B Does Photon Emission Cause Decoherence?

Feeble Wonk
Messages
241
Reaction score
44
In the never ending quest to understand a complicated idea for which I completely lack the academic requirements to do so, I'd like to ask a few basic questions that I hope will allow simple yes/no responses (to ease the frustration of the physicist/mathematician contributors). Sadly, the answer of "Your question makes no sense" is also a very real possibility, so we might abbreviate that response to "Ugh" for simplicity sake.

First question: In terms of decoherence, does the emission of a photon from a particle constitute a physical interaction with the environment/system in a similar manner to the absorption of a photon?
 
Last edited:
Physics news on Phys.org
When excited atoms passing thru the Young slits, emit a photon it changes the density matrix . It gives some which-path information the visibility of the franges decreases.
 
naima said:
When excited atoms passing thru the Young slits, emit a photon it changes the density matrix . It gives some which-path information the visibility of the franges decreases.
Does this provide information with regard to the location of the photon emitting particle?
 
Last edited by a moderator:
  • Like
Likes Feeble Wonk
Information is about the path. And so about the position.
 
  • Like
Likes Feeble Wonk
DrClaude said:
Yes.

There is a very nice experiment showing this using molecules:
Lucia Hackermüller, Klaus Hornberger, Björn Brezger, Anton Zeilinger & Markus Arndt, Decoherence of matter waves by thermal emission of radiation
http://www.nature.com/nature/journal/v427/n6976/full/nature02276.html
http://arxiv.org/abs/quant-ph/0402146
naima said:
Information is about the path. And so about the position.
Thank you both. Let me work through the sources you've provided. I might offer a follow up question later, if that's OK.
 
Last edited by a moderator:
Feeble Wonk said:
First question: In terms of decoherence, does the emission of a photon from a particle constitute a physical interaction with the environment/system in a similar manner to the absorption of a photon?
To have a decoherence-like interaction, you need interaction with a large number of degrees of freedom. If the particle (assumed to be an elementary particle or a particle with a very simple structure) and the emitted photon do not interact with the environment, nothing like decoherence will happen. The process of emission will be continuous and unitary, nothing like a quantum jump will occur. The quantum jump requires environment with many degrees of freedom. The environment may be external (e.g. surrounding gas or measuring apparatus) or internal (a complex emitting particle).

The same is true when emission is replaced by absorption.
 
  • Like
Likes Igael, Feeble Wonk and naima
This point is very interesting.
It is often said that the visibility interference pattern decreases because of a possible detector of photons. Do you say that the origin is the actual presence of another existing environment (the gas or something else)?
 
naima said:
It is often said that the visibility interference pattern decreases because of a possible detector of photons. Do you say that the origin is the actual presence of another existing environment (the gas or something else)?
Yes. To decrease visibility of interference pattern you need some environment, which can be a detector or something else.
 
  • #10
naima said:
Information is about the path. And so about the position.
Knowing which path gives information about the momentum in the direction of the path and about the position in two orthogonal directions orthogonal to it. Thus it gives only partial position information.
 
  • #11
Demystifier said:
The environment may be... internal (a complex emitting particle).
The same is true when emission is replaced by absorption.

Could you please expand on this?
 
  • #12
Feeble Wonk said:
Could you please expand on this?
For internal decoherence (in a somewhat different context) see
http://lanl.arxiv.org/abs/1406.3221 [Eur. J. Phys. 36 (2015) 045003]
and references therein.
 
  • Like
Likes Feeble Wonk
  • #13
Demystifier said:
For internal decoherence (in a somewhat different context) see
http://lanl.arxiv.org/abs/1406.3221 [Eur. J. Phys. 36 (2015) 045003]
and references therein.
Thank you. Most of the math is over my head, but the discussion and conclusion summary is excellent.
 
  • #14
Demystifier said:
To have a decoherence-like interaction, you need interaction with a large number of degrees of freedom. If the particle (assumed to be an elementary particle or a particle with a very simple structure) and the emitted photon do not interact with the environment, nothing like decoherence will happen. The process of emission will be continuous and unitary, nothing like a quantum jump will occur. The quantum jump requires environment with many degrees of freedom. The environment may be external (e.g. surrounding gas or measuring apparatus) or internal (a complex emitting particle).

The same is true when emission is replaced by absorption.

