I recently realized I can't give a good answer to the seemingly simple question "how big is a photon?" so I did some reading on the subject and the short answer I can now come up with is "that depends". The slightly longer answer is it depends on how the photon is produced and what you mean by “size.” In one sense photons are elementary particles with no evidence of internal structure: scattering experiments show they have no parts. When a photon strikes a photographic plate it produces a localized point, not a smear, and there is no sign of matter interacting with one portion of a photon before another. Photons are also massless and electrically neutral, so they do not have a rigid physical boundary that could be measured like the surface of a ball.
But on the other hand red light has a wavelength of about 650 nanometers, so does that mean a red photon is 650 nanometers across? No, because Heisenberg's Uncertainty Principle must be taken into account. Wavelength tells us the spacing of the crests of the underlying electromagnetic wave, not how long a single photon is in space. The actual spatial extent of a photon depends on its coherence length, that is to say the distance over which its wave-like oscillations remain well defined. And coherence length = c × coherence time = c/(2πΔf).
So coherence length is tied to Heisenberg’s Uncertainty Principle: ΔE × Δt ≳ ℏ/2. A photon that is emitted over a short time interval (Δt is small) has a large uncertainty in energy (ΔE is large), which translates into a broad frequency spread and therefore a short coherence length. But if the emission lasts a long time then the frequency uncertainty is small and the photon can stretch out over a very long distance. The way the photon is produced can make a big difference.
A red photon from even a cheap laser diode has an extremely narrow frequency spread giving it a very long coherence length, several meters, and for high-quality lasers it can be several miles. By contrast, a red photon emitted from blackbody radiation, like the glow from an incandescent bulb, has a broad frequency spread, and therefore a very short coherence length, about the width of a human hair. In both cases the photons are indivisible quanta, but their wave packets have very different spatial extents.
So the “size” of a photon cannot be pinned down to a single number. In interactions, it behaves as if it has no size at all, striking at a point. But in terms of its wave-like character, it can extend over hundreds of nanometers in wavelength and, depending on how it is produced, anywhere from a fraction of a micrometer to many miles in coherence length. A photon is therefore not like a little ball of light with a fixed diameter, it's more useful to be thought of as a quantum excitation of the electromagnetic field that travels like a wave but interacts with matter like a particle, and whose spatial extent depends on both the uncertainty principle and the circumstances of its creation.
John K Clark See what's on my new list at Extropolis
bph
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Thanks for the exposition.
Brent
On Tuesday, September 2, 2025 at 2:16:15 PM UTC-6 Brent Meeker wrote:
>>Thanks for the exposition.
Brent>But you, being the expert you are, already "knew" the answer. It had to do with the wf of a photon. But oddly, you haven't a clue what differential equation would have to be solved to obtain that wf. WTF. AG
In the two-slit experiment, if you quantize the electromagnetic field, the field amplitude takes on the role of a photon’s probability amplitude. That amplitude behaves like a wave, so it interferes, and the squared magnitude (|E|^2) gives the probability distribution for where a photon is likely to be detected on the screen. If you send photons one at a time, each detection looks random, but over many trials the hits build up exactly into the interference pattern predicted by |E|^2.
When you use a bright source, such as a laser, you no longer just have a single photon but a huge number of them, so |E|^2 doesn’t just describe a probability distribution, it gives the average number of photons arriving at each point. And as the number of photons increases classical optics approximates quantum mechanics more and more closely.
John K Clark See what's on my new list at Extropolis
tvi
On Tue, Sep 2, 2025 at 6:05 PM Alan Grayson <agrays...@gmail.com> wrote:On Tuesday, September 2, 2025 at 2:16:15 PM UTC-6 Brent Meeker wrote:>>Thanks for the exposition.
Brent>But you, being the expert you are, already "knew" the answer. It had to do with the wf of a photon. But oddly, you haven't a clue what differential equation would have to be solved to obtain that wf. WTF. AGAs seen below, the electromagnetic wave function is described by 4 differential equations discovered by James Maxwell about 10 years before Einstein was born :Gauss's Law for Electricity: ∇ ⋅ E = ρ / ε₀
Gauss's Law for Magnetism: ∇ ⋅ B = 0
Faraday's Law of Induction: ∇ × E = -∂B/∂t
Ampère's Law ∇ × B = μ₀J + μ₀ε₀∂E/∂tTo this day those equations are the bread and butter of electrical engineers, they don't include any of the quantum properties of light but they don't need to in order to explain the Doppler red shift. If you want to find the quantum wave function, and not just the electromagnetic wave function, and also include relativistic effects, then things become a little more complicated.In the two-slit experiment, if you quantize the electromagnetic field, the field amplitude takes on the role of a photon’s probability amplitude. That amplitude behaves like a wave, so it interferes, and the squared magnitude (|E|^2) gives the probability distribution for where a photon is likely to be detected on the screen.
