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9:16 AM
I need some artistic advice
If I am to represent an Observer, what would be the ideal curve to do it
Straight line could work, but I need to convey "it could be in a non-flat spacetime and also it could be accelerated"
Probably some kind of bezier curve
 
9:34 AM
I think most kinds of curves would work for that
 
They will, but will they all look aesthetic
 
depends on the composition of the whole graphic :P
maybe the curvature of your observer line needs to form a golden ratio with something to be aesthetic
 
Rate my observer
Hard part is, how do you include mathjax on a svg
"Currently, the only way to include MathJax within an SVG diagram is through <foreignObject>."
 
10:02 AM
@Slereah $1.5e$ out of $2\pi$
 
Close enough
Making svg diagrams is time consuming
 
10:21 AM
Much better
 
 
1 hour later…
11:44 AM
Giving a read to "A Posteriori Estimates for Partial Differential Equations"
seems like what I was looking for
 
fqq
12:01 PM
@Slereah how are you making your SVGs? when I had to do it I just rendered latex to SVG (online I think) and pasted that into inkscape
not great
 
By hand mostly
Error estimation theory is such a mess
It's a giant pile of theorems
 
12:40 PM
and why do those weirdoes use $D$ for the gradient
 
12:53 PM
Writing SVG by hand can be time-consuming, but I enjoy it. :) Although I also like to semi-automate the process, by writing Python code that generates the SVG code. I don't often bother with that these days. Sage has made me a bit lazy. :) I mostly just create the diagram in Sage & let it render it to PNG or SVG, using matplotlib. OTOH, it is nice to do it by hand when you want to make compact SVGs that are relatively readable by humans.
BTW, you can post links to SVG here in chat & on the main site. You can't upload them to Imgur, but you can host them yourself on Github.
2
 
I mean I just write raw SVG on my articles
there's no file involved
 
Of course, the SVG code has to be well-behaved. It can use SVG or CSS animation techniques, but not JavaScript.
 
also it has <foreignobject> tags which I don't think will behave nicely here
 
Probably not.
I don't know what Sage does to handle MathJax in a SVG. I doubt it's compact, but it's most likely totally portable. Matplotlib embeds any fonts you use into your SVG...
 
My article on GR measurements is a giant mess
I need to edit it a bit I think
and more to the point, finish it
I just need to learn functional analysis first, a small task I'm sure
 
1:13 PM
Here's some Python-generated SVG. An equilateral pentagon inscribed in an ellipse.
Here's a temporary file of that. It should display for a while, until it gets kicked off the SageMathCell server.
 
Why do analysis people use $\Omega$ for subsets of $\mathbb{R}^n$
One of the least pleasant letter to write
 
Omega's easy. But I've been writing since I was a kid, doing electronics. I'm not fond of $\zeta$ or $\xi$, though. :)
You'd think xi would be easy, but I tend to mess up the relative sizes of the various loops, in my effort to make sure it doesn't look like $\varepsilon$, or something else.
 
I can write omega but it will be a little curvy
 
1:29 PM
Another annoying one is $\varpi$. It looks too much like $\bar\omega$
 
How often do you use the varpi
I'm not sure I've ever used it for a paper
 
I never use it myself, but I've seen it in maths papers. Eg, number theory stuff about frequency & sums of primes. IIRC.
 
 
1 hour later…
2:34 PM
Why is all the functional stuff about elliptic equations
You'd think hyperbolic equations would be also important
 
 
4 hours later…
7:02 PM
@ACuriousMind @Slereah Yo
Do you guys know this normal ordering crap
 
Sure
 
In Polchinski vol 1 page 239 there's some field $X(z, \overline{z})$ that breaks into the holomorphic and antiholomorphic part $X = X_L(z) + X_R(\overline{z})$ and the guy writes the vertex operator $V_{k_L, k_R}(z, \overline{z})$ as $: e^{i k_L X_L(z) + i k_R X_R(\overline{z})} :$
Can you explain me what this means?
 
now that's an advanced application of normal ordering :P
 
How do I normal order something defined just in a single hol-antihol coordinate pair
Not my question, a friend's
 
7:06 PM
that's CFT normal order, see physics.stackexchange.com/q/46975/50583
but see also physics.stackexchange.com/q/232705/50583 for Polchinski's idiosyncrasies
 
