I have the answer to the big questions that have been puzzling the great thinkers for over a century...well, you see how the mind works.

What you probably can't imagine is how many different ways that I find support for my obsession. I don't want to provoke you but the fact is that I find several baffling contradictions, for lack of a better word, in your own arguments as presented in the four short paragraphs above; I'd like to try to explain them to you from my point of view, but I am almost sure that it would all end badly as it did with SpectraCat. You would take my attemps to explain my ideas as insufferable arrogance and gross disrespect for those who are obviously more knowledgeable than me.

 

[Frame Dragger]

Cesiumfrog, it's hard for me to know what to make of all this. A week ago I would have never believed that a group like Jaynes et. al. could be the universally acknowledged leaders of the "semi-classical school" without having dealt with my "little antennas with their radiation resistance". When SpectraCat steadfastly maintained this all last week, I could only marvel at what I considered his ignorance or willful blindness, especially when he insisted he knew all about "semi-classical treatments". How, I wondered, can he believe he knows what he's talking about if he's never even heard of calculating the radiation resistance of the hydrogen atom to get the Einstein A coefficient?

Cesiumfrog, I know I'm going to disappoint you because I sense that you feel you are being patient with me, trying to gently guide me back onto the right path by shaking of the blinders that prevent me from seeing the light. The sad fact is that what you have told me today only reinforces my conviction, my dementia as FrameDragger so ably diagnosed it, that I know things that nobody else does, that I'm on the track of something really big. Because if Jaynes et al weren't dealing in my little antennas, then maybe I'm the first. Maybe I have the answer to the big questions that have been puzzling the great thinkers for over a century...well, you see how the mind works.

What you probably can't imagine is how many different ways that I find support for my obsession. I don't want to provoke you but the fact is that I find several baffling contradictions, for lack of a better word, in your own arguments as presented in the four short paragraphs above; I'd like to try to explain them to you from my point of view, but I am almost sure that it would all end badly as it did with SpectraCat. You would take my attemps to explain my ideas as insufferable arrogance and gross disrespect for those who are obviously more knowledgeable than me.

Conway, I don't believe you're demented. I laid out a number of possiblities, of which "mental illness" is simply one, and not dementia. Given some time, I find you to be somewhat contradictory. When it comes to general physics, you seem utterly capable, able to give advice, etc. It may just be that this is the current limit of your understanding in the context of an internet forum.

If a trusted advisor, professor, rabbi, whatever... whom you presented your theory to carefully examined it, then laughed it off... how would you react? Your retreat into sarcasm and bitterness is understandable given the admittedly semi-hostile environment around you at this point. I wish that you would stop being defensive long enough to answer the questions posed to you by SpectraCat and Cesiumfrog, rather than beat a hastey retreat into the rhetoric of desperation.

Maybe you're just a crank, and I'm giving you too much credit (which would be odd, I'm not usually generous in that fashion), but I think this is a self-esteem issue for you, or some kind of article of faith. Maybe the issue is that you are unwilling to present your theory in the face of criticism and even scorn? If so, I would ask that you consider weathering the storm.

Personally, I think you want to get to point C from A without passing through B, and it pisses you off to have what you thought (think?) is a really elegant theory that still makes some kind of sense to you, blown away by literally EVERYONE you presented it to. That only leaves your ego (in the psychological sense, not the insult) very little room:

1.) You can admit that you're wrong, go back to the drawing board and resume at the point where you decided the learning was done, and it was time to become an amatuer theoretician. This is the healthy and normal response, albiet an unpleasant one

2.) You reject the faceless non-people who are just text on a screen to you after all, and stick to the principles and gumption that took you this far. Not a bad choice, but rigid, and therefore prone to rupture when you encounter more personal rejection

3.) We are all assholes who don't recognize your genius. Despite the professionals here believing otherwise, you are right in the face of all denial. What you formulated makes sense, following naturally from patterns you picked up during research and schooling for a career other than physics. This is very intuitive for you, and a joy ("obsession"), and who are we to piss all over it, right?

4.) Get lost in the numerology. "What you probably can't imagine is how many different ways that I find support for my obsession." I can believe it, much as I can believe that people see the Madonna in a pancake, or that we all see patterns because we're hardwired to find them (even when they are not there). People believe in god, a devil, angels, etc... your faith is hardly stranger. This is your religion, and we're not respecting that, much as you're not respecting that you came to a site, presented a theory, and upon rejection of it you now refuse to engage other than to defend your IMAGE.

