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12:01 AM
@ACuriousMind In fact, I don't think that equation can even be true. For instance, if $f(x)=|x|$ (Euclidean norm), then $f^{-1}(1)$ is compact (it's a sphere) and since $L$ is linear it is continuous, so $L(f^{-1}(1))=\mathbb R^{m-n}$ is definitely wrong
 
12:12 AM
@ACuriousMind Some linear algebra musings: Let $V,W$ be vector spaces and $L:V\to W$ be linear. Conjecture: If $M\subset V$ (set theoretic subset, not linear subspace) and $L(M)=W$, then $M$ is a vector space.
Let $v,w\in V$ such that $L(v)=x,L(w)=y$. Then $\exists c\in V$ such that $L(c)=ax+by=L(av+bw)\implies c\cong av+bw$ $\mod\mathrm{ker}\,L$.
So, $M/\mathrm{ker}\,L$ is a vector space?
> Barack Hussein Obama II (reportedly born in Honolulu, Hawaii on August 4, 1961)
Conservapedia is AWESOME
Yeah, that's definitely not true that $M$ is a vector space.
But $M$ with the kernel modded out is definitely one.
 
 
3 hours later…
3:46 AM
> According to a NBC News poll, from August of 2014, Obama's approval rating was a dismal 40%[14], showing that six in ten Americans disapproved of his liberal policies. Given that liberals frequently engage in deceit, the actual approval ratings could be much lower.
Haha
 
@0celo7 lol
 
@user507974 it's not wrong
this is an awesome site
 
liberals are so much more annoying to engage in a debate with than non-religious conservatives
religious is like half-half
 
@user507974 why would engaging with a rational human being be annoying
 
@0celo7 which one is the rational?
 
3:53 AM
I'm probably in violation of some hate speech rule at my school right now
 
you know, im not gonna lie. I still dont know which is politically correct to say, that homosexuality is nature or nurture or both. Apparently even trying to answer that question is bigotted
i wouldnt be surprised if saying "i dont know" would be considered hate speech
 
How about "I don't care, I'm here for the lulz"
 
your bigotted for not caring for the plights of the homosexual you evil funny person
cuz now humor is problematic
and (i say with respect for the respectful parts of your institution) fuck your school if they cant take a joke
 
lol that site is not a joke
the dude who runs it is 100% cereal
 
i just dont have any respect for universities impinging on free speech
@0celo7 maybe, im about 50-50 on that
but in all seriousness, trying to engage in an intellectual debate with the average liberal is like watching a person without teeth try to eat popcorn
 
they literally cannot digest facts and change their opinion on something
 
> often condemn the God-given order of gender roles, as laid out in the Holy Bible
God dammit
Why are so many conservatives religious
 
@0celo7 traditionalism
 
still though that part is upplayed in the media
 
4:00 AM
> Quantum mechanics is predicted in several additional respects by the Biblical scientific foreknowledge.
Haha
 
what uni do you go to (or at least how conservative/liberal is it)
 
cf. e.g. my profile
 
im guessing its pretty conservative?
 
no
 
once you get urban university and southern its like flipping a coin
much more conservative probably than a california university
 
4:02 AM
we have an "office of diversity" that paints rainbows and shit on our sidewalks
and they tried to ban gender-specific pronouns but the governor told them to fuck off
(governor is technically the chair of the school board)
 
its pretty bad in CA
thank god im not at Berkeley though, wouldnt be able to stomach that probably
 
I can't stomach knowing OF Berkeley
 
haa
but yea, when you are on student apartments board you here so much of this diversity stuff it makes you sick of it
and I promise at least everyday i get one stupid email from some organization for LGBTQWTFOMGBBQ1337 whatever else
 
BBQ?
Wait, don't tell me
We'll probably get banned
 
I had the misfortune of hosting one of these diversity workshops in our complex so I peeked in on it
 
4:10 AM
what the hell is that
I know our RAs have to do that, one of my friends is an RA
 