I'll relay this back to him and get back to you if he has queries
 
note that the "ordering" comes in here because the Taylor series expansion of the exponential contains arbitrary products of the two $X_{L/R}$, and physicists would probably describe the intention here as "just apply normal ordering order by order to the Taylor expansion"
@BalarkaSen I was going to ask what madness overtook you that you were reading string theory :P
 
oh sure
Age old excuse
 
@ACuriousMind OK now I want to understand: the exponential contains terms which are products of bunch of $X_L$, $X_R$'s. Pick a particular term, how do you normal order it? Polchinski's normal order is defined for a product of a pair of operators in $z_1, \bar{z}_1$ coordinates and $z_2, \bar{z}_2$ coordinates respectively
My question, not his
 
@BalarkaSen The $X_L(z)$ or $X_R(\bar z)$ are implicitly functions $X_L(z,\bar z)$, $X_R(z,\bar z)$
the notation just means that $\partial_{\bar z} X_L = 0$ and $\partial_z X_R = 0$
 
7:15 PM
OK, what is $:A(z, \bar{z}) B(z, \bar{z}) :$? I only understand $:A(z_1, \bar{z}_1) B(z_2, \bar{z}_2):$
 
ah, just normal order the thing on the right and then take $z_1 \to z_2$
 
But $:A(z_1, \bar{z}_1) B(z_2, \bar{z}_2): = A(z_1, \bar{z}_1) B(z_2, \bar{z}_2) + \eta^{\mu \nu} \log(|z_1 - z_2|)^2$
If you take that limit my guy goes to zero
Well, blows up
 
Wouldn't want your guy to blow up
 
@BalarkaSen well, the thing is that the non-ordered $A(z_1,\bar z_1)B(z_2,\bar z_2)$ is divergent, too
the normal order is (see the posts I linked) exactly the non-divergent part
 
Yeah I was reading that post, that's relevant
Shit seems to have essential singularities kek
 
7:23 PM
happens a lot in QFT!
 
well, it's the old "quantum fields are really distributions and you shouldn't be multiplying their values at a point" :P
but physics is like "but I want to" and so we are blessed with OPEs
 
Normal ordering is essentially baby's first renormalization
Remove divergences from the Hamiltonian
 
Can anyone help me understand this : The surface cur­rents are induced by the magnetization of the medium by the applied magnetic field and therefore depend on the magnetization M of the specimen.
The currents (because of electron movement in atoms and because of spin_ are always present in the material,
so what exactly is induced here?
induced means, that something which wasn't present, because of reason now becomes present
How exactly the external magnetic field induces something which was present all along?
The only thing I can understand is that the magnetic field, redirects the magnetic moment of the atoms, and that's it.
Is this what it;s meant with induced ?
 
@imbAF well, yes - and the "redirection" of the magnetic moment happens by the magnetic fields "inducing" the electron current to orient themselves differently
I think you got the idea, this is just using "induce" in a slightly looser sense that you seem to expect
 
yes it induces
redirection
not the current itself
@ACuriousMind I have one question for the dielectrics. As you know the following equation is true: $D = \epsilon_0 E + P$
is E in this case, the electric field inside the dieelctric ?
 
7:38 PM
oh no, I'm horrible with EM in media!
I don't want to say anything wrong about that
 
I see
 
@ACuriousMind If you want to make it relatable, it's related to the Gordon decomposition of the Dirac field, IIRC
 
In mathematical physics, the Gordon decomposition (named after Walter Gordon) of the Dirac current is a splitting of the charge or particle-number current into a part that arises from the motion of the center of mass of the particles and a part that arises from gradients of the spin density. It makes explicit use of the Dirac equation and so it applies only to "on-shell" solutions of the Dirac equation. == Original statement == For any solution ψ {\displaystyle \psi } of the massive Dirac equation, ( i...
 
is a particle divisible in infinity or it has an end, and if yes, which is that end ?
 
7:47 PM
whaaaat
 
your science fiction answer would be?
 
Also that
I'm not even sure what you mean
 
well
molecule - atom - proton - quark -??-??....
 
