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7:00 PM
To really do the calculation, though, you have to have the complete diagram. Or a good (mathematical) justification for leaving out part of it.
 
So, just to summarize, can you have a diagram that starts or ends with a photon and tell a physicist that the mass of the particles used to create the photon are in its kinetic energy?
 
There are things called factorization theorems which justify how you can draw parts of Feynman diagrams and do certain kinds of meaningful calculations with them.
 
@DavidZ oh, right
 
@Arc676 I'm not quite sure what you mean there
 
@Arc676 that would be a partial diagram then, as DZ says
@DavidZ think pair production. Is it an OK diagram?
 
7:02 PM
For example, if I draw a diagram with an electron-pair that annihilates into a photon, can I say that it's complete by saying that the mass of the leptons is in the photon's energy?
 
No
 
Or a photon that pair-produces an electron-pair saying that the mass comes from the energy of the photon?
I'm guessing neither that is complete
 
@Arc676 Think about it from the center-of-mass frame of the electron and positron. In that frame, the net momentum before the reaction is zero, but after the reaction is nonzero.
@Arc676 Again, in that case, the net momentum after the reaction is zero but before the reaction is nonzero.
 
I don't know what center of mass is...
 
Well, it's really center of energy
 
7:03 PM
@DavidZ wait, it would be the reverse, no?
In the center of mass frame, the e and p have zero net momentum
But the photon has momentum in all frames
 
Well, whichever state (initial or final) has the electron and positron, there is zero net momentum.
 
ah yes that
now it makes sense
(same thing that Chris said, but I thought over it more after that)
I think I've already gone through this before and gotten myself straightened out, but seem to be rusty.
 
@Arc676 Anyway, if you don't know what center of energy is, it's probably way premature for you to be learning about Feynman diagrams
 
I'll google it
So you CANNOT have a diagram that starts or ends with a photon
 
But the gist is that I'm talking about a reference frame in which the electron and positron have zero net momentum.
 
user54412
7:05 PM
i've seen authors distinguish between "center of mass" (origin of your coordinates is such that the masses times vector displacements sum to 0) vs. "center of momentum" (origin is not important, but probably coincides with center of mass for ease; velocity is chosen such that (3-)momenta sum to 0)
 
@DavidZ CoE is CoP , or ...?
 
What's the difference between center of mass, energy, and momentum
 
@Arc676 You cannot have a diagram that starts or ends with a single photon. Unless it's a really boring diagram that just has one photon doing nothing.
 
A diagram with no reaction, that is
 
@DavidZ can't the photon itself split?
 
7:06 PM
I was about to correct myself ;-)
 
user54412
at first I was going to counter with a photon -> e+e- virtual pair -> photon...
 
You can have a diagram where a photon splits into a virtual electron-positron pair and then turns back into a photon. The point is, if you start with a photon, you have to end with a photon, and vice-versa.
 
Yep
 
user54412
@DavidZ but if that photon is on-shell, is it possible?
 
@ManishEarth You said e and p can represent electron and positron. Doesn't p represent proton?
 
user54412
7:07 PM
as in, will the electron/positrons be too off shell?
 
@Arc676 I'm not sure of the exact technical definitions of these things. I'm just talking about a reference frame in which the initial particles have zero net momentum.
 
@Arc676 no, that was me trying to type less
e and e+
 
@ChrisWhite You can certainly draw the diagram and calculate the amplitude, and I think it will come out to be nonzero, but I'm not sure.
 
@ManishEarth Ah...
 
@ChrisWhite what's too off shell?
isnt off shell ... off shell?
 
user54412
7:08 PM
@ManishEarth i have no idea :P
 
@ManishEarth Sorry, my wireless likes to crap itself randomly lately and I just now got back on... I was around for that conversation, yet
 
user54412
but it just seems that finding any finite position in E-p space for a typically massive particle to behave like it has no mass...
 
Does anyone know a site with an explanation for center of energy and momentum or should I ask here?
 
user54412
maybe i just need to write down an actual equation
 
7:09 PM
@Arc676 here is fine
 
The whole E^2 - p^2 = m^2 relation goes out the window for virtual particles
 
CoMomentum is the frame where net P is zero
 
@DavidZ Are you sure about that?
 
Dunno what CoE is, suspect it to be the same thing
 
user54412
@ManishEarth CoMomentum? that's a new term for me
 
7:09 PM
In the context of Feynman diagrams I've seen CoMo being used
 
Center Of Momentum @ChrisWhite
 
@ChrisWhite Center of Momentum :P You just used it
 
user54412
ohhhh
 
I would call it CoP, but that gets confusing
 
@Arc676 Yep. E^2 - p^2 can have any value for a virtual particle. But in general, the greater the difference between E^2 - p^2 and the m^2 of the actual particle, the less likely the reaction is.
 