It's always some variation on the old theme: MICE: "Money, Ideology, Compromise/Coercian, Ego". They'll make you betray confidences, change your life, and maybe end it... naturally they drive us to more subtle and less destructive ends. Ideology, and Ego for you conway, but not dementia. You're not stupid, or forgetful... you're excited like an addict chasing a high, and if you have to give up the notion of being "on to something big", then what's the point, right? Doesn't the knowledge that you're discovering something that eludes "great thinkers for over a century" excite and please you? It's like a secret garden, but sadly you made the error of turning over your fantasy to the cold embrace of the scientific method.

My advice? Find meaning, excitement, and purpose beyond "the next big thing". If that's what you think science is, and how most of physics is "done", you're in for some pain. Finally, if you're unwilling to engage someone as helpful and polite as cesiumfrog, why bother with any of this? What's the worst thing that could happen... Cesium rejects your hyothesis. The issue of "arrogance" was not your theory, but the manner in which you present it, as being on a par with QED and QFTs in general. I also seem to recall you kept telling Cat that something was "his theory" versus "your theory", when it was really "you vs. QM".

I suspect that if you don't actively attempt to piss off the people you present this theory to, you stand to learn something. Of course, to make this cicle complete, maybe you don't WANT that. Think about what you really want out of this... to crow about a theory you can't/won't share or adequately defend?

 

[Cthugha]

Cthuga, I appreciate your input, but I don't understand it, especially your use of the phrase "just the opposite". You say they compare the quantized two-level atom with a quantized cavity field mode (call this A) to the semiclassical model (B). Are you saying they compared A to B and found B could explain some but not all? That's what I understand...that A is SQM and B is "semiclassical".

If I've understood that correctly, that I have to ask again: just what was the "semi-classical model" they used if not my little antennas with their radiation resistance etc? I'd really like to know.

First: I did not read the entire thread, so I do not know what exactly is your understanding of semiclassical.

What Jaynes and Cummings did was: Take a two-level atom and treat it quantum mechanically. Now they studied the interaction of this quantum mechanical atom with classical light (semiclassical treatment) and a quantized cavity field mode (Jaynes-Cummings model, quantum treatment). So the difference is the treatment of the em field.

Because if Jaynes et al weren't dealing in my little antennas, then maybe I'm the first.

Again, I have not read the whole thread and am not sure what exactly you are after. It is well known that a linear combination of energy eigenstates in QM can lead to an oscillating motion of charge and therefore an oscillating dipole. This is often explained in analogy to antennas in beginners' courses on em-theory or group theory because you can see that transitions are only dipole-allowed if they show a different symmetry. However, this model is not exhaustive. You need to go further to include quadrupole allowed transitions and need much, much more to explain nonclassical light from single photon sources.

 

[conway]

Okay, that's helpful, and it seems to agree with the way Cesiumfrog described the Jaynes school of thought. I thought all along what I was doing was the "semi-classical approach" but maybe I was wrong. I'm understanding that they use the e-m field as a perturbation, and then retreat to the SQM framework to calculate transition probabilities between eigenstates... the old Bohr "quantum leap". That's exactly halfway to my approach so I guess my ststem would have to be called the "75%-classical approach" because I treat the field as classcal e-m and the atom as a tiny oscillating dipole. So I don't have "transition probabilities" and quantum leaps, I have radiation resistance and continuous power output.

It's still hard for me to believe that no one has staked out this territory already. It seems pretty obvious. There's all kinds of phenomena that are totally natural in this system. I'd like to work though the physics with anyone who's interested but I'm having a problem getting people to take those "little antennas" seriously. People seem to agree that they exist theoretically but then insist that I'm not allowed to apply Maxwell's equations to them. When I do and get seemingly correct results (e.g. my ballpark calculation of the Einstein A coefiicient) it is dismissed as coincidence. Other people just want to psychoanalyze me. But then, you haven't asked me to rehash the old arguments from this thread. So let it be.

(EDIT): I hope this is not a further infraction, but I just wanted to clarify that my post was originally three paragraphs long and the last paragraph was deleted by the moderator.

(EDIT 2): There is just a little glitch in the notification system where by when I posted my first edit, it messed up the notification. The notification bar originally said: Edited by ZapperZ...Reaason: Removed advertisements for personal theory. Just wanted to clarify that it wasn't me editing my own post. (But this is.)