As far as we know for now quarks are elementary
 
hmmm
their gyromagnetic factor even in QED is not an exact number
but smth like 2.000 and a bunch of numbers
and even if that wasn't the case
 
7:50 PM
yeah but quantum effects are involved
 
nothing is build by itself, pretty paradoxical thing to be true
from*
Another question : what's the difference between a dead human and an alive one in terms of quantum mechanics ?
 
I think you can find the difference with just plain old classical mechanics
 
let's stick to the micro world tho
like for example, do they have both the same stored energy at rest?
 
why stick to the micro world
Might as well ask the difference between a bowl and a cup in terms of quantum mechanics
 
8:06 PM
hmm...primary change I can think of, nr of electrons rotating around the nucleus
should be an indicator of different materials?
+ studying the human life, you are trying to have a quantum explanation of life and death.
can't apply those concepts to a bowl and a cup
 
if you want a fairly boring definition, the most fundamental one I've read was that a living thing will draw Gibbs free energy from their environment
although of course that's not true of just living things, but that's a pretty basic difference between a living and dead organism
 
@imbAF reductionism doesn't work like that
a rectangular plate and a circular plate have no "quantum explanation" of their difference, the difference is purely classical and macroscopic
 
yes, if you would look it like that, only via a classical viewpoint you can talk about their shape (in this case).
 
likewise, a living and a (freshly) dead multicellular organism don't differ in their molecular makeup or anything like that, just their neurons have stopped firing/their blood has stopped flowing/whatever
 
But all I was trying to say is that, you can study human biology etc from an inanimate pov
 
8:16 PM
if you're doing biology you're pretty much by definition not studying inanimate systems
 
And find solutions about different deceases etc simply observing the micro world
 
I'm sure there's plenty of molecular differences between a live and dead cell, but those probably don't boil down to a simple QM argument, except maybe in that free energy idea
 
just because the molecules aren't "alive" when looking at molecular biophysics doesn't mean it's a science of "inanimate" things - it's the science of what happens inside of living things on a molecular level
 
Also "alive" is probably a bit hard to define here
I'm sure from a microscopic point of view, a lot of biological processes still happen after an organism dies
 
you can have many "biological" processes happening in a test tube
 
8:18 PM
just less and less so as time goes on
 
just...that doesn't explain anything about the difference between a living thing and a dead thing
 
Example : Someone who suffers from Diabetes, if you would speak as a biologist/ doctor you would recommend some medicine, which had some side effects. But you could look it this way: Someone who suffers from diabetes, on a quantum mechanical level has a certain "group" of subatomic particles on a lower amount then another body. So how do we try and change that, so this number can increase to the same levels, that a normal entity has them
Yeaah sloppy explanation, but can't do better
 
@imbAF but that's not the case - diabetes isn't caused by "subatomic particles"
 
not caused
 
it's a complex defect of the biological processes that normally process sugar
 
8:20 PM
but there is a difference in chemicals or w/e else in your body
you lack insulin for example
 
sure, insulin isn't subatomic
 
It's build from molecules,
everything is build from subatomic particles, at least what is considered as matter
 
insulin is a (very complex) molecule
 
yes
My idea is that there is no real difference between living things and objects. A bunch of particles arranged differently
in different quantity / different arrangement / different movement etc etc
 
I think you're confusing reductionism and monism here. Our modern understanding of living things is that they're just the same as everything else - made of matter, and everything they do is ultimately explainable by the same laws that govern all matter
that's monism
 
8:23 PM
and reductionism ?
 
but it doesn't imply that you can usefully reduce every explanation of how a thing (living or not) works to quantum mechanical or subatomic explanations
 
and what's the counter argument to that?
 
thats (a common caricature of) reductionism
@imbAF note the usefully
I'm not saying you can't in principle do this, but in practice the reductionist explanation will be so hopelessly overcomplicated and intractable you can't actually do anything with it
 
with our current level of understanding and intellect sure
50k years later, who knows
 
take classical thermodynamics: In principle the behaviour of a gas in a container and the pressure and so on is just a function of the position and momentum of each particle of the gas
 
8:26 PM
But I like monism, apparently. I think you can explain everything in a fundamental way, qm way, if that's what fundamental means in this case
 
but no one thinks about gases like that - they do statistical mechanics and talk about pressure, temperature and equilibrum instead
in principle the explanation in terms of the individual gas particles is valid, but it's not useful in practice
and not because we lack understanding or anything
 
so basically we study living things in a classical way, right ?
 
