I am thinking here of how creation vs. absorption compare for a photon. A single photon may be emitted when an electron in an atom returns down to the ground state from an excited state. In a reciprocal event, such a photon could be subsequently absorbed by a similar atom causing an electron to jump from the ground state up to the excited state.

A single photon has a wavefunction associated with it. In the case of emission, the wavefunction suddenly appears in the vicinity of the atom and then radiates out from that source. In the case of absorption, the wavefunction may be initially present over a large volume but is said to suddenly disappear (collapse) at the instant the atom gets excited. Both these events are probabilistic and follow the rules of quantum mechanics.

In most cases, physics runs equally well forwards or backwards. Presumably this applies to the emission of a photon by one atom and its absorption by a nearby atom. However the wavefunction description of this process is dramatically asymmetric in time. If I try to run it backwards, I see a wavefunction that abruptly appears in a large volume around one atom and then magically converges towards the other and disappears.

Maybe is just part of the mystery, but is there no quantum-mechanical description of such an event where the description itself has time-symmetry?

Quantum-mechanical example with spatial and time symmetry:
For what it's worth, the following picture shows a perfect ellipsoidal cavity with two atoms - one at each focus. This is a pathological case, but it does seem like the transfer of the excited state from one atom to the other would involve a time-symmetric evolution of the wave function.
ellipsoidal cavity with two atoms
An experiment starts by initiating the states of the two atoms and the experiment concludes by measuring the states of the two atoms. In reverse time, do processes of initiating and measuring simply reverse roles but are otherwise identical?

symmetry between initialization and measurement?

  • $\begingroup$ The wavefunction doesn't collapse in the moment the photon is absorbed by the atom, but in the moment you measure the atom to be excited. $\endgroup$ – A. P. Mar 1 at 9:30
  • $\begingroup$ In the case of emission, the wavefunction suddenly appears in the vicinity of the atom and then radiates out from that source. Who told you that? $\endgroup$ – Gert Mar 1 at 10:15
  • $\begingroup$ @Gert please correct me regarding 'emission' $\endgroup$ – Roger Wood Mar 1 at 19:17
  • $\begingroup$ @RogerWood The Time Dependent SE describes these transitions from, say $\psi_1$ to $\psi_2$. The wave function as you understand it here is for stationary states only. $\endgroup$ – Gert Mar 1 at 20:53
  • $\begingroup$ @RogerWood en.wikipedia.org/wiki/… $\endgroup$ – Gert Mar 1 at 20:56

Emission and absorption of a photon aren't instantaneous processes as long as you don't perturb the system by measuring its state. If you do, the system collapses in a non-reversible way. Let me explain how it evolves in the case you don't measure:

Spontaneous emission

An atom in the excited state $| a \rangle$ emits light in the same spatial pattern as a classical dipole antenna:

As you correctly state in your question the emission starts out from the position of the atom and moves away from it at the speed of light. Similar to an antenna which is not damped by electrical resistance, but only by the energy it loses due to radiation, the power it emits decays over time. For the case of the atom the state $| a, 0 \rangle$ in which the atom is in the excited state and there is no photon present evolves towards the state in which the atom is in the ground state $| b \rangle$ and there is a photon in a superposition of many modes with different wavevectors $\vec{k}$. This happens smoothly: $$ | \psi (t) \rangle = c_a (t) \, | a, 0 \rangle + \sum_{\vec{k}} c_{b, \vec{k}} (t) \, | b, 1_{\vec{k}} \rangle $$ The temporal evolution is exponential, i.e. $\left| c_a (t) \right|^2 = e^{- \Gamma t}$, so that after infinite time the atom is completely in the ground state and the photon is completely emitted. For a more rigorous description see the Wigner-Weisskopf theory as described for example in Scully & Zubairy – Quantum Optics (1997) chapter 6.3.

Time-reversed spontaneous emission

All of the described evolution happens unitarily, hence it can happen backwards as well as forwards. If you have an atom in the ground state and prepare a photon in a spatial mode matching the emission pattern of the atom having the right temporal profile you can deterministically drive the atom into the excited state. This is described in Stobińska et al. EPL 86 (2009). It is of course very difficult to do, because you need to focus the light from the full $4 \pi$ solid angle onto the atom and find a way to shape the photon to an exponentially rising wavepacket.

