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3:00 PM
Ok, that's a very helpful thing to know.
Thanks.
I will now retreat to a cafe with my notebook and a pen, and will likely return later for a more rigorous go-over.
I'm also interested to understand this without the discrete approximation step.
 
I assume there are "operator-y" ways to think about all of this stuff.
 
@SirCumference I have an astronomy question. Do you have a few minutes to spare?
 
@2017 Sure :)
 
Heh, actually, I think this extra source term is going to wind up being a normalization factor that I don't care about...
We'll see.
 
3:02 PM
@DanielSank I don't know what you're doing, of course, but usually, the term without the source ends up being the normalization factor
 
@SirCumference Yeah, so I was learning the applications of Doppler's shift recently. Most books seem to mention that light from cosmic objects is redshifted/blueshifted. But what is the reference for the light? w.r.t what is the redshift/blueshift measured?
 
@2017 Not sure if I understand your question. Do you want to know how to calculate redshift?
 
Suppose the received wavelength is $\lambda_R$
Then what is the $\lambda_o$ ? Such that $\lambda_o-\lambda_R=\text{shift}$
 
OK, so the formula is
$$1+z = \frac{f_{\mathrm{emit}}}{f_{\mathrm{obsv}}}$$
Or $$1+z = \frac{\lambda_{\mathrm{obsv}}}{\lambda_{\mathrm{emit}}}$$
 
@SirCumference Yup, how do you know the $f_{emit}$ ?
 
3:06 PM
@2017 Many observations are made of emission/absorption lines. We know where in a spectrum certain ones should show up, and if the observed spectrum can be matched with a spectrum at $z=0$, we can tell how much the wavelength has been shifted by. We then use @SirCumference's formula.
 
@HDE226868 "we know where in a spectrum certain ones should show up"....but for that you need to know the composition of the cosmic object beforehand, isn't it?
 
@2017 Sure, but you can expect certain lines to show up in most cases, depending on what the object is.
(This is for spectroscopic redshift, not photometric redshift.)
 
@HDE226868 "expect certain lines to show up in most cases"...could you give some examples? I'm not sure I get you...
Do you mean for planets or stars you expect some spectral lines for sure?
 
@2017 The Balmer series is commonly observed.
@2017 Yes, you'd expect something like that to show up in most stars.
Stars obviously have quite a lot of hydrogen, and there should be plenty of that in the atmosphere. This leads to Balmer lines.
 
3:13 PM
@HDE226868 We now know that stars have a lot of hydrogen. But, before this technique of doppler shift was discovered, did we know it? Or it was just an educated guesswork initially ?
I suppose the wavelength of each different type of material is shifted by nearly same amount....so perhaps some extrapolation would do the job
 
@2017 I don't know that off the top of my head. I believe spectroscopy of the Sun (and thus theories of its composition) slightly predates the proposal of the Doppler shift, but I'm not 100% sure.
There were plenty of developments in the 19th century, though.
 
@HDE226868 Ah, that's seems an interesting topic :-) Thanks for helping...I need to read a bit more about this! Thank you!
 
@2017 No problem.
 
@SirCumference Thank you too :-)
 
@2017 Oh, np
 
3:36 PM
0
Q: Stings in the loop space of timelike curves

SlereahIn Smith's paper on homotopy groups for Lorentz manifolds, he builds the loop space of all timelike loops in the following fashion : Consider all piecewise continuous timelike curves which start and end at point $x$. This include timelike curves with $q$ changes in time orientation (the tangen...

plz respond
I kind of suspect that when he says "this isn't enough to have a group structure", he was refering to the absence of the constant path
But that doesn't really explain why stings are there
 
@ACuriousMind can you expand on the idea that $J A^{-1} J$ has something to do with propogation?
In general, we have some linear equation $T|\psi\rangle = |J\rangle$ and we want to solve for $|\psi\rangle$.
To me, a "Green's function" is the solution to $T |G \rangle = |e \rangle$ where $|e \rangle$ is some basis vector.
 
but what is
the red function
 
So then $|J \rangle = \sum_i |i\rangle J_i$ and $$T |\psi \rangle = \sum_i |i \rangle J_i$$ so $$|\psi \rangle = \sum_i |G_i \rangle J_i \, .$$
 
"Smith's understanding of the relationship between corporeal and physical objects extend to his interpretation of biology, where he has become an opponent of Darwinian evolution, as the fundamental element in a species would be its form, not its causal history, which evolutionists favor."
"Smith has also taken a stance towards a relativistic rehabilitation of geocentrism."
Wew lad
I'm starting to have doubts about that guy
I hope he's not crazy about math either
 
@DanielSank It's classical propagation, not quantum: If $A$ is a linear differential operator, then one can often solve the equation $AG = \delta$ for $G$, where $\delta$ is the usual delta distribution. Then, the equation $A\phi = J$ is solved by $\phi = \int G J$ (that's a convolution, I don't want to botch the variables here).
So the operator $\int G$ is inverse to $A$.
 
