Photon Size: Uncertainty Principle & QM Explained

[Maui]

There are no photons classically.

You could state the same of all elementary particles, that's why 'classically' was in quotes denoting that size seems to play a practical role(e.g. the example of light diffraction in optics).

 

[Dale]

You could state the same of all elementary particles, that's why 'classically' was in quotes denoting that size seems to play a practical role(e.g. the example of light diffraction in optics).

If a photon were a classical particle with some size then it wouldn't diffract at all.

 

[Maui]

If a photon were a classical particle with some size then it wouldn't diffract at all.

I agree but I didn't say a photon was a classical particle. Only that in some practical respects photon's wavelength attributes a physical size that appears to be a limit in photography and optics in general(microscopes, etc.).

 

[vanhees71]

The question is, how to define the radius of an (elementary or composite) particle, atom, or molecule. In physics such quantities have to be defined as a measurable quantity. Usually one measures charge radii of the (sub)atomic object, usually by elastic scattering of electrons. Measuring the differential cross section as a function of the scattering angle gives the charge radius. Such experiments measure, the root-mean-square radius, which is defined as
r_{\text{ch}}^2=\langle r^2 \rangle_{\rho}=\frac{\int_{\mathbb{R}^3} \mathrm{d}^3 \vec{x} \; \vec{x}^2 \rho(\vec{x})}{\int_{\mathbb{R}^3} \mathrm{d}^3 \vec{x} \; \rho(\vec{x})},
where \rho is the charge distribution of the object.

For photons I'm not aware of any proper definition of its radius. It's anyway pretty wrong to assume that photons can be thought of as little classical particles at all! There's not even a well-defined position operator for a photon!

 

[Bill_K]

There's not even a well-defined position operator for a photon!

Yes, for sure that's the majority conclusion, but there seems to be some controversy remaining about it, and maybe the difficulty has been overstated. There's a candidate position operator that was found in 1948 by Pryce,

x ≡ i ∇_p + p x s/p²

where s is the photon's spin vector. The shocking thing about this x is that its three components don't commute,

[x_i, x_j] = -i ε_ijk p_k p·s/p³

Nevertheless, there's an argument by Mourad that this is not so bad. He says,

The three components of the Pryce operator cannot be simultaneously diagonalized, so that one cannot find states localized exactly at a given point in space. Newton and Wigner argued that this makes the photon non-localizable. However, we will show that although the commutator of the three components is non-vanishing, one can find states which are ”localized" within an arbitrarily small region.

 

[sophiecentaur]

I agree but I didn't say a photon was a classical particle. Only that in some practical respects photon's wavelength attributes a physical size that appears to be a limit in photography and optics in general(microscopes, etc.).

Wavelength and size are not related. Diffraction calculations are based on an infinitely long wave train. The effect of one photon is just an individual occurrence. How can you say there is some sort of correspondence between the wavelength and any idea of 'size'? Any 'entity' that can have a 'single' wavelength needs to have infinite extent. An entity with very limited extent needs a very large range of associated wavelengths. That's the (Fourier) relationship between temporal and frequency domains (or the equivalent spatial thing), surely.

 

[Maui]

Wavelength and size are not related.Diffraction calculations are based on an infinitely long wave train. The effect of one photon is just an individual occurrence. How can you say there is some sort of correspondence between the wavelength and any idea of 'size'? Any 'entity' that can have a 'single' wavelength needs to have infinite extent. An entity with very limited extent needs a very large range of associated wavelengths. That's the (Fourier) relationship between temporal and frequency domains (or the equivalent spatial thing), surely.

Are you saying that a photon's wavelength has no associated width? How do you explain diffraction patterns below the 200 nm? It sounds like a contradiction to measure the practically measured wavelength of photons in nm and at the same consider the photon as not spatially extended.

After all the wavelength of photons is a real measureable phenomenon determining properties of the EM field(colors, visible light, etc.).

I was listening to a physics professor lecturing on QM and he raised the question "How big is a photon?" and indicated it had arisen during his PhD defense.

He than began to discuss the accurately known frequency and wavelength of a laser emitted photon (and thus accurately known momentum) in the context of the uncertainty principle.

It seems most physicists think of photons as part of the EM field which is of infinite extent and 'photons' with definite and detectable properties as excitations of that field upon measurement.

 

[sophiecentaur]

Are you saying that a photon's wavelength has no associated width? How do you explain diffraction patterns below the 200 nm? It sounds like a contradiction to measure the practically measured wavelength of photons in nm and at the same consider the photon as not spatially extended.

After all the wavelength of photons is a real measureable phenomenon determining properties of the EM field(colors, visible light, etc.).

It seems most physicists think of photons as part of the EM field which is of infinite extent and 'photons' with definite and detectable properties as excitations of that field upon measurement.

You need to go back to elementary diffraction theory and see what it is really saying. There is nothing to do with 'width' of the waves in the calculation of the interference between two slits. The pattern is related to the spacing of the slits and the wavelength (longitudinal variation). There is nothing 'special' about the wavelength of 200nm; the same theory applies to 200km or 2nm. The 'lateral extent' of a photon, as a concept, is meaningless because there is a probability that it can be measured over the whole area of a 100m sphere after it has 'travelled' for just 300ns from a point source. This is true for whatever wavelength of EM we are considering.