Like 5 seconds after they finished defining what a micro-aggression is (which took WAY TOO LONG), and how it is a bad thing to generalize people and their experiences and say that just because someones x gender or race they will do something, they go on to say in the next slide how men all men harass women by talking to them because they want to bang them of something like that
 
I like harassing my gf and she likes being harassed
We're both terrible people
 
like im not kidding, i wrote this down somewhere it was so hypocritical and ironically done in the presentation
 
She enables my harassment
 
I decided to call him out on that one then after he says, you know, i didnt think of it like that maybe youre right but lets move on, some putz in the audience says that by definition it cant be applied to straight males because they come from a position of privilege
and they move on
 
4:14 AM
correct
I was once told blacks cannot be racist to whites because the people they are allegedly being racist against are in a position of power/privilege
 
@0celo7 its just sad to see how much they've perverted the language
ive always said the english language is used to conceal meaning (ty George Carlin for this great line)
 
I don't get Carlin
is he a liberal?
he might just be a massive misanthrope
 
or he was just here for the ride
but probably the misanthrope was part of it
i mean he said he loves individual people
he just understood how sickeningly destructive group think is
i mean for as much as liberals like to harp on being secularist feminism has kind of become another religion
and racial equality movements
and just like religions you cant hope to accomplish the goals but disagree on opinions, anything is excommunication worthy an offense
@0celo7 he was probably just an anti-neocon if you think about him politically
 
yeah he was isolationist
 
which ironically is functionally a libertarian, though he would not get along with a lot of them
 
user116211
4:24 AM
> $$v_x= \frac{dx}{dt}~~v_y= \frac{dy}{dt}~~v_z=\frac{dz}{dt}~~v_t=\frac{dt}{dt}=1 $$ doesn't make a four-vector $(v_t,v_x,v_y,v_z)$ because $dt$ in the denominator is unsymmetric.
 
hmm?
 
user116211
Okay, this is what Feynman said; but I didn't get what he meant by unsymmetric. Can anyone tell me what he meant by that?
 
@MAFIA36790 do $t\mapsto -t$ and see what happens
(I think)
(not sure exactly what the context is)
 
user116211
@0celo7 He wanted to show it is not that easy to evaluate the time-component of four vector.
 
uhhhh
 
user116211
4:27 AM
@0celo7 Velocity would get reversed, but $v_t$ would be $1\;.$ So?
 
@MAFIA36790 well how is he defining 4-vector?
 
user116211
> We define a four vector as a set of the four quantities $a_t,a_x,a_y$ and $a_z,$ which transform like $t,x,y$ and $z$ when we change to a moving coordinate system.
 
ah, ok, and how do these coordinates transform
 
user116211
@0celo7 Lorentz transformation, of course.
 
and that is?
 
user116211
4:32 AM
$$t'~=~ \frac{t-vx}{\sqrt{1-v^2}}~~~ y'~=~y\\ x'~=~ \frac{x-vt}{\sqrt{1-v^2}}~~~z'~=~z$$
 
so how does $(v_t,v_x)$ transform under that transformation
 
user116211
He chose units where $c~=~ 1\;.$
 
@MAFIA36790 i know
 
user116211
$$v_t'~=~ \frac{1}{\sqrt{1-v^2}}~~~ v_x'~=~ \frac{v_x}{\sqrt{1-v^2}}$$
 
@MAFIA36790 wait, where are you reading this?
 
user116211
4:37 AM
@0celo7 Feynman Lectures Vol 2.
 
where exactly
 
user116211
Electrodynamics in Relativistic Notation, page 374
 
user116211
Wait, lemme give the CalTech site:
 
I found it
@MAFIA36790 ah, this is what he means
(I think, I don't know any relativity)
What he means is that
$$(\frac{dx}{dt},\frac{dt}{dt})$$
it does NOT become
$$(\frac{dx'}{dt'},\frac{dt'}{dt'})$$
I think, lol
This is not very clear
 
user116211
Oh! that's what he meant by unsymmetry?
 