In the case of a Stern Gerlach device, I see several steps in the decoherence;
1) the degrees of freedom of the electron (spin, position) and those of the magnetic field interact and decoherence occurs. What does this "occurs" mean?
We can have at any time t many copies of the electron prepared in the same state (mixed here). We can measure say their Wigner function. It needs that they interact with macroscopic apparatus to get an image. Varying t, we see how the Wigner function and decoherence evolve.
This leads to the second point.
But before measuring the state with a macroscopic device we cannot say that decoherence completely occured. It has nothing to do to the remaining presence of little off diagonal terms. It is still possible to erase what was done. the two output beams of the SG can be the inputs of a beam merger whose output is the initial electron's state.
Things are reversible.
2) registration of the decoherence.
It is what happened when we measured the Wigner function. It is different from a screen in front of the SG. We get here a macroscopic spot which gives the value of spin measurement. In one case we measure the density matrix and in the other the spin. In both cases there is irreversibility.
This scheme can easily understood in the case of an emitted witness photon. Is it the same when the atom absorbs the photon? What is then the environment?
 
  • #15
naima said:
But before measuring the state with a macroscopic device we cannot say that decoherence completely occured.
...
Is it the same when the atom absorbs the photon? What is then the environment?
How do you know that absorption of the photon by the atom has occured? Before detecting the absorption by a macroscopic device, you cannot know that. So this is where environment is in the case of absorption.
 
  • #16
naima said:
2) registration of the decoherence.
It is what happened when we measured the Wigner function. It is different from a screen in front of the SG.
As i read again these lines, i am no more sure that they are different. When one gets a tomogram of the density matrix he has to measure quadratures and for each of them he gets random outputs just like with a screen.
Bhobba wrote that measurement (with its random output) occurs when decoherence is done. I see it from the other side: Decoherence is done when measurements occured.
 
  • #17
Demystifier said:
To have a decoherence-like interaction, you need interaction with a large number of degrees of freedom. If the particle (assumed to be an elementary particle or a particle with a very simple structure) and the emitted photon do not interact with the environment, nothing like decoherence will happen. The process of emission will be continuous and unitary, nothing like a quantum jump will occur. The quantum jump requires environment with many degrees of freedom. The environment may be external (e.g. surrounding gas or measuring apparatus) or internal (a complex emitting particle).

The same is true when emission is replaced by absorption.
Well, decoherence is very efficient (to the dismay of quantum-computer afficionados). It was demonstrated by Zeilinger at all doing double-slit/grating experiments with Bucky balls that the emission of a few black-body photons is sufficient to make the interference go away

http://arxiv.org/abs/quant-ph/0402146
 
  • #18
Demystifier said:
If [...] the emitted photons do not interact with the environment
This is nearly impossible, unless the experiment is done in outer space and the photon escapes into the vacuum, to be absorbed only by a very distant star (which can be ignored due to the finite speed of light).
 
  • #19
You see that a few photons caused the (first step of) decoherence when you look at the interferences.
You need then a macroscopic device.
Demystifier answered to my question about absorbed photons, that to know if the photons were absorbed you had to measure the atom with a macroscopic device. without that decoherence is reversible.
 
Last edited:
  • #20
Where do you need a macroscopic device? Of course, to measure the buckyballs you need a detector. The decoherence through the random emission of thermal photons is not a macroscopic process. The interesting thing about the buckyballs is that they are "mesoscopic", i.e., with 60 or 70 atoms in a molecule they have on the one hand a lot of degrees of freedom and a quasi-continuous energy spectrum, being in this sense on the edge of becoming "macroscopic" objects. On the other hand they are not that large that you can't control them. So you can cool them down so much that they show quantum-mechanical coherence effects in their passage through gratings. Heating them up in a controlled way these interference effects cease more and more the more thermal photons are emitted. That's the demonstration of decoherence and gradual loss of quantum behavior in a pretty well managable system!
 
  • #21
I am afraid that you anwer about another topic. What i said is about the irreversibility of decoherence. Everybody agree that decoherence is a measurable time evolving process.
Is there some thing in your book about possible reversibility of decoherence?
Read my post 16.
You wrote "of course you need a detector..."
This "of course" is the core of the problem.
 