 

[Frame Dragger]

Okay, that's helpful, and it seems to agree with the way Cesiumfrog described the Jaynes school of thought. I thought all along what I was doing was the "semi-classical approach" but maybe I was wrong. I'm understanding that they use the e-m field as a perturbation, and then retreat to the SQM framework to calculate transition probabilities between eigenstates... the old Bohr "quantum leap". That's exactly halfway to my approach so I guess my ststem would have to be called the "75%-classical approach" because I treat the field as classcal e-m and the atom as a tiny oscillating dipole. So I don't have "transition probabilities" and quantum leaps, I have radiation resistance and continuous power output.

It's still hard for me to believe that no one has staked out this territory already. It seems pretty obvious. There's all kinds of phenomena that are totally natural in this system. I'd like to work though the physics with anyone who's interested but I'm having a problem getting people to take those "little antennas" seriously. People seem to agree that they exist theoretically but then insist that I'm not allowed to apply Maxwell's equations to them. When I do and get seemingly correct results (e.g. my ballpark calculation of the Einstein A coefiicient) it is dismissed as coincidence. Other people just want to psychoanalyze me. But then, you haven't asked me to rehash the old arguments from this thread. So let it be.

(EDIT): I hope this is not a further infraction, but I just wanted to clarify that my post was originally three paragraphs long and the last paragraph was deleted by the moderator.

YOU'RE the guy with the blog about "quantum siphoniong"?! Oh hell, you should have said that to begin with so none us wasted our time. There is nothing even APPROACHING real physics in what you do, and I might add that NO ONE has agreed with your "little antennas".

Usually, whe people put a half-baked theory forth, they at LEAST try to understand the one they're trying to replace. How ridiculous, you're just another crank pushing your theory here, which is completely contrary to the educational mission of the site.

By the by, the original paragraph made it to my email notifications, so I was able to enjoy the full post. You know, I the first time you said it (a while back) I thought you were JOKING about the Nobel... this really is textbook illusory superiority, and Kruger-Dunning. Go back to school conway, and learn what the hell it is that science IS.

You seem to know some math, but your grasp of the sceintific method is breathtakingly poor. You are also quite deceptive:

https://www.physicsforums.com/showpost.php?p=2638960&postcount=32

Oh look, that's you claiming that the photographic process has been explained by this theory... one you came up with, and are trying to propogate. It's funny, you see, I wouldn't have referred to it as though I were simply one of many who believed this, and formulated it.

 

[conway]

YOU'RE the guy with the blog about "quantum siphoniong"?! Oh hell, you should have said that to begin with so none us wasted our time. There is nothing even APPROACHING real physics in what you do, and I might add that NO ONE has agreed with your "little antennas".

Usually, whe people put a half-baked theory forth, they...

I think I said they recognized the existence of the antennas in the model, they just dispute my claim that we should allow them to radiate according to Maxwell's equations. I hope I'm not taking any of these quotes out of context:

From Spectracat, post 85:

I assure you that I understand it just fine. I never said that the wavefunction was stationary ... I said that the expansion coefficients for the two basis states don't change in the absence of an external perturbation, which is not at all the same thing. Yes, there is a time dependent oscillation of the charge density in this picture. The oscillation will even also have a non-zero dipole component if you choose a single p-orbital for the expansion. However, as I said, in the absence of an external perturbation, such a superposition will persist forever with no change in the expansion coefficients for the eigenstates. This is basic stuff! ... It is a *classical* antenna, and it has no bearing on what an atom "actually does", at least not according to the well-established theory called quantum mechanics...

From collinsmark, post 69:

...my knowledge of quantum electrodynamics (above and beyond non-relativistic quantum mechanics) is presently rather sparse, but from what I can gather, I am not presently aware of electrons radiating energy when being in a superposition of states, even though the expectation value of the wave-function may oscillate.

From Cthuga, post 104:

It is well known that a linear combination of energy eigenstates in QM can lead to an oscillating motion of charge and therefore an oscillating dipole. This is often explained in analogy to antennas in beginners' courses on em-theory or group theory because you can see that transitions are only dipole-allowed if they show a different symmetry.

From yoda jedi, post 63:

RIGHT !
clever insight

called ψ-complete view, unlike ψ-epistemic.
as for ψ-epistemic which quantum states are solely representative of our knowledge.

Okay, that last one may be a little out of context.

 

[Frame Dragger]

I think I said they recognized the existence of the antennas in the model, they just dispute my claim that we should allow them to radiate according to Maxwell's equations. I hope I'm not taking any of these quotes out of context

post 85: "It is a *classical* antenna, and it has no bearing on what an atom "actually does", at least not according to the well-established theory called quantum mechanics...