3:51 PM
"According to Smith, such an interpretation of quantum mechanics allows for the usage of the hylomorphic concepts of act and potential to properly understand Quantum superpositions."
 
@ACuriousMind (I use $*$ for convolution)
@ACuriousMind Ok so $J A^{-1}J$ is like $\langle J | \int GJ \rangle$.
 
I could send him an email, he's still alive
 
...as we said earlier.
 
@DanielSank Yes, exactly
 
If he knows how to use a computer
(He's 87)
Oh wait
I know what's going on
His math papers are from the 60's
His crazy papers are from the 90's
 
3:54 PM
And you can get surprising mileage out of the idea that now taking functional derivatives w.r.t. $J$ of that gives you back combinations of $G$, depending on how many you take.
 
He got the physicist disease
 
Interesting. I wrote $|\psi \rangle = \sum_i |G_i \rangle J_i$, but you wrote $\phi(x) = (G * J)(x)$.
 
That's behind the "generating functional" that forms a large part of the path integral approach to QFT.
 
These must be the same thing.
@ACuriousMind That sounds familiar.
$$\langle x | \psi \rangle = \sum_i \langle x | G_i \rangle \langle i | J \rangle$$
@ACuriousMind I think your form requires translational invariance, or something.
 
@DanielSank Yes, the Green's function only acts as a simply convolution if $A$ is translationally invariant
Otherwise it's a true function of two variables and you don't convolve, you simply integrate $\int G(x,y) J(y)\mathrm{d}y$.
 
3:58 PM
@ACuriousMind Yeah ok.
That matches what I have up there in bra-ket notation.
Thanks.
I might have written $G_y(x)$ where you have $G(x,y)$, but whatever.
 
4:10 PM
@JohnRennie If we pull an elastic rod with a constant force $F$ upwards (gravitational acceleration still stays g), then to calculate the extension in the length of the rod (using the Young's modulus method) do we consider the net effect of $g$ and $F/m$ or do we only take $F/m$ ? My book neglects the $g$...but I think that is wrong!
 
4:37 PM
@heather we should chat about your multi qubit basis question.
 
@DanielSank, I saw your comment, but I'm not sure how the Kronecker product relates (I read through the wikipedia article).
 
Ok let's start from the beginning. What are you trying to do?
 
@EmilioPisanty Thanks for pointing out the copyright though, I would've screwed up.
 
@SirCumference No worries, just think it through next time
To be honest, I'm not entirely sure whether the logo infringes that image as it is
 
Yep :)
 
4:45 PM
it's probably covered under fair use (?), but that's always a tricky area
In any case, I still think the question is not particularly well formulated (and indeed it's pretty entitled) in its current version, but I've seen that you just won't be persuaded so oh well
 
@EmilioPisanty Well if you have any suggestions, I'm all ears. I'm just hoping my suggestion will be heard.
 
@SirCumference I've said it something like five times already
 
@DanielSank generate a list of the basis vectors that will be eventually used to calculate the state of a qubit, which will be manipulated in the program.
 
Make it clear that there are in-practice instances of the logo being under-resolved
in the question itself
 
OK, I'll get to that when I get home
 
4:48 PM
"vector logo" isn't a goal in itself
it's a tool to get a crisp logo in all real-world instances
 
Which is a few hours from now
 
@heather the basis vectors are always $\{ (0,0,1), (0,1,0), \ldots\}$.
 
the fact that you can zoom in enough to get it to show its pixels is meaningless if under normal conditions it shows fine
 
I think your real question is what these tuples mean in terms of the single qubit states.
 