  • #22
It doesn't matter whether you detect the radiated photons or not. The decoherence is due to the electromagnetic interaction of the charges making up the buckyball and the electromagnetic (quantum) field, leading to the emission of photons. Thus, the buckyball is coupled to the "environment", i.e., the electromagnetic field, and this leads to decoherence. Only the groundstate of the buckyball is strictly stable, i.e., no photons can be emitted due to energy conservation. Decoherence has nothing to do with the observation of the photons. Particularly you don't need a "conscious being" to take note of the results of measurements to cause decoherence.
 
  • #23
One more time you did not read post 16.
I talked about the electron in the SG. (the equivalent of you buckyball).
The electron decoheres in the magnetic field. WE AGREE.
You refuse to talk about what occurs after.
If the electron is not detected by a macroscopic screen or a detector, there is a possibility for recoherence.
When you have a decaying atom things only get irreversible decoherence if you measure the atom OR the decay product with a macroscopic device. Here you only talk about one of the two things.
 
  • #24
vanhees71 said:
Well, decoherence is very efficient (to the dismay of quantum-computer afficionados). It was demonstrated by Zeilinger at all doing double-slit/grating experiments with Bucky balls that the emission of a few black-body photons is sufficient to make the interference go away

http://arxiv.org/abs/quant-ph/0402146
Note that Zeilinger et al talk about complex molecules, while my statement contains an explicit note that it refers to particles with a very simple structure.
 
  • #25
naima said:
One more time you did not read post 16.
I talked about the electron in the SG. (the equivalent of you buckyball).
The electron decoheres in the magnetic field. WE AGREE.
You refuse to talk about what occurs after.
If the electron is not detected by a macroscopic screen or a detector, there is a possibility for recoherence.
When you have a decaying atom things only get irreversible decoherence if you measure the atom OR the decay product with a macroscopic device. Here you only talk about one of the two things.
Why should in a SG apparatus something decohere as long as there's no interaction of the electron with "the environment" (let's ignore that a SG experiment with a charged particle is very difficult if not impossible)? Just running through an external field doesn't decohere anything. There the time evolution is described by a unitary time evolution of the single electron. The SG apparatus doesn't lead to decoherence but to an entanglement between position and spin-projection.
 
  • #26
vanhees71 said:
Why should in a SG apparatus something decohere as long as there's no interaction of the electron with "the environment"?
Because the SG apparatus itself counts as environment. The SG apparatus is a macroscopic device, so most fine degrees of freedom of it cannot be controlled or monitored. Hence decoherence!

vanhees71 said:
The SG apparatus doesn't lead to decoherence but to an entanglement between position and spin-projection.
The SG apparatus leads to both. Let me also remind you that decoherence always involves entanglement.
 
  • #27
A single particle moving in a (inhomogeneous) magnetic field is described by a unitary time evolution (in the non-relativistic approximation). So no decoherence occurs in the usual setup of (idealized) SG experiments before the particle hits the screen, where it is registered.
 
  • #28
vanhees71 said:
A single particle moving in a (inhomogeneous) magnetic field is described by a unitary time evolution (in the non-relativistic approximation). So no decoherence occurs in the usual setup of (idealized) SG experiments before the particle hits the screen, where it is registered.
Yes, but I consider the screen to be a part of the SG apparatus. Otherwise, you are fully right.
 
  • #30
In which book? I've nothing about decoherence in my manuscripts. Concerning decoherence in the SG experiment in the above quoted preprint they write already in the abstract

"We include the interaction with the environment, as described by the Caldeira-Leggett model."

Then of course you have decoherence. No surprise!
 
  • #31
vanhees71 said:
So no decoherence occurs in the usual setup of (idealized) SG experiments before the particle hits the screen.
vanhees71 said:
Then of course you have decoherence. No surprise!

It is hard to follow you. Are you saying that here we have not an idealized SG device?
 
  • #32
Of course not. That's taking into account the rest gas in the vacuum tube. Then of course you have decoherence.
 
  • Like
Likes naima
  • #33
Thanks for this explanation.
We have 4 types of freedom degrees:
spin and position of the particle.
those of the air and of the magnetic field.
Suppose there is no gaz.
is there still entanglement of the 3 remaining degres and is there decoherence when we trace out the magnetic field?
 