not sure that's a useful statement, either - a lot of molecular chemistry/physics is based on our understanding of QM
but we're not doing QM like "particle in a well QM" there
 
But when you treat a disease, you talk about what will it do to your body, not to your building particles
 
sure
 
8:28 PM
so it's classical
 
but our "study of living things" is very broad - someone treating a broken leg might not care about details of protein folding, but people studying a particular process inside our body (perhaps one causing a disease by making the wrong protein) might
 
which is an attempt of a non classical way of dealing with the problem
it simply goes up to a certain level of complexity
 
classical/quantum isn't a hard border
at the lowest level, everything is quantum, but describing everything in those terms gets too complicated quickly, so we do approximations
 
I am not disagreeing with anything you said.
 
there's a sliding scale of approximations between "fully classical physics" and "fully quantum physics"
 
8:31 PM
I just think, that if we would be able to study living things in such a detailed way, maybe we would be able to cure things that we currently cannot
and I can't prove that xD
 
I'm pretty sure modern medicine is not currently limited by our understanding of quantum physics :P
the body is a very complicated thing, and it's the interactions between its countless subsystems that are hard to understand, not the molecular physics at a single receptor or whatever
 
Do I have to take out the metabolic pathway diagram
 
Yes ofc
@Slereah pls no
 
(this perhaps wasn't true some decades ago, but it's true today - we can model proteins and understand how one molecule fits into another, etc)
 
This is biology
 
8:34 PM
was fun for me, but not a deep dive into the micro world
hence I had to choose physics :D
@ACuriousMind one more question
How can, in this reality, energy conversion and Bing bang be true simultaneously ?
 
what is the bing bang
is that that strip club in the Sopranos
 
assuming those are typos, see physics.stackexchange.com/q/10309/50583
 
:D
bigus bangus*
 
if they aren't typos, I won't be converted into a follower of Bing Bang via energy or any other means
 
lmaooo
big bang*
so ?
 
8:39 PM
so what?
I already posted a link to that same question on the main site
 
Ok, gonna inspect that
The time-translational invariance is broken, so via Noether's theorem, one doesn't expect a conserved quantity. Also, if one defines the "total" stress energy tensor as a variation of the action with respect to the metric tensor, it vanishes in GR because the metric tensor is dynamical and the variation has to vanish because it's an equation of motion (Einstein's equations).

If the space is asymptotically flat or AdS or similarly simple, a conservation law - for the ADM energy - may be revived.
I need multiple books to be able to understand this answer
 
the simple answer is "energy conservation is not quite as absolute a law as you've been led to believe" :P
 
good
because if the universe would have been here all along, that would have been the lamest revelation ever
for me
or maybe it is conserved
in this reality and fabric of space time
as an after affect of the big bang?
 
Noether's theorem relies on the boundary conditions of your spacetime manifold to be not too bad to work
Hence why it is not gonna work well next to a singularity
 
Ehhh Physics is tough. specially for some1 like me who needs to know the answer to every tiny single why.
 
8:50 PM
As Earman would put it
This is what happens
 
It gets tiresome after a while
 
naked sigularity?
 
9:03 PM
@Slereah could you help me with two illustrations and 2 explanations ?
 
 
2 hours later…
11:19 PM
0
Q: I'm asking something really obvious. Why is is marked as "unpublished personal theory"?

BarrierRemovalI'm asking a really obvious question; many people told me that they had this thought and question, so why is this marked as a personal theory (Is mass the source of space-time?)? It should be possible, in my opinion, to ask questions like, "Why are we sure that Earth is a sphere and not a flat su...

 
If I have a Grassmann field $\psi^\alpha$, can I just commute the symmetry group elements with eachother?
I.e. with suppressed indicies is $G_1 G_2 \psi_1 \psi_2 = G_2 G_1 \psi_1 \psi_2 = G_1 \psi_1 G_2 \psi_2 $?
Sorry I meant $G_1 G_2 \psi_1 \psi_2 = G_1\psi_1 G_2 \psi_2$
 
11:49 PM
Are classical fermionic fields Grassmann numbers?
 
@DIRAC1930 what does "fermionic" mean if not anticommuting, i.e. being Graßmann numbers?
 

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