Either way, there's no "we" in updating the logo file
The design is managed entirely by the SE design team
and a vector logo file is not a trivial change
 
4:50 PM
@DanielSank not always...i thought for a single qubit system, it was [0,1] or [1,0]; for a two qubit system, [0,1,0,1], [1,0,1,0], [1,0,0,1], or [0,1,1,0]
 
@BenNiehoff In the corners of nuclear and particle experimentation (and instrumentation) that I've been involved in there is an expectation that every paper can be found on arXiv.
 
Not all browsers support svg
 
@EmilioPisanty Duly noted.
 
I've had papers with tens of citation by the time they first appeared in "print".
And they were in PRL at that.
 
and that means that they need to implement a fallback png
and that means code
and it means testing to make sure it works fine for all relevant browsers
 
4:52 PM
I can't chat from my computer...
test
 
Nawh, just a quiz.
 
i can read it @DanielSank
 
@heather you have to remember what it means to write vectors as lists of numbers.
 
@DanielSank each of the components of the vector
 
It's probably worth implementing if it actually impacts how the site looks, but if it doesn't then it's not worth the extra work. So put the evidence up front.
 
4:53 PM
Those lists implicitly mean $$(a, b, c) \equiv a |e_1 \rangle + b|e_2 \rangle + c |e_3 \rangle$$ where $|e_i \rangle$ is a particular choice of basis vectors.
 
Yep :)
 
The bitmap logo is probably a holdover from way before high-dpi was a thing
 
If you're trying to write a basis in its own basis, then of course they'll be $(0,0,1)$, $(0,1,0)$...
 
and this site is not usually at the top of the list in terms of getting site-design upgrades
 
^ THat.
 
4:54 PM
witness e.g. the network-wide CSS update
6
Q: Is there a known timeline for the deployment of the new CSS?

Emilio PisantySome six to eight weeks ago, Stack Exchange announced a programme to re-design the CSS and tweak the site styles throughout the network, including the completely redesigned profile pages. Since then, we've made some big requests to come with the re-design, so we've remained "on deck" for some tim...

 
@heather I think you're confused because you 1) don't know what your basis vectors actually are, and 2) Don't know how those basis vectors relate to the single qubit basis.
 
including a sizeable update to the profile pages
 
@DanielSank right
 
We've just big enough to be "important" in some way, but still small enough that it's not a very important kind of important.
 
@DanielSank oh
but...that isn't what i'm looking for, i'm looking for the basis, just not written in it's own basis, i guess. the basis that i'd use to calculate the state of the qubits.
you're right, i'm very confused =/
 
4:55 PM
@ACuriousMind If $$ \int dx_1 \ldots dx_n \exp \left( -\frac{1}{2} \sum_{ij} A_{ij}x_i x_j \right) = \sqrt{\frac{(2\pi)^n}{\text{det}A}} \, ,$$ then what is $$ \int dx_1 \ldots dx_n \exp \left( -\frac{a}{2} \sum_{ij} A_{ij}x_i x_j \right) \, ?$$
 
@dmckee I dunno
 
vzn
@Obliv an interesting topic for Computer Science chat? swade is one of the worlds leading authorities on babbage machines/ engines, he basically got the designs to really work over ~1½ century after devised, hes got a good book out on it too, recommend it. there have been some exhibitions at museums in recent times.
 
being the very last site to get the CSS update was...
not demoralizing, but you do have to wonder
 
@DanielSank Do $x'_i = \sqrt{a} x_i$.
 
I would think I'm just multiplying $A$ by $a$, but when I look up the result elsewhere we get a new factor of $\sqrt{a^n}$.
@ACuriousMind Right but why can't I think of it as a scaling of $A$? Scale factors factor out of determinants...
@heather, when I write a matrix, what do the elements of the matrix mean?
 
4:59 PM
Either way, @SirCumference put your evidence up front, and keep in mind that whenever the design is involved you are asking other people to do work for you.
 
Oh wait...
If I scale a matrix, the determinant scales by that scale factor raised to the dimension of the matrix, doesn't it?
 
@DanielSank yes
 
@DanielSank Indeed it does
 
Yes, of course, because determinants are volumes of the result of acting the matrix on the unit hypercube.
Ok we're done here. Thanks @ACuriousMind and @EmilioPisanty.
 
@DanielSank well, the basis vectors of the system you're transforming too.
 
5:00 PM
@heather you keep getting confused by this :-) We've had this discussion before.
 
@DanielSank or, more simply, the matrix scales by $a$ whenever you multiply each row individually by $a$.
 