Absorption of a spread-out photon

Coming back to the apparent paradox of your question: If the wavefunction of a photon is extended over a large area how does it excite the atom as if it was localized there? The answer is "It doesn't.". Like in the case of spontaneous emission the state of the overall system evolves in a superposition of the atom being in the ground state / the photon flying around and the atom being excited by the photon. Just that in the case of a photon not matching the spatio-temporal radiation pattern of the atom the probability of the atom being excited $\left| c_a (t) \right|^2$ is very low. So the majority of the wavefunction still describes a free-flying photon.

Only when you measure the state of the atom (or the presence of the photon) you force the system to be in either of the states. This is the moment when the whole spread-out photon collapses to be either absorbed or detected somewhere on a camera. The whole mystery is in the description of collapse due to measurement. But this is another topic, covered in questions like "Practically, how does an 'observer' collapse a wave function?".

Is the absorption also a measurement?

There is a connection between the (partial) absorption of the photon and a projective measurement. By their interaction the atom and the photon become entangled, just like in more advanced collapse models the detector becomes entangled with the observed system. As an example consider an animal-friendly version of Schrödinger's cat: A radioactive atom, which can trigger a detector and an experimentalist monitoring the detector. If the atom was alone it would evolve into a superposition of decayed and not decayed $$ | \psi_{\text{atom}} \rangle = \alpha | \text{decayed} \rangle + \beta | \text{not decayed} \rangle \text{.} $$ If you include the detector into the Hilbert space you can model the system of detector plus atom as an entangled state $$ | \psi_{\text{atom + detector}} \rangle = \alpha | \text{decayed} \rangle | \text{triggered} \rangle + \beta | \text{not decayed} \rangle | \text{not triggered} \rangle \text{.} $$ Involving the experimentalist as well then yields the state $$ \begin{align} |\psi_{\text{atom + detector + experimentalist}} \rangle = \quad &\alpha | \text{decayed} \rangle | \text{triggered} \rangle | \text{decay observed} \rangle \\ + &\beta | \text{not decayed} \rangle | \text{not triggered} \rangle | \text{no decay observed} \rangle \text{.} \end{align} $$ Because the experimentalist is part of the superposition, in each branch of the wavefunction it appears to the experimentalist as if the atom is now in a definite state – as if it had collapsed from the initial superposition.

So in the end the distinction between the atom and a macroscopic detector is artificial. But it's justified, because the atom can be coherently manipulated to unentangle it from the photon. For macroscopic systems like the detector (and experimentalist) this is pretty hopeless because they have too many degrees of freedom.

Absorption of a focused photon

In the case of the elliptic cavity the emission of atom $A$ is indeed reshaped to match the spatial emission pattern of atom $B$. Despite this the probability that atom $B$ absorbs the photon is still less than $1$, because the temporal profile of the emitted photon is exponentially decaying, while perfect absorption (time-reversed spontaneous emission) requires an exponentially rising profile.

If the cavity size is reduced such that the emission of the photon takes significatly longer than a round-trip of in the cavity, the excitation being initially in atom $A$ can be fully transfered to atom $B$ and vice versa.

The following is a simulation starting in the state $$ | a_A \rangle | b_B \rangle | 0 \rangle \text{,} $$ i.e. atom $A$ in the excited state, $B$ in the ground state and $0$ photons in the cavity. The state evolves according to the Hamiltonian $$ \hat{H} = \hbar g \left( \hat{a} \left( \hat{\sigma}^+_A + \hat{\sigma}^+_B \right) + \hat{a}^\dagger \left( \hat{\sigma}^-_A + \hat{\sigma}^-_B \right) \right) $$ (sourcecode here).

As long as no projective measurement is performed the excitation is symmetrically exchanged back and forth between the two atoms.