When talking about the interaction with matter, it is more precise to talk in terms of frequency. The energy of a photon is normally given by E =hf, with good reason. The wavelength, locally, is not actually going to be the same as the free space wavelength because, by definition, the photon is not interacting in free space but in the presence of matter. The frequency is going to be unchanged but what actual value of wavelength can you give your photon? (certainly not c/f)

 

[Maui]

There is nothing 'special' about the wavelength of 200nm; the same theory applies to 200km or 2nm. The 'lateral extent' of a photon, as a concept, is meaningless because there is a probability that it can be measured over the whole area of a 100m sphere after it has 'travelled' for just 300ns from a point source. This is true for whatever wavelength of EM we are considering.

But in practice there is something special in that photons at 200 nm are already in the UV portion of the EM field. Ordinary light microscopes hit the diffraction limit of visible light just above the 200 nm limit or at 1 PHz. AFAIK 200-300 nm is exactly the diffraction limit of visible light.

What you seem to be talking about is the probability amplitude of finding an electron which is different from photons wavelength. Or are you saying they are related?

When talking about the interaction with matter, it is more precise to talk in terms of frequency. The energy of a photon is normally given by E =hf, with good reason. The wavelength, locally, is not actually going to be the same as the free space wavelength because, by definition, the photon is not interacting in free space but in the presence of matter. The frequency is going to be unchanged but what actual value of wavelength can you give your photon? (certainly not c/f)

This seems to imply that my impression was correct in stating that -

It seems most physicists think of photons as part of the EM field which is of infinite extent and 'photons' with definite and detectable properties as excitations of that field upon measurement.

 

[Cthugha]

In fact already Maxwell's equations allow for highly localized solutions in free space. Phys. Rev. Lett. 88, 100402 (2002) cites some of them and states that "Remarkably, in contrast to the conclusions reached in previous studies, localization need not be related to photon wavelength nor necessarily associated with a wavelength-scale spatial range."

Getting away from the "size" concept, there are for sure several characteristic length scales of light fields. We have at least the wavelength, the coherence length, a decay length of the electric field/intensity, a decay length of the energy density and a decay length of the detection probability. While in simple cases several of these characteristic length scales will coincide, already the not that complicated case of non-monochromatic single photons leads to strange results like the maximum of the energy density being somewhere else than the highest detection probability and both scaling very differently. The Mandel/Wolf has a chapter on that topic (12.11 in my edition).

So is one of these length scales "better" as a size than the others? I do not think so. These different concepts of length scales exist separately for a good reason.

 

[sophiecentaur]

But in practice there is something special in that photons at 200 nm are already in the UV portion of the EM field. Ordinary light microscopes hit the diffraction limit of visible light just above the 200 nm limit or at 1 PHz. AFAIK 200-300 nm is exactly the diffraction limit of visible light.

What you seem to be talking about is the probability amplitude of finding an electron which is different from photons wavelength. Or are you saying they are related?

This seems to imply that my impression was correct in stating that -

Different parts of the Em spectrum(you mean?) will diffract differently for a given obstruction, of course; their wavelengths are different and so the structure is a different size in wavelengths. Also, the energy of the photons will be different so the effect of the material may be different (absorption / refractive index etc.) . But what has that got to do with the Quote "Width".

When I use the term probability, I mean that the classical optics of diffraction (the pattern) give the probability that photons will be detected in different locations (the light and dark areas). But this has nothing to do with the 'size' of the photon.
Try reading Cthugha's last post if you want to go further than the elementary level.

 

[Maui]

Different parts of the Em spectrum(you mean?) will diffract differently for a given obstruction, of course; their wavelengths are different and so the structure is a different size in wavelengths. Also, the energy of the photons will be different so the effect of the material may be different (absorption / refractive index etc.) . But what has that got to do with the Quote "Width".

Length and width are dimensions and properties of size and volume. I don't see how Cthugha's post supports your evasive explanations so far. Certain wavelengths are diffracted by certain widths. What is there to explain?



What do you mean by 'structure of photons'? If they have a structure and based on this structure they are diffracted below a certain limit(measured in nm as are all spatially extended objects), how is that not a practical limit for photons of visible light?

 

[sophiecentaur]

Length and width are dimensions and properties of size and volume. I don't see how Cthugha's post supports your evasive explanations so far. Certain wavelengths are diffracted by certain widths. What is there to explain?



What do you mean by 'structure of photons'? If they have a structure and based on this structure they are diffracted below a certain limit(measured in nm as are all spatially extended objects), how is that not a practical limit for photons of visible light?

Chuga's post is at a much higher level than what we are discussing. I am pointing out that your ideas are not (even) consistent with elementary ideas about diffraction. (The specifically 200nm bit is a total red herring, for instance as it rerfers to one particular circumstance. As I said, diffraction occurs at all wavelengths). It is you who are suggesting (by implication) a structure for a photon. Follow up on what Chuga's references if you want to talk about 'extent'; it certainly has nothing to do with any ideas of "width" of a photon to explain diffraction. You are trying to over simplify things. I am being evasive, if you like, because all I can do is to point out the inconsistencies of what you are saying. If you cannot see that then how can you move on to the more meaty stuff that Chuga and others are writing about?