  • #34
I don't know what you mean to "trace out the magnetic field". The magnetic field is at the heart of the whole experiment, no matter whether you take into account the interaction with the rest gas (air) in the vacuum tube or not.
 
  • #35
I trace out the magnetic field when i take the partial trace on its degrees of liberty. We then get the density matrix of the particle in the spin and position basis.
It is the usual thing. And i suppose there is no gas.
 
Last edited:
  • #36
No, the usual description is that of an atom moving in an external magnetic field, i.e., a one-particle description. If you assume that there is no gas, then there is no decoherence but unitary time evolution of the single-particle state only. For a complete treatment, see

http://arxiv.org/abs/quant-ph/0409206
 
  • #37
"We know that spin coherence is lost as the state evolves in time and the two spatial parts become orthogonal. Since the measurement process naturally invokes the partial trace over the spatial part of the initially pure global state the remaining spin part becomes a mixture." (Amir Caldeira)
in http://arxiv.org/abs/quant-ph/0608192
Caldeira adds at the end that
"Recovery of coherence should be achieved simply by recombining the two beams"

That is what i said: coherence is fragile when not measured by a macroscopic device (the magnet measures nothing)
 
Last edited:
  • #38
I don't agree with the authors that this is "decoherence" in the usual sense. If you trace out the position information, of course you end up with a mixed state, but that's not decoherence, which is due to interaction of the quantum system with "the environment" (which can be among other sense also the measurement apparatus).
 
  • #39
When we measure a spin with a SG the only thing which matters here is the density matrix in the up down basis. And it is not pure.
 
  • #40
This has nothing to do with decoherence!
 
  • #41
There are several ways to measure entanglement. We can use Neumann's entropy. We can say that there is entanglement if the states are not separable (yes/no answer). There is also linear entropy.
We have an analog thing with decoherence.
Let us us take a two level state. When it is pure its entropy is null and and when it has decohered its entropy may be equal one bit.
In all cases we vave in its density matrix 2 null off diagonal terms.
We usually say then that decoherence is done.
This is a yes/no characteristic.
As the particle was entangled we can consider the global Hilbert space of all the degrees of freedom. Caldeira ended its paper by saying that coherence can be recovered simply by merging the beams of the SG apparatus. Here the spin of the particle was coupled with its z position. The coherence is fragile because we have only to act on one degree to erase the decoherence.
We see that in addition to the nullity of the off diagonal terms, there is another quantity which measures the easiness to recohere. It is the dimension of the global hilbert space (minus 2 here). If it is high we would have to manage numerous parameters to get recoherence and spontaneous recoherence is highly improbable. Robustness of decoherence only appears when macroscopic internal or external numbers of degrees of freedom come into play.
Measurement cannot give outputs if decoherence was done but fragile. That is why you need a screen in front of rhe SG.
 
  • #42
There is another way to say that:
In the SG with no gas the spin decoheres. it is in an improper mixed state. one does not see the outcome. If the particle enters a bubble chamber, its spin density matrix remains unchanged but we see the result. coherence cannot reappear. In this second period the particle is entangled with the gas environment. The mixed state begins to be a statistical (proper) mixture of results and one is observed. Proper and improper mixtures have the same matrix but are physically different. the particle evolves here from an improper to a proper mixture state. There is no collapse. Only a statistical mixture at the end.
Zurek gives a time coefficient Zu(t) which enable to describe the state as
(1 - Zu(t)) (improper) + Zu(t) (proper).
Another related point of view: http://arxiv.org/abs/0901.0795
 
Last edited:
  • #43
Again: If there is no gas and thus the system closed, i.e., a single particle moving in a magnetic field, nothing decoheres. The time evolution is entirely unitary. There cannot be decoherence with a unitary time evolution. That's behind the socalled "measurement problem", discussed vigorously in this forum (forgetting the physics over the philosophy unfortunately ;-)).
 
  • #44
vanhees71 said:
I don't agree with the authors that this is "decoherence" in the usual sense.
You already said that you disagree with the co-author of the Caldeira-Leggett model. Who is mainstream? You or Caldeira?
Caldeira himself says that something differs from the usual sense. It is not decoherence but the notion of environment. Here we have not a particle which decoheres while interacting with other particles but a degree of feedom entangling with other degrees of freedom.
I notice that the other usual forumers are very cautious and silent.
 
Last edited:
Back
Top