On Wednesday, September 3, 2025 at 6:05:55 AM UTC-6 John Clark wrote:On Tue, Sep 2, 2025 at 6:05 PM Alan Grayson <agrays...@gmail.com> wrote:On Tuesday, September 2, 2025 at 2:16:15 PM UTC-6 Brent Meeker wrote:>>Thanks for the exposition.
Brent>But you, being the expert you are, already "knew" the answer. It had to do with the wf of a photon. But oddly, you haven't a clue what differential equation would have to be solved to obtain that wf. WTF. AGAs seen below, the electromagnetic wave function is described by 4 differential equations discovered by James Maxwell about 10 years before Einstein was born :Gauss's Law for Electricity: ∇ ⋅ E = ρ / ε₀
Gauss's Law for Magnetism: ∇ ⋅ B = 0
Faraday's Law of Induction: ∇ × E = -∂B/∂t
Ampère's Law ∇ × B = μ₀J + μ₀ε₀∂E/∂tTo this day those equations are the bread and butter of electrical engineers, they don't include any of the quantum properties of light but they don't need to in order to explain the Doppler red shift. If you want to find the quantum wave function, and not just the electromagnetic wave function, and also include relativistic effects, then things become a little more complicated.In the two-slit experiment, if you quantize the electromagnetic field, the field amplitude takes on the role of a photon’s probability amplitude. That amplitude behaves like a wave, so it interferes, and the squared magnitude (|E|^2) gives the probability distribution for where a photon is likely to be detected on the screen.
How can the amplitude give a probability if its value is generally not less than unity? AG
How can the amplitude give a probability if its value is generally not less than unity? AG
John K Clark See what's on my new list at Extropolis
kcj
On Wed, Sep 3, 2025 at 10:06 AM Alan Grayson <agrays...@gmail.com> wrote:How can the amplitude give a probability if its value is generally not less than unity? AG|E|^2 gives the relative probabilities of detecting a photon at different points on the screen, it gives you the correct curve shape but is not normalized so all the probabilities don't add up to exactly one. To make it a true probability distribution that integrates to 1 you divide |E|^2 by a constant, the total integrated intensity across the screen.
>> |E|^2 gives the relative probabilities of detecting a photon at different points on the screen, it gives you the correct curve shape but is not normalized so all the probabilities don't add up to exactly one. To make it a true probability distribution that integrates to 1 you divide |E|^2 by a constant, the total integrated intensity across the screen.> But this E is the classical energy, and when the EM field is quantized don't we need a huge number of photons to define the curve you reference above?
> Is there a differential equation that when solved, gives us the wf of a RELATIVISTIC particle?
> Is there an equation that gives the wf of a photon? TY, AG
John K Clark See what's on my new list at Extropolis
ijt
On Wed, Sep 3, 2025 at 6:53 PM Alan Grayson <agrays...@gmail.com> wrote:>> |E|^2 gives the relative probabilities of detecting a photon at different points on the screen, it gives you the correct curve shape but is not normalized so all the probabilities don't add up to exactly one. To make it a true probability distribution that integrates to 1 you divide |E|^2 by a constant, the total integrated intensity across the screen.> But this E is the classical energy, and when the EM field is quantized don't we need a huge number of photons to define the curve you reference above?If you are able to calculate the probability distribution for where a single photon is likely to deliver its quantum of energy after passing through two slits, then you will be able to calculate how the energy will be distributed across the entire screen for any finite number of photons that passes through those two slits.> Is there a differential equation that when solved, gives us the wf of a RELATIVISTIC particle?If you start with Maxwell's Equations then you get that automatically because, although they were discovered a decade before Einstein was born, they are 100% compatible with both Special and General Relativity. Interestingly they are NOT compatible with Newtonian physics because Newton claimed that all speed was relative, but Maxwell's Equations can produce an absolute speed, the speed of light, and there are no specifications about who should observe that speed, so everybody must. Resolving that inconsistency was the motivation Einstein had for developing relativity; he made no changes to Maxwell's Equations, he thought they were fine just as they are, instead he modified Newtonian physics.