^ yes
 
@DanielSank we have? let me check the transcript then, i don't want to waste your time
 
It was a long time ago and the connection is probably not obvious to you.
Forget quantum computing.
We need to go over some linear algebra stuff.
 
@dmckee Meanwhile, I'm not sure if any of my papers have tens of citations at all! :P
 
5:03 PM
BTW, now that there's some form of quorum:
given that this exists
 
in the sense of plural tens
 
@ACuriousMind can you unlock this?
 
@BenNiehoff It's all about subfield. That's why bibliometrics are a terrible way to evaluate scientists.
 
5:03 PM
Does our site logo infringe the Wikipedia copyright?
 
or @dmckee
@heather go here
 
I'm a very run-of-the-mill researcher and I'm an author on two topcite-500 papers.
 
@DanielSank Done
@EmilioPisanty Is a Feynman diagram even copyrightable?
 
@ACuriousMind Ideas are not copyrightable
specific instances of graphics are
the site logo is a direct copy, just monochromated
 
user228700
@JohnR: Did u get around to watching the video?
 
5:05 PM
@DanielSank okay
 
and take out the arrow and the t
 
My most-cited (and coincidentally, oldest) paper has 24 citations...that is the only one with plural tens :P
 
@EmilioPisanty But only if they pass some threshhold of originality. I have my doubts this one does.
 
@BenNiehoff I guess I feel better now =P
 
@EmilioPisanty What do you feel better about?
 
5:06 PM
@Kaumudi.H Hi :-) yes I did have a look, but I think it was American cooking rather than British. I'm pretty certain we never had Cambell's cheese soup in the UK.
 
I'm quite sure that Feynman diagram had been drawn thousands of times before the version on wikipedia was first constructed.
 
@BenNiehoff 34 citations on my most-cited paper
 
user228700
@JohnRennie Hi :-) Yep, it was primarily American.
 
And if not, it's easy to just draw another one that looks pretty similar...
 
That's the point, it's not a looks-similar case
It's clearly a direct copy
 
5:07 PM
I would consider Feynman diagrams more like words: you assemble them from a finite set of predetermined components.
 
sure, I'm saying if it bothers you, you could correct the problem easily
 
user228700
Are ur servers doing OK? (:-P)
 
Oh, and most of my citations are from collaborators and their friends :P
 
@BenNiehoff I can't. Changing the design assets is an SE job.
 
I see. Well, one could write them a threatening letter
 
5:10 PM
@BenNiehoff My sole lead-author paper has six citations. And half of them are from the collaboration I did that work for.
 
@BenNiehoff you'd have to be the copyright holder for that to be even mildly threatening
but being a good internet citizen is worthwhile on its own
 
well, it's possible that Feynman diagrams aren't copyrightable anyway
 
And two of the others are in a context that comes down to "We were careful not to get into the kind of pickle where we'd have to do the work that McKee did".
 
is there a legal SE where one could ask? :P
 
::sigh::
 
5:10 PM
there is
 
actually, yeah, there's a legal SE
 
@BenNiehoff Law
 
goddammit
google scholar
 
5:11 PM
The last one is a very nice comment in a major review, so that's something.
 
stop bungling up my name
 
what did they do?
 
@BenNiehoff That EP Alatorre is Emilio Pisanty Alatorre
and they've gone and put my paternal surname down as a middle initial
 
ah, I see
 
Ignoring the Christoffels (which can't be ignored), this is the shortest I can get Schwarzschild, which is not that short :( :
 
5:13 PM
are you Spanish?
 
@EmilioPisanty Is Alatorre a second surname or more akin to a middle name? (I have no idea how your name works, as you might see)
 
That still seems shorter than what Wald does
 
@BenNiehoff I'm Mexican
 
ah, ok
 
Pisanty is my paternal surname, Alatorre is my maternal surname
I normally publish as Emilio Pisanty because maternal surnames confuse English speakers to no end
 
5:16 PM
@0celo7 Write up a Straumann/Wald solution shorter than mine above
 
but the thesis needed to be in the name I was registered under and that needed to match my passport
and, of course, it's gone on to confuse the hell out of google scholar
now to figure out how to bring it into the fold
 
one of my grad-school friends was Mexican...he was named José Raúl, but only introduced himself as José
we found out three years later that he in fact goes by Raúl back home :P
but he thought it would be confusing that someone went by their middle name, so he just used the other one with us for three years instead :P
 
yeah, that can happen
it's not as bad as needing to invent entirely new names, like many Asian people feel they need to do
 