4:42 AM
I think so...
 
user116211
thanks @0celo7; I owe you a treat.
 
Let's see if I have any relativity books on my shelf
just one
@MAFIA36790 Mr. @JohnRennie will know for sure
I don't know any physics I'm afraid
 
@0celo7 Just maths and engineering? :-)
 
@JohnRennie Not even that
I can pick my nose successfully
 
Well it's 05:45 here, and I'm not even awake enough to scratch my bum, let alone pick my nose.
I'd probably end up scratching my nose and picking my bum
 
4:46 AM
depending on how clean it is, that might be an enjoyable experience
 
Ugh, I feel sick now
@MAFIA36790: what were you asking?
 
user116211
23 mins ago, by MAFIA36790
> $$v_x= \frac{dx}{dt}~~v_y= \frac{dy}{dt}~~v_z=\frac{dz}{dt}~~v_t=\frac{dt}{dt}=1 $$ doesn't make a four-vector $(v_t,v_x,v_y,v_z)$ because $dt$ in the denominator is unsymmetric.
 
user116211
22 mins ago, by MAFIA36790
Okay, this is what Feynman said; but I didn't get what he meant by unsymmetric. Can anyone tell me what he meant by that?
 
I suspect he just means that the $t$ coordinate is being treated differently to the other three.
 
user116211
Sometimes, he uses ambiguous words.
 
4:49 AM
In the four velocity all four coordinates are differentiated wrt $\tau$ so this is symmetric.
 
@JohnRennie Poor you
 
user116211
I think Feynman wanted to mean what 0celot told above.
 
@JohnRennie I like how in the mathematical literature $t$ is the proper time
 
@0celo7 that seems an odd convention. What do they use to denote coordinate time?
 
@JohnRennie they don't?
coordinate free
 
4:53 AM
Ah, yes. One day I must get comfortable with the coordinate free approach.
 
@JohnRennie I can help you
@JohnRennie and if I needed to use coordinates I would use $s$ for proper time
 
I suppose having both proper time and proper distance is a historical artefact, though to be fair both have their uses.
 
proper distance?
that's a physicist thing
never shows up in math
no respectable mathperson writes $\mathrm ds^2$
@JohnRennie I might use $l$ too
 
Is it really necessary to $\mathrm d$ everywhere? @MAFIA36790 even goes back and edits it into my old posts :-) Does anyone really care?
 
@JohnRennie no
when I need to do a lot of them I won't bother
see above
 
user116211
4:58 AM
@JohnRennie If you don't like them, you can rollback; I've told you numerous times ;)
 
@MAFIA36790 I don't care either way. I'm just surprised people care enough to type the extra eight characters :-)
 
user116211
Actually $\rm d$ represents operator while $d$ is a variable.
 
user116211
@JohnRennie Nay, just write once and copy-paste it ;P
 
using $d$ as a variable is still poor form
when I see $d$ I think of a topological metric
 
user116211
5:02 AM
Hello.
 
yo
Which volume of the Feynman lectures are you reading?
 
user116211
Now, I'm reading 2.
 
@JohnRennie when are you going to read a "mathematically sophisticated" GR book and what will it be
 
@0celo7 the trouble is that to the extent I'm a physicist at all I'm a phenomenologist not a theoretician.
I'm interested in what GR can tell me about the world, but less interest in the details of the theory itself.
I went through a brief phase of being really interested in maths for its own sake at about your age, but these days I see it as just a tool
 
5:07 AM
What was your specialty in Physical Chemistry?
 
milk @Sᴋᴜʟʟᴘᴇᴛʀᴏʟ
@JohnRennie what % milk do you drink
 
Computational chemistry. I did my final year project on distributed multipole analysis for the decsription of scattering.
@0celo7 full fat.
 
@JohnRennie wow
 
If you look at the calorific content then the difference between full fat and skimmed is small in absolute terms unless you drink gallons of the stuff.
 
5:09 AM
oh really
 
And skimmed milk leaves your coffee a chaming babyshit brown colour.
 