  • $\begingroup$ That's certainly helpful. Let me digest what you are saying and the references. I'm worry that there's an inherent time-asymmetry in even trying to state the problem. We're talikng about a photon moving from one atom to another. There is a measurement afterwards, but is there also an implicit measurement beforehand? It seems like the source atom is assumed to be deterministic but the sink/target atom seems to be probabilistic. Can this be reversed so that we start with the assumption that the photon has been absorbed and ask about the probabilities of where it came from? $\endgroup$ – Roger Wood Mar 5 at 1:35
  • $\begingroup$ @RogerWood The evolution of the wavefunction is deterministic. It's the measurement, which has probabilistic outcomes. I've added another paragraph about whether the absorption itself is already a measurement (assuming that's what you mean by 'implicit measurement'). $\endgroup$ – A. P. Mar 5 at 12:49
  • $\begingroup$ @RogerWood With the other question, do you mean starting from the collapsed state in which the photon was absorbed and rewind the evolution from there? Or do you mean considering only the part of the wavefunction which led to an absorption and tracing back the evolution of the this part? $\endgroup$ – A. P. Mar 5 at 12:49
  • $\begingroup$ Your answer and comments are very helpful and make sense. I'm somehow still stuck on the apparent inherent time asymmetry, but I can't quite pin down the question to ask. I've added an edit to my question that focusses on the idea that there should be some equivalence between the initiation of experiment and the measurement of the outcome. $\endgroup$ – Roger Wood Mar 6 at 0:50
  • $\begingroup$ @RogerWood The only thing which takes away the symmetry is the measurement. Everything else evolves unitarily and therefore in principle reversible. I've added a description of the case with the elliptic mirrors. $\endgroup$ – A. P. Mar 6 at 17:55

Firstly a remark about the termonology: Wave functions do not appear or disappear - that would contradict conservation of charge, probability, etc. What changes is the state of the system.

Wave function collapse refers to the localization of the system in an eigenstate of the measurement operator due to the interaction with a macroscopic object. Measurement operator in this case is the interaction operator between the quantum and the macroscopic systems. The macroscopic system is often called "observer", which is a misleading term, as it implies some consciousness on the part of this system, while all that matters is that it has a very large number of degrees of freedom - i.e., it can be considered in classical limit, which often implies the thermodynamic limit. These properties of the macroscopic object make the wave function collapse irreversible - in the sense that teh return to the initial state is improbable (with thermodynamically vanishing probability).

This process has been studied in many other contexts under the name of decoherence, where a system is couple to a bath with infinitely many degrees of freedom (typically modeled as a collection of many harmonic oscillators), which can be considered to be in thermodynamic state, etc. - Hopefully you see the similarity. Caldeira-Legget model, reduced density matrix, quantum kinetic equation - these are all the terms coming from this field.

Electromagnetic vacuum is one example of such a bath - the spontaneous emission can be considered an irreversible process with teh atom becoming localized in its ground state. Such a view however is applicable only when the electromagnetic vacuum satisfies the conditions of being a macroscopic object, outlined above. Thus, if we are dealing with an atom in a cavity, coupled to a few long-living photon modes, the atom will emit and reabsorb the photons, since they do not get thermalized (another way of saying that in this case photon field has a limited number of degrees of freedom and is not in a thermodynamic equilibrium). In Jaynes-Cummings model this is known as wave function collapse and revival (a rather suggestive language in our context).

Absorption of a photon can be similarly associated with a wave function collapse, if the atom "forgets" how it got excited. It is a bit more complicated in this case to define which part of the EM field serves as a bath.

Finally, note two different mathematical formalisms are frequently used for the situations where the collapse occurs and does not in absorption: Fermi golden rule and Rabi oscillations respectively.

Disclaimer I have avoided writing any equations, since most fo them would be necessarily reproducing the admirably detailed answer by @A.P.

  • $\begingroup$ Thanks, I still find some of these concepts quite difficult to grasp. The way you are describing the collapse or decoherence sounds a lot like the 2nd law of thermodynamics. We have set up a special contrived state which naturally evolves (collapses?) into a typically 'random' state. It's a 'random' state that still includes a particular macroscopic parameter we can observe, but it's random in the sense that there are so many other hidden parameters that we cannot expect it to reverse with any reasonable probability. $\endgroup$ – Roger Wood Mar 10 at 2:23
  • $\begingroup$ I am stretching the things a bit: in QM "observer" is an external non-quantum entity, "a microscopic object" - whatever it means. So when I am trying to describe it from the quantum mechanical point of view, as a "bath", I am using circular logic... but it seems to me as the only way to make sense of your question. In quantum measurement theory creating of a wave function is not defined - only its collapse. $\endgroup$ – Roger Vadim Mar 10 at 7:57
  • $\begingroup$ you state: "In quantum measurement theory creating of a wave function is not defined". This raises the more general question: "In quantum theory, is the creation of a wave function defined?" $\endgroup$ – Roger Wood Mar 12 at 2:56

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