I think that happens less often now
 
but yeah, there's some pretty intense pressure to change how you interact with your name because English-speaking culture simply can't be bothered to acknowledge that there are other naming conventions
@BenNiehoff I knew multiple people who did that in grad school a couple years back
 
5:20 PM
sure, not saying it doesn't happen
but I know loads of Asian people who just use their actual names
but backwards of course
 
haha...even I have run out of space for my name on a form where little boxes were provided for one letter each
and I don't even have a long name
I dunno wtf they were thinking
 
@EmilioPisanty That's common enough that I have a half-Korean friend who experiences a kind of inversion of that: His name is Otto and it's quite common for people to ask him "No, what's your real name?" since they don't believe an Asian would have such a stereotypically Northern German name.
 
one of those was behind some large-scale outage if I remember correctly
 
@EmilioPisanty There's a better version of that somewhere that actually gives examples for each point
Unfortunately I seem to have misplaced the link to it
 
5:27 PM
I've had Indian people be impressed that I could actually pronounce their names...I was mostly surprised that I guess nobody had bothered trying before
 
@BenNiehoff i have some friends who are indian, and rarely does anyone pronounce their names right. i had to get them to explain to me how you're actually supposed to pronounce their names (especially their last names).
now I do it correctly, thank goodness, but i also wince along with them when a teacher butchers it especially well.
 
Paging Cow-smoothie (@Kaumudi.H)
 
@BenNiehoff As a fun fact, Indians themselves find Indian names of people (belonging to other states) very difficult to pronounce. For example, I still don't know how to pronounce @Kaumudi.H's name! India has just too many languages and dialects.
 
I'm not talking about perfect pronunciation...I don't know the exact IPA values of all the sounds. But most people don't even bother to use the right number of syllables and put them in the right order
 
ah, yes, this is what it was
> Cloudflare hit by leap second “software panic” snafu on New Year’s Day
caused by code that assumed that a datetime function would be monotonous
 
5:33 PM
@BenNiehoff Yeah, I agree with that. Some of my friends had very bad experience in Singapore when they were forced to select a new name for themselves as the people there couldn't pronounce them properly.
 
user228700
@2017 Cow-moothie works :-P
 
@Kaumudi.H just "cow" will be shorter and sweeter :D lol
 
user228700
Sure :-P
 
Hi everybody
 
user228700
BTW yes, I completely agree. My neighbor calls me "Gomathi" because she still doesn't know how to pronounce my real name.
 
5:37 PM
@Kaumudi.H, hello =)
 
Obviously the EFE for Schwarzschild involve the second derivative of the (logarithm of the) time scale factor with respect to position $\frac{d^2 \nu}{d r^2}$ plus all obvious ways to make the first derivative of this non-linear, e.g. $(\frac{d \nu}{d r})^2$ and $\frac{d \nu}{d r} \frac{d \lambda}{dr}$ as well as the derivative of the (logarithm of the) radial scale factor, per unit radius $\frac{\lambda'}{r}$, up to signs and scale factors :'( :'( :'(
 
Why are you obsessed with the most basic solution
 
Because it's the whole content of GR!!!! (modulo tons of stuff)
 
Not the actual derivation though
 
@bolbteppa where's your metric ansatz?
 
5:44 PM
I can copy in the metric and Christoffels if you want
 
@bolbteppa no. Why should I?
 
Do you not think it's useful to know the most important calculation in a subject like the back of your hand?
 
I mean, it's a calculation you can do in a page :P
 
@bolbteppa no
Not even a little
I think you need to reevaluate how you view science
 
Engineers don't need to I suppose
(burn)
 
5:54 PM
How is that a burn?
 
You can't put Schwarzschild into a bucket of water and just get the answer, need to assume spherical symmetry and get it directly
 
What?
 