7:10 PM
and CoM is Center of Mass.
 
user54412
reminds me of one particular intro to SR book that insists on saying "momenergy" for 4-momentum
 
@ChrisWhite hahahaha sounds like something I would do
 
@DavidZ If the formula is E^2=(mc^2)^2+(pc)^2 shouldn't you mention c somewhere in that equation?
 
@ChrisWhite confirmed that photon -> e+ e- -> photon is a necessary correction to the photon propagator
 
@Arc676 natural units, c=1
 
7:11 PM
Natural units?
 
In physics, natural units are physical units of measurement based only on universal physical constants. For example the elementary charge e is a natural unit of electric charge, and the speed of light c is a natural unit of speed. A purely natural system of units is defined in such a way that some set of selected universal physical constants are each normalized to unity; that is, their numerical values in terms of these units are exactly 1. While this has the advantage of simplicity, there is a potential disadvantage in terms of loss of clarity and understanding, as these constants are then...
 
So when exactly can you use c=1
 
Feel free to put in the c's to make the units work out, if you like.
@Arc676 Whenever you're using units such that the numerical value of the speed of light is 1.
 
@Arc676 anytime, as long as you remember that this constrains your unit system
 
If c=1 what is OUR speed when we walk...?
 
7:13 PM
See, we have 3-5 fundamental units (mass, length, time, current, temperature)
 
I'm guessing this numerical value is only used when one measures really fast objects right?
@ManishEarth and they are kg, m, s, A, ºC right?
 
If we set G,c,hbar to 1, that fixes a system of units for mass, length, time. Setting epsilon_0 and k_B to zero fixes the other two if necessary
@Arc676 those are the SI units
 
@Arc676 $1.4 \times 10^{-9}$
 
But I can pick a unit system where $G=c=\hbar=k_B=\varepsilon_0=1$
 
Is a formatted formula supposed to appear? I just get plain text
and a lot of slashes and dollar signs...
 
7:14 PM
Nope, I use an extension
 
Ah
 
68
A: Should chat have TeX support?

robjohnI will leave the original post for historical reference, but as mentioned in the Update below, all four bookmarks are located on this installation page. There are four bookmarks: start ChatJax installs MathJax and starts a loop that renders $\LaTeX$ as needed. This is intended for use in chat, ...

 
4
Q: MathJax in chat (ChatJax offshoot)

ManishEarthThis is an offshoot of ChatJax, which enables MathJax along with mhchem on chat. Copy the text below: javascript:(function(){if(window.MathJax===undefined){var%20script=document.createElement("script");script.type="text/javascript";script.src="https://d3eoax9i5htok0.cloudfront.net/mathjax/lat...

 
@DavidZ On the topic of before, if you CAN'T have a diagram in which the final state weighs more than the initial state, you can only have a Higgs as an intermediate particle right?
Or can you begin the diagram with the Higgs?
 
@Arc676 why can't we tree up a bunch of lighter ones to create a Higgs?
 
7:18 PM
@Arc676 When the initial state particles are moving very fast, i.e. they have a lot of kinetic energy, there can be enough energy to create a real/on-shell/m=125GeV Higgs boson.
 
Higgs will decay though
 
The Higgs boson itself is unstable, so it will decay quickly whether it's real or virtual.
But if your Higgs boson is on shell, you can validly draw a Feynman diagram which starts with a Higgs boson.
 
but can we draw one that ends with an H?
because decay
 
user54412
@DavidZ in the same sense as you can validly draw a diagram beginning/ending with a free neutron, right?
 
I thought you said you cannot have a "real" complete diagram in which it produces a particle with more mass by using the energy of the others
 
7:20 PM
@ChrisWhite Yeah, that sounds about right
 
@ManishEarth That would be a diagram that doesn't show the last reaction, therefore incomplete
 
@Arc676 No, I didn't say that. Well, maybe I did by accident way back, but I would have been wrong. If you remember which message it was exactly, I could clarify.
 
thought so
 
user54412
@ManishEarth i feel there's a time reversal symmetry you're trying to break there
 
@ChrisWhite The force is strong with this one
 
7:21 PM
@ManishEarth You can, if you take the final state Higgs boson to be on shell. You would then find that the amplitude is zero unless the initial state particles have 125 GeV in the center of momentum frame.
 
@DavidZ Not sure which message, but I think it came up when we were talking about the initial or final photon
@ManishEarth Who is "this one"
 
@DavidZ So we can have a feynman ending with an undecayed product if it is on shell?
@Arc676 CW
 
@Arc676 Yeah, I don't quite remember either, but I think I may have made an incorrect statement back there somewhere. The point is, it's energy that matters, not mass.
 
As in, feynman diagrams can end with muons and all?
 
@ManishEarth You referred to the person you were directing the message to in third person...?
 
7:22 PM
@ManishEarth Yes. Of course that doesn't mean the product will sit there forever. It will decay, you just don't have to show that in the Feynman diagram.
 
