Sure they can be measured but there is no experiment that guarantees that c contributes very much. Like my poor analogy of the guitar string the energy is contained in the oscillating (frequency) of the photon and has little to do with its propagation. What experiment can prove it comes from c ? What experiment proves one idea over the other? There's already a flaw in one of the ideas considering A massless photon needs an elaborate explanations to explain its momentum. And it really doesn't even do that, it just uses a reverse calculation. — Bill Alsept26 mins ago
You experimentally measure the photon momentum and get $p=h/\lambda$ and Bill Alsept still doesn't seem to believe it. Or am I misunderstanding what he's saying?
@AccidentalFourierTransform That'd be "not constructive". I've moved the thread to chat. @JohnRennie Bill has some idiosyncratic views on light/photons (see the website linked in the profile), you're likely wasting your time.
Take $\Lambda$ to be a Lorentz matrix, it satisfying $\Lambda^T \eta \Lambda=\eta$. By writing $\Lambda=\exp[-\frac{i}{2}\omega_{\mu\nu}\mathcal J^{\mu\nu}]$, we find that the generators satisfy
$$
[\mathcal{J}^{\mu\nu},\mathcal{J}^{\rho\sigma}]=i(\eta^{\mu\rho}\mathcal J^{\nu\sigma}+\cdots) \qqu...
@heather Here's an interesting way to think about it: remember when I talked about the scale factor? The ratio between a galaxy's distance at some time $t$ and its distance now? $a(t) = \frac{\text{distance}(t)}{\text{distance}_{\text{now}}}$
13.8 billion years ago, $a$ was equal to zero.
Every single distance in the universe was zero. However, when the Big Bang happened, $a$ began increasing. Space started to be created between matter.
btw the guy there said I'll probably want to get an adapter for it since it's 1 inch smaller than a hdd but its not necessary if i dont move it around a lot.
what do you think?
@BernardoMeurer sorry i read this wrong, i went for a samsung 850 evo 250gb
@ACuriousMind "banged" his cousin...i thought i read somewhere he hit his younger cousin or something when she was born. am i misunderstanding something?
the idea that objects with mass cannot reach the speed of light because they gain mass and therefore slow down as they approach it in a vicious cycle. the photon can go the speed of light, therefore it doesn't have mass.
@AccidentalFourierTransform But if the photon were massive, would it vary its velocity when moving through gravitational fields or the like? Honest question.
@AccidentalFourierTransform hm, well, I'm not as familiar with that one as I would like, but I would be wary of any definition of particle that prohibits having zero mass
@AccidentalFourierTransform Oh, you mean as a renormalization parameter? Well, I see your point, but I still don't really agree with it. I think the evidence suggests that a proper theory should be able to handle massless particles, and a theory which is incapable of doing so is only useful as an approximate description of reality, unless we find experimental evidence indicating otherwise.
@AccidentalFourierTransform But still, if the photon were massive and decreased its potential energy, wouldn't that increase its speed, so $c$ wouldn't be constant anymore?
@AccidentalFourierTransform Not exactly true, E.g. Coleman-Mandula fails only when there is no massive particle, and I don't really know why LSZ would need mass off the top of my head, either
In other words, if our theories are not compatible with massless particles, I place the blame on the theories rather than on the definition of particle. While recognizing that we don't really know which is the proper resolution.
@heather yeah, but remember $p \neq 0$ for photons
@DavidZ call it a renormalization parameter, call it a real mass. But it is there, in the theory. You cannot take $m\equiv 0$ without running into all sorts of wild divergences
and IR divergences cannot be reabsorbed into counter-terms
@AccidentalFourierTransform What are you talking about? If you're going so formal, then a massless particle is just a state transforming in the massless representation of the Poincaré group. Weinberg's theorem proves that all massless vector bosons are gauge bosons and therefore are protected from acquiring any mass, so renormalization is irrelevant unless the gauge symmetry is anomalous
@ACuriousMind hmm I have to disagree there. CM explicitly assumes that there are no massless states (and a finite number of massive states below any finite energy). And LSZ fails in theories with massless particles
both from the theoretical POV and the practical POV
To put this in other words: if I understand correctly, you observe that QFT can't describe massless particles and conclude that massless particles can't exist, whereas I observe that QFT can't describe massless particles and conclude that QFT is likely not to be a proper description of reality
In any case fundamental QFT is not my area of expertise so I can't challenge you on the mathematical arguments
@AccidentalFourierTransform Explain the success of QED and gauge theories, then. I'll concede they are probably rigorously undefined, but that applies to all but the most trivial or low-dimensional QFTs, so it's a red herring.
@DavidZ more or less. When I said that there are no massless particles I meant that they are not well defined mathematically. I would never venture to claim anything about "reality"
The "keeping mass finite and then sending it to 0" is just another renormalization scheme, I don't see why that should be more disturbing than all the other divergences we have to control in perturbative renormalization
@ACuriousMind you can work with massive QED, and take $m\to 0$ at the very end
that is what it is actually done in real computations anyway
try to calculate the electron self-energy in massless QED
it diverges. The theory is ill-defined
@ACuriousMind no no no no, not at all. Keeping $m\neq 0$ is fundamentally different from keeping $\Lambda<\infty$. IR divergences and UV divergences have nothing to do
using a massive photon is not a renormalisation scheme
@AccidentalFourierTransform And how is that formally consistent regarding the construction of the space of states? You need something equivalent to Gupta-Bleuler quantization (BRST quantization) to get the correct states for the massless theory, and taking the limit of the massive theory does not induces the necessary quotients. Making the massless particle massive completely fails for non-Abelian theories because the decoupling of the longitudinal mode in the amplitudes is more subtle.
@ACuriousMind you can have massive QED with longitudinal states, and these have negative norm. And you have to construct the space of states. It is more complicated than in the massless case but it is in principle the same procedure. You can use the Stückelberg method to restore the gauge invariance of the massive theory, and everything else works similarly to the massless case
As of today, the Stückelberg method is the most general way to give gauge bosons mass
If you're going to make formal complaints about divergences, I'm complaining about the state space of your $m\to 0$ theory begin formally wrong because it still includes those states, even if they decouple