@bolbteppa that's obviously wrong
you can't assume a cat is spherical
but you can do just fine with a sphere and a cylinder
 
^
#getreal
 
lol, very true @EmilioPisanty
 
5:58 PM
5 cylinders, two spheres?
 
two spheres?
 
head and body
 
four legs and tail, for the cylinders...hmm, body is probably better as a cylinder
 
or this
 
and you could add in triangular prisms as the ears
 
5:59 PM
The body is not spherical unless the cat is obese
2
 
but really, single sphere and six cylinders is plenty
 
@heather the ears make up a very small volume
 
@0celo7 true =)
@EmilioPisanty that's a very styling cat
 
or this
 
$\int_{cat}dV = \int_{sphere_{head}}dV_1 + \int_{cylinder_{body}}dV_2 + 4\int_{cylinder_{leg}}dV_3 + \int_{cylinder_{tail}} dV_4$
 
6:00 PM
source
14
A: How do astronauts turn in space?

WetSavannaAnimal aka Rod VanceAlthough this has indeed "worked to bits" on the Physics and other SE sites it's worth looking at, for the sake of Space Exploration, the interesting history behind the analysis of the falling cat. For the fully rigorous description of the cat's righting reflex - perfectly in keeping with conserv...

 
What is the average density of a cat? :-P
 
Is it more than humans?
 
@0celo7 link doesn't work
 
6:02 PM
@EmilioPisanty hmm. Imgur is doing strange things on my phone
 
> The imgur.com page isn’t working

> imgur.com redirected you too many times.
 
It's saying I have to wait 3400 seconds until I upload again.
Never had that happen
 
i see the cat
it really doesn't care at all, lol
 
It's a cat. Not caring is in the job description.
 
OBE
@0celo7 sup?
oh because drake is canadian?
@ACuriousMind I like your new pic.
nice blue shadows on your face
 
6:23 PM
It seems people on the chat downvote my imgur posts
Wtf is up with that
 
How do I make slanted dots in mathjax?
$$\ddots$$
oh
 
What are slanted dots?
 
dots ddots vdots
 
@ACuriousMind this is mostly for you.
I'm trying to create an opportunity to carefully explain what we discussed earlier. If you don't have time, I will attempt an answer, but I'd rather not muddy the waters with something less than crystal clear.
 
What are some important maths topics that are common through out physics ? I am looking to get some books to brush up my maths during the summer and want to know what topics in maths to read up on to get a good head start
 
Can someone please check the following QM query please. Given an ensemble of $N$ two-level systems where we define operators $\hat{J}_z := \sum_i \frac{1}{2} \hat{\sigma}_{i}^{z}$ and $\hat{J_-} := \sum_{i} \hat{\sigma}_{i}^{-}$ where $\hat{\sigma}_{i}^{z}$ is the $z$ pauli operator and $\hat{\sigma}^-_{i}$ is the lowering operator on the $i$-th particle i.e. $\hat{\sigma}_{i}^{-}| \uparrow...\uparrow_i...\uparrow \rangle = |\uparrow...\downarrow_i...\uparrow \rangle$.
How does it follow that
$$\hat{J}_{z}(J_-| \uparrow...\uparrow \rangle) = \sum_{i,j}\frac{1}{2}\hat{\sigma}_{i}^{z}|\uparro
 
7:02 PM
@ACuriousMind FYI, when I use bra-ket notation, that does not mean I'm thinking quantum.
It just means I'm thinking vectors.
 
7:33 PM
So @DanielSank about your question
The identity you give comes from the following (this is the analogous computation for field theory since I happen to have that one written out): If $\mathcal L=-\frac{1}{2}\phi(\square+m^2)\phi+j\phi$ then $$Z[j]=\int \mathcal{D}\phi e^{iS[\phi,j]}=Z[0]\exp \Big(-\frac{i}{2}\int d^4 x d^4y j(y) \Delta(x-y)j(x)\Big)$$ where $\Delta$ is the propagator, i.e. solves $-(\square +m^2)\Delta(x-y)=\delta(x-y)$.
 
OBE
@WDUK topology and geometry are used a lot in theoretical physics so you could learn about those. but you didn't specify your level. I would say vector calculus is one of the most important areas of math for learning physics.
 
So your $A^{-1}$ is $\Delta$ (or its analog in your context)
 
Peskin gives a cool discrete derivation of that, also in chapter 2 here desy.de/~jlouis/Vorlesungen/QFTII11/QFTIIscript.pdf
 
So I don't really understand the question @DanielSank
 
@DanielSank I'm not sure I can carefully explain it in your discretized case. In the continuous case I could (though I'd have to be a bit careful about what "kind" of Green's function we have here, exactly), but I can't say for sure if the relation between the propagator and the inverse diffusion operator carries flawlessly over.
Discretization has a nasty habit of breaking things when you least expect it :P
 
7:42 PM
@ACuriousMind Why can't you just go through the exact same derivation?
For the field theory version, you just do a shift by $-\int d^4y j(y)\Delta(x-y)$---I think I should be able to do the same, no?
 