Oh yeah, he's clearly agreeing with you there. :roll:
Really, I strongly suspect that Collinsmark, who just wanted to help you, Cthuga who just wanted to help you, are going to probably NOT wanting you to allign them with your farkakt guesswork masquerading as a theory.

As for Yoda Jedi, who knows, but since his quote IS out of context, I assume you put it in for bulk fiber?

 

[SpectraCat]

To set the record straight, I for one never agreed that the description of atoms in superposition states as classical antennas has any physical significance beyond understanding the dipole-selection rules (I think this is what Cthuga is saying as well). Furthermore I have stated in several places that I don't believe that the classical Maxwell equations can be used to extract physically sensible results from the oscillating charge densities predicted by the TDSE for an atomic superposition state.

To call something a "classical antenna" implies that it can absorb and emit radiation in a classical (i.e. continuous fashion), whereby the energy coupled into or out of the system is proportional to the squared amplitude of the electric field. It is well-known that this is not a correct description of absorption and emission from atomic states, therefore I would say that the description of atoms as "classical antennas" is physically incorrect.

 

[Count Iblis]

How did |conway> collapse into |[STRIKE]conway[/STRIKE]>

 

[Frame Dragger]

Ahhhh, that sweet line through his name... it's like an icepick has been removed from my damned temple.

@Thread: Requiem in terra pacis. *wave*

EDIT: @Count Iblis: He was perturbed? Orrr... maybe he was siphoned away by the staff...

 

[SpectraCat]

Here is another example of the incorrectness of the antenna model: it doesn't give the correct explanation for superpositions of excited states. There is no physical reason why the ground state has to be used in a superposition ... if the gas is hot enough, then you should be able to observe superpositions of excited eigenstates as well.

Consider a two-state superposition of the 2s and 3p eigenstates. According to your classical antenna model, this should emit and absorb only at the lowest line in the Balmer series (i.e. the Hydrogen-alpha line at 656.3 nm). However, the quantum mechanical model I have described in past posts predicts that the emission will also occur at the Lyman-beta line (3p-->1s transition @ 102.5 nm), and in fact almost all of the emission will occur at that wavelength, since the Einstein coefficients for spontaneous emission are inversely proportional to the *third power* of the wavelength. Thus the Lyman-beta emission, which is absent from the "classical antenna" model for such a superposition, is ~260 times more likely than the Balmer-alpha emission.

 

[George Jones]

How did |conway> collapse into |[STRIKE]conway[/STRIKE]>

As has been suspected for some time, conway was the return of someone twice-banned (now thrice-banned).

 

[SpectraCat]

As has been suspected for some time, conway was the return of someone twice-banned (now thrice-banned).

Oh jeez ... what a waste of time all these threads have been. It explains a lot though .. I wonder what his handle will be the next time he raises his head? Perhaps "itrytoCONyouintothinkingmyWAY"? At least that would be more honest ...

 

[George Jones]

Oh jeez ... what a waste of time all these threads have been.

I hope not a total waste of time; you have fleshed out some arguments that you might want to use in the future, and to which you can give links.

 

[SpectraCat]

I hope not a total waste of time; you have fleshed out some arguments that you might want to use in the future, and to which you can give links.

Yes, you are right. What I really meant is that trying to convince him of anything was a waste of time ... keeping incorrect notions of how physics works out of a physics database is certainly not a waste of time.

 

[DrChinese]

Ahhhh, that sweet line through his name... it's like an icepick has been removed from my damned temple.

You're killing me!

Hey, better you than me!

 

[Cthugha]

To set the record straight, I for one never agreed that the description of atoms in superposition states as classical antennas has any physical significance beyond understanding the dipole-selection rules (I think this is what Cthuga is saying as well).

Just for the records: Yes, that was my intention. I did not mean to suggest any far-reaching analogies between classical antennas and the emission behavior of atoms.

 

[ZapperZ]

All discussions pertaining to the running of PF and policies should be done in the Feedback forum, not in this or any other threads in the physics subforums.

Zz.

 

[Frame Dragger]

You're killing me!

Hey, better you than me!

Thank you very much.

@SpectraCat: You don't strike me as a "cat" who falls for the same trick twice.

@ZapperZ: Noted. Seeing as you obviously read what I had to say on the subject, I can assume that I don't need to actually repeat it in that subforum?