> Is there an equation that gives the wf of a photon? TY, AGAs I explained before, the electromagnetic field amplitude can take on the role of a photon’s probability amplitude.
On Thursday, September 4, 2025 at 4:38:50 AM UTC-6 John Clark wrote:
On Wed, Sep 3, 2025 at 6:53 PM Alan Grayson <agrays...@gmail.com> wrote:
>> |E|^2 gives the relative probabilities of detecting a photon at different points on the screen, it gives you the correct curve shape but is not normalized so all the probabilities don't add up to exactly one. To make it a true probability distribution that integrates to 1 you divide |E|^2 by a constant, the total integrated intensity across the screen.
> But this E is the classical energy, and when the EM field is quantized don't we need a huge number of photons to define the curve you reference above?
If you are able to calculate the probability distribution for where a single photon is likely to deliver its quantum of energy after passing through two slits, then you will be able to calculate how the energy will be distributed across the entire screen for any finite number of photons that passes through those two slits.> Is there a differential equation that when solved, gives us the wf of a RELATIVISTIC particle?
If you start with Maxwell's Equations then you get that automatically because, although they were discovered a decade before Einstein was born, they are 100% compatible with both Special and General Relativity. Interestingly they are NOT compatible with Newtonian physics because Newton claimed that all speed was relative, but Maxwell's Equations can produce an absolute speed, the speed of light, and there are no specifications about who should observe that speed, so everybody must. Resolving that inconsistency was the motivation Einstein had for developing relativity; he made no changes to Maxwell's Equations, he thought they were fine just as they are, instead he modified Newtonian physics.
But ME's describe the behavior of the EM field, not the relativistic behavior of a particle. So I pose my question above again. TY, AG
> Is there an equation that gives the wf of a photon? TY, AG
As I explained before, the electromagnetic field amplitude can take on the role of a photon’s probability amplitude.
But this is within the context of the double slit experiment. If there is a wf for a photon, it should be, I think, independent of any experimental set up. AG
John K Clark See what's on my new list at Extropolis
ijt
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On 9/4/2025 6:24 AM, Alan Grayson wrote:
On Thursday, September 4, 2025 at 4:38:50 AM UTC-6 John Clark wrote:
On Wed, Sep 3, 2025 at 6:53 PM Alan Grayson <agrays...@gmail.com> wrote:
>> |E|^2 gives the relative probabilities of detecting a photon at different points on the screen, it gives you the correct curve shape but is not normalized so all the probabilities don't add up to exactly one. To make it a true probability distribution that integrates to 1 you divide |E|^2 by a constant, the total integrated intensity across the screen.
> But this E is the classical energy, and when the EM field is quantized don't we need a huge number of photons to define the curve you reference above?
If you are able to calculate the probability distribution for where a single photon is likely to deliver its quantum of energy after passing through two slits, then you will be able to calculate how the energy will be distributed across the entire screen for any finite number of photons that passes through those two slits.> Is there a differential equation that when solved, gives us the wf of a RELATIVISTIC particle?
If you start with Maxwell's Equations then you get that automatically because, although they were discovered a decade before Einstein was born, they are 100% compatible with both Special and General Relativity. Interestingly they are NOT compatible with Newtonian physics because Newton claimed that all speed was relative, but Maxwell's Equations can produce an absolute speed, the speed of light, and there are no specifications about who should observe that speed, so everybody must. Resolving that inconsistency was the motivation Einstein had for developing relativity; he made no changes to Maxwell's Equations, he thought they were fine just as they are, instead he modified Newtonian physics.
But ME's describe the behavior of the EM field, not the relativistic behavior of a particle. So I pose my question above again. TY, AGThey also describe the energy propagation of the EM field. And given the known energy per photon that implies the probability distribution of the photons.> Is there an equation that gives the wf of a photon? TY, AGAs I explained before, the electromagnetic field amplitude can take on the role of a photon’s probability amplitude.
But this is within the context of the double slit experiment. If there is a wf for a photon, it should be, I think, independent of any experimental set up. AGNo, it is not only in the context of the double slit experiment. The context of the double slit experiment is supplied by initial conditions.