@Danu The relation between the propagator and the inverse continuous diffusion operator relies crucially on the propagator being the Green's function of the diffusion operator. I don't see how it would mean in the discretized case to say that the propagator is the "Green's function", or what its relation to $A$ is.
@Danu What?
This isn't about deriving the value of that integral
It's about how the inverse operator $A^{-1}$ is related to the propagator.
 
@OBE i start uni next september so i imagine the first year is a lot of classical physics which i already know the math for.
beyond that i dunno what will be the next thing to learn
 
@ACuriousMind So what I was saying is that to obtain that relation in the case I know about, you can just do that shift on $\phi(x)$ and get the result
I probably didn't understand what's discretized about this variation
 
@Danu Uh...I still think you're explaining how to get the r.h.s of the formula Daniel wrote down in his question after "there's a known formula"
 
I don't care about discrete versus continuous.
I'm only doing discrete for now because I don't know the continuous case well (yet).
Also, green's functions work fine in discrete land.
 
7:51 PM
@ACuriousMind I probably don't understand the question.
I thought the question was sorta, how does $A^{-1}$ relate to $\Delta$
My answer was, they are the same
 
@DanielSank No doubt they do, but I have no clue
 
If I have $T|\phi \rangle = |J \rangle$, I can solve that with "Green's functions" whether those vectors are continuous or not.
I instead solve $T|G_i^e \rangle = |e_i \rangle$ where $|e_i\rangle$ is a set of basis vectors.
 
@DanielSank "However, I am given to believe that there is a link between $A^{-1}$ and the propagator $W$" if your question is - what is the link between the inverse of a differential and the propagator - then the answer is that they are the same thing.
At least for physicists
 
@Danu ...that's exactly what I am not sure about for the discrete case.
 
Then $$|\phi \rangle = \sum_i \langle e_i | J \rangle |G_i^e \rangle$$
 
7:53 PM
@ACuriousMind So why can't I just do a shift by the thing I wrote down to the field, given that propagators still work apparently
 
In quantum mechanics and quantum field theory, the propagator is a function that specifies the probability amplitude for a particle to travel from one place to another in a given time, or to travel with a certain energy and momentum. In Feynman diagrams, which serve to calculate the rate of collisions in quantum field theory, virtual particles contribute their propagator to the rate of the scattering event described by the respective diagram. These may also be viewed as the inverse of the wave operator appropriate to the particle, and are, therefore, often called (causal) Green's functions (called...
 
Doing that shift, all you need is that it's a propagator; the result just falls out immediately after some cancellations
 
@Danu You should probably write down what "shift" you're talking about explicitly because I have no idea what it has to do with anything.
 
Y U no write answers?
 
@ACuriousMind $\phi(x)\mapsto \phi(x)-\int d^4x j(y) \Delta(x-y)$ (I did write it down)
 
7:54 PM
Also, someone please acknowledge that the equation I wrote above is a discrete version Green's functions.
 
where $\Delta$ is defined such that if the Lagrangian is of the form $\phi A\phi$, then $A\Delta=\delta$
 
My issue is that I don't know how $W(x,t;x_i,t_i)$ is supposed to be a "Green's function" for $A$.
 
$W$ is a transition matrix element/probability/whatever.
 
In the continuous case, it's a Green's function in the sense that $(\partial_t - D\partial_x^2)W(x,t;x_i,t_i) = \delta(x-x_i)\delta(t-t_i)$
 
^and that's the (only) crucial thing in my proposed identification
agreed, @ACuriousMind?
 
7:58 PM
@Danu Yes - but how do you get it when you replace $\partial^2_x$ by its discretized version $A$?
 
yo I don't know shit
 
To me, that's the crux of the question here. Does that even make sense/hold?
 
@Semiclassical Do you happen to know about this? ^
(feel free to ignore if you don't feel like contributing)
 
@DanielSank I think it might well be the case that the relation exists in the continuous but not in the discrete case - in which case the phrasing of your question has led most people astray, see also its current comments
 

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