@Arc676 it's a quote from Star Wars
 
@DavidZ That makes sense since they're interchangeable
 
@DavidZ ah, thanks. That's what I originally meant when talking about "not having to show the full reaction"
 
@ManishEarth I know that part, but you added the @, so it's like calling the person you're talking to "him"
 
7:23 PM
@Arc676 Oh, that's because I used the message-reply. Wanted to link messaged
 
@ManishEarth Ah
 
@Arc676 you might find this interesting reading
 
@Articuno Ludovic? I don't think anybody understands his questions
 
user35386
okay, that is relieving
 
7:24 PM
It seems this Ludovic has built up a reputation for hard-to-understand questions
 
though...they probably should be closed then
 
Yeah, I was going to say, it seems like several people understood them well enough to upvote them
 
@Arc676 hard-to-understand similar fluid dynamics questions with big pictures that somehow my brain doesn't let me read in full
 
How do you have a planet inside water (first link)
 
O_0
 
7:32 PM
Just to summarize the earlier topic, I understood that you can have basically ANY particle in the initial state, as long as the final state has equal or inferior mass, correct?
 
@Arc676 Energy. Not necessarily mass.
 
Right, energy. How do you measure the energy of each particle?
 
Actually that depends on how you define mass. If you define it as the total of the masses of the individual particles in the initial state, then you can definitely have higher-mass particles in the final state. But if you define the mass of the initial state as the energy of the initial state in the reference frame where those particles have zero net momentum, then you cannot have more energy in the final state.
 
So can I have two gluons produce a quark-pair that interact and create a Higgs boson (which later decays into a quark pair)?
 
Yep
 
7:40 PM
And how would I mathematically prove this?
 
Draw the Feynman diagram, calculate the corresponding amplitude, and show that it's nonzero
The process is known as gluon fusion, or vector boson fusion
 
I've never calculated "amplitude" I followed a non-mathematical and very basic tutorial (yes, I know, not the best way to learn physics, but I'm also busy with other things)
Another idea: we know how to draw vector fusion, how do I calculate exactly how many Z bosons the up-quarks can emit? They obviously cannot emit an infinite amount of Z bosons and an infinite amount of Higgs bosons, because that would be an incredibly obvious violation of mass conservation (and consequently, due to their interchangeability, energy conservation)
 
No, remember, there is no such thing as mass conservation in particle physics
 
So energy conservation, how do I prove that I cannot have an infinite amount of Z bosons and therefore higgs bosons?
How do I know how many times the same two quarks can accomplish vector fusion
In fact, how do I know vector fusion can be achieved at all? How can two up-quarks react and have a final state of 3 up-quarks and one anti-up-quark
 
Um... wait, I'm a little confused. There's no need for up quarks to be involved.
Vector boson fusion looks like this:
(not the bottom right diagram)
 
7:49 PM
Wait, I thought vector fusion was only the diagram on the top right
the one with the quarks Z bosons, and the Higgs in the final state
Even if the three (i.e. not the bottom right) are all called vector fusion, I meant the one on the top right
How do I prove "this quark can only emit x Z bosons, and therefore only x Higgs bosons can be created"
 
You don't, really, because in principle the quark can emit any number of Z bosons. But the probability decreases sharply as the number of emissions increases.
 
Wait, so I can essentially spend the rest of my life drawing a diagram that never ends in which I produce infinite matter in a very unlikely situation? Wouldn't that violate energy conservation since each Higgs can decay into a quark-pair, each with its own energy?
 
Not necessarily. Remember, the masses of the particles only matter for the initial state and the final state. So as long as in the end, you wind up with some combination of particles that has a total energy equal to the total energy you started with, there's some probability that the reaction will happen.
(well, subject to all the other conservation laws of course)
 
So it's actually possible to have two quarks, produce 100 Higgs bosons, have them decay into 100 quarks pairs, and end with 202 up quarks and 100 anti-up-quarks each with a minute amount of energy?
 
Yep
 
7:59 PM
I have one question: For example i have triange (a = 5 and b = 4) and i want to calculate C ^ 2 using gmn(metric tensor) * dy(r) * dy(s). C ^ 2 will equal to (kronecker_delta(mn) * sum((dx(m)/dy(r)) * (dx(x) / dy(s)) * dy(r) * dy(s)), and then it will equal to (kronecker_delta(mn) * sum(dx(m) * dx(n)), and When I will put numbers, it will equal to 5 ^ 2 + 4 ^ 2 yes? Am I correct?
 
Well, possible in the sense that you could draw that Feynman diagram, and it would make a nonzero contribution to the total amplitude
 
@DavidZ Wow...
 
@Gigi10012 5^2 + 3^2? Did you mean 5^2 + 4^2? In any case someone else might have to respond more carefully to that.
 
@DavidZ thanks
 
I'm gonna go now, I'll c you all tomorrow!
 
 
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