Brent
So No, I don't agree that applying the double slit will yield a wf
for a photon which supports a similar result as in the case just mentioned. And I am beginning to suspect that we have no equation, the solution of which gives us the wf of a RELATIVISTIC particle, or a PHOTON. If such equations exist, plesae post them. TY, AG
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> I am beginning to suspect that we have no equation, the solution of which gives us the wf of a RELATIVISTIC particle,
>or a PHOTON.
On Thu, Sep 4, 2025 at 11:10 PM Alan Grayson <agrays...@gmail.com> wrote:> I am beginning to suspect that we have no equation, the solution of which gives us the wf of a RELATIVISTIC particle,The Dirac Equation was discovered way back in 1928, and it describes the quantum wave function of a RELATIVISTIC electron.(iγμ∂μ−m)ψ=0ψ is a four-component wave function that represents the quantum state of a fermionm is the mass of the particleγμ is called the gamma matrix, it encode spin and relativistic effects∂μ=(∂/∂t, ∂/∂x, ∂/∂y, ∂/∂z), it's called the four-gradient and it represents spacetime derivativesAnd i of course is √-1>or a PHOTON.
Maxwell’s Equations already are relativistic and they already describe the correct degrees of freedom. So quantization of the electromagnetic field automatically results in photons. So there’s no need for a separate photon wavefunction equation.
> I was aware of Dirac's equation and that it described the electron, but I didn't know that the variable function solved for, was the electron's wf. Are you sure its solution is the wf of a relativistic electron?
> Regardless of the initial condition, we always get an interference pattern on the screen,
> there's no way to get the result for a free particle,
On Fri, Sep 5, 2025 at 7:45 AM Alan Grayson <agrays...@gmail.com> wrote:> there's no way to get the result for a free particle,A "free particle" is a particle that is not subject to ANY external force or have any potential energy, so its total energy is kinetic. That makes things simpler and as a result the quantum wave function is just a plane wave. But in the real world things are more complicated because "free particles" do not exist.
On Fri, Sep 5, 2025 at 6:45 AM Alan Grayson <agrays...@gmail.com> wrote:> I was aware of Dirac's equation and that it described the electron, but I didn't know that the variable function solved for, was the electron's wf. Are you sure its solution is the wf of a relativistic electron?Yes. And for bringing Quantum Mechanics and Special Relativity into harmony is why Dirac received the Nobel Prize, and why he is considered to be one of the best physicists of the 20th century.
>> A "free particle" is a particle that is not subject to ANY external force or have any potential energy, so its total energy is kinetic. That makes things simpler and as a result the quantum wave function is just a plane wave. But in the real world things are more complicated because "free particles" do not exist.> But we can imagine a free particle in empty space
>and we do that often.
> So, IMO, there's no way to get a particle's wf from a double slit experiment,
> Has the solution wf for the electron been solved? If so, by whom? Dirac?
On Fri, Sep 5, 2025 at 9:44 AM Alan Grayson <agrays...@gmail.com> wrote:>> A "free particle" is a particle that is not subject to ANY external force or have any potential energy, so its total energy is kinetic. That makes things simpler and as a result the quantum wave function is just a plane wave. But in the real world things are more complicated because "free particles" do not exist.> But we can imagine a free particle in empty spaceIf you're forcing a particle to go through two slips in a wall before it reaches a detector screen then it is not a free particle.
>and we do that often.College professors often do that because it makes a problem much simpler, so simple he can give it as a homework problem and his students might actually have a fighting chance of actually being able to solve it. But nobody does it because we often (or ever) see a "free particle" in nature.
> So, IMO, there's no way to get a particle's wf from a double slit experiment,Perhaps you should consider changing your opinion. In his book "The Feynman Lectures on Physics", Richard Feynman said "the two slit experiment contains all the mysteries in Quantum Mechanics, a phenomenon impossible to explain in classical terms".> Has the solution wf for the electron been solved? If so, by whom? Dirac?As I've mentioned before, Dirac found a way for Quantum Mechanics and Special Relativity to live together in harmony, and he did it 97 years ago. To this day nobody has been able to do the same thing for General Relativity, it's the holy grail of physics.
> I've never seen a solution to Dirac's equation
n
On Fri, Sep 5, 2025 at 3:57 PM Alan Grayson <agrays...@gmail.com> wrote:> I've never seen a solution to Dirac's equation
n