 

[Maui]

Chuga's post is at a much higher level than what we are discussing. I am pointing out that your ideas are not (even) consistent with elementary ideas about diffraction. (The specifically 200nm bit is a total red herring, for instance as it rerfers to one particular circumstance. As I said, diffraction occurs at all wavelengths).

Yes, it occurs at all wavelengths and I never ever questioned that(I wonder why you mention it at all). I did say the plain obvious though - diffracton occurs at all wavelengths at specific slit widths corresponding to light's wavelength.

It is you who are suggesting (by implication) a structure for a photon. Follow up on what Chuga's references if you want to talk about 'extent'; it certainly has nothing to do with any ideas of "width" of a photon to explain diffraction. You are trying to over simplify things. I am being evasive, if you like, because all I can do is to point out the inconsistencies of what you are saying. If you cannot see that then how can you move on to the more meaty stuff that Chuga and others are writing about?

I see no coherent statement in Cthugha's on the relationship between a photon's lack of spatial extension and its practical wavelength implications -- he admits there are different scales of length all valid for photons(if I understood correctly). I have stumbled upon similar discussions in the past and they end inconclusively which seems to highlight that quantum theory is obviously neither perfect nor complete theory and a more fundamental theory would better explain photon behavior and have fewer conceptual issues(which all seem to spring from attempts at realism in the micro realm). That's hardly surprising given that the person who discovered the duality of photons said the following:


"All the fifty years of conscious brooding have brought me no closer to answer the question, “What are light quanta?” Of course today every rascal thinks he knows the answer, but he is deluding himself" - AE

 

[sophiecentaur]

I am beginning to see part of your problem here. Diffraction occurs for all wavelengths and with all sizes of obstacles. There is always a pattern (never an abrupt transition) whichever combination you choose; truncation in space will result in a variation in the amplitude of the beam (Fourier). You seem to be claiming otherwise. This is in a classical context but you really should clear that up first.
I also repeat my earlier question which is - where does the "width" of the photon, to which you referred earlier, come into the formation of a diffraction pattern? Can we please clear this up before moving on?

You see, I have never read anything of substance that suggests that the extent / width / length of a photon has any real meaning. It has either zero size or unbounded extent, depending on where you are considering it. Nowhere have I found anyone who shows it has a particular 'size', related to its wavelength.

However clever Albert was, he died a long time ago and things have actually moved on a bit since his time. He was very right about many things but that is as far as it goes. He was fallible (and treated his wife very badly, I believe.)

 

[Cthugha]

It seems most physicists think of photons as part of the EM field which is of infinite extent and 'photons' with definite and detectable properties as excitations of that field upon measurement.

The meaning of the term 'photon' has unfortunately undergone several changes over the decades and the same term has been used for two rather different concepts which is unfortunate.
In the old days of QM, Dirac and others used the term photon for the modes you get in a spectral decomposition of the light field into monochromatic modes with discrete occupation number and fixed energy (and thus of course infinite extent in time). With the arrival of quantum optics in the sixties, a photon rather is an eigenstate of the photon number operator. That means pretty much every state which contains EXACTLY one photon (or one photon per pulse for pulsed light). These can be polychromatic and have pretty much any spatial and temporal shape. Two very different concepts, but unfortunately a single name. The first concept is a useful tool for theorists (but not a state actually realized due to the infinite extent). The second concept is what people actually realize in the lab when they speak of single photon states.

Yes, it occurs at all wavelengths and I never ever questioned that(I wonder why you mention it at all). I did say the plain obvious though - diffracton occurs at all wavelengths at specific slit widths corresponding to light's wavelength.

The problem I see with trying to attribute the diffraction limit to a property of photons is that the diffraction limit is usually rather considered to be a description of the imaging system used. It gives the minimum diameter of an Airy disk in imaging which is the wavelength divided by two times the numerical aperture of the system, where the latter depends on the refractive index of the material and the focusing angle with an optimal value of roughly lambda/2.7 to lambda/2.9 (which roughly gives the mentioned 150-200 nm). However, there are several material and design parameters entering here. Even further, the diffraction limit applies to a certain imaging technique: confocal microscopy. You can easily get better resolution by going to a 4 pi microscope. Alternatively, one can also use STED microscopy or go to near field techniques like total internal reflection microscopy to get sub-wavelength resolution. Each technique gives its own limit.

Also, one can use interferometric techniques and show that for some states - even classical ones - several photons can be way better localized than one photon alone (see e.g. Phys. Rev. A 70, 041801(R) (2004), "Subwavelength coincidence interference with classical thermal light"). In a nutshell, the point I tried to make is that there are many different types of states of the light field and while it might seem attractive to connect some characteristic length scales (like wavelength) of the field with some "true" spatial extent for some special states, it usually does not work out in the general case.