I am in need of milk
I will investigate this
 
user116211
Oh, BTW, I drink coffee without milk.
 
@JohnRennie coffee?
@MAFIA36790 You're a man. Without sugar, too?
 
user116211
@0celo7 actually, sugar-free.
 
5:10 AM
Coffee is an essential part of my wake-up strategy
 
@JohnRennie Damn, you sound like an old man
 
user116211
@0celo7 old nerd man.
 
@Sᴋᴜʟʟᴘᴇᴛʀᴏʟ less interesting than you might think. It was mostly calculating the electron density and fitting it with a multipoles not centred at the centre of the molecule. It turned out not to be very useful. At least I don't know of anyone who used it in real calculations.
@MAFIA36790 correct on all three counts :-)
 
user116211
aha!
 
But you forgot to add devastatingly witty and handsome :-)
 
user116211
5:13 AM
damn
 
user116211
BTW, who is the oldest at PSE?
 
user116211
Annav, I suppose?
 
This chat is a brilliant way to avoid doing any real work :-)
 
user116211
Hmmm.
 
6:03 AM
@JohnRennie: But one still can't make T=0, though... and we really don't know what other phase transitions can occur at even lower temperature, even if we have the effective theory on some scale. Some cosmological models even assume that there is an infinite hierarchy of scales "at the bottom". — CuriousOne 43 mins ago
But then, what does it mean for something to have below zero kelvin that is not negative kelvin (i.e. not the type where $\frac{\partial E}{\partial S} < 0$)...?
 
6:27 AM
https://www.sciencedaily.com/releases/2016/06/160602151842.htm

Magnetic materials just got a lot more interesting
 
6:43 AM
@0celo7 Constructive does not mean finitist
 
user116211
@yuggib: o/
 
and even finitists admit an infinite number of naturals/primes
\o
 
7:02 AM
@JohnRennie the saddest thing was in the comments for the Einstein ring was in the comments, someone was like "Astrology is great. Keep it coming"
 
user116211
@user507974 This is unfortunate. They don't seem to understand the difference between astronomy and that damn shit.
 
Just start throwing scorpions at people everytime they mix up the two
watch the problem disappear in a big %$*#ing hurry
 
My preferred way to deal with noisy arguments (noisy as in the parties refuse to settle into a compromise or solution), intensify the anger of both sides so that, eventually like matter and antimatter, they annihilate each other in a bang

Bam! Problem solved as the noise is silenced and tranquility is restored
 
7:15 AM
o/ @Secret
 
Obivously that's a last resort...
Most people (even cranks I have met so far) are reasonable enough to not go into mad anger without losing focus on the problem
 
@Secret worst case scenario you get to watch a fight break out
 
Well... then I will quickly leave the place (or if it is really serious, start rallying the bystanders when in a safe situation and call the police)
 
@user507974 you couldn't make it up :-)
 
In other news, I also read NewScientist, but I also read Sciencedaily and Scientific American
these 3 sources are how I maintain my broadness in the science despite going deeper like typical researchers do
One thing to be aware about Sciencedaily, though, is that for some physics articles, they like to make eye catching but inaccurate titles. Other times, they like to recycle some previously reported research
A guide to Sciencedaily is that for each week it often has some focus on some genre. E.g. in one of the weeks you will see most articles talking about e.g. skymions, other days they wil be talking about Zika virus
 
7:37 AM
@Secret i really dont like newscientist
at least a few sections of it really show off their donors interests
 
user116211
The only thing I enjoy is Lumo's Reference Frame.
 
@Secret all your boson are belong to us?
 
lol
 
 
1 hour later…
9:44 AM
Hi everyone! Why the photon field does not couple to the axial current in the massless fermion limit? Just consider the dirac lagrangian with m=0. This is chiral symmetric $U(1)_L \times U(1)_R$. Then, we have two currents. The sum of the currents $J_L + J_R = J_V$ is the vector current that is coupled to the photon when we gauge the theory. But, we have another current that is the axial one $J_A = J_L - J_R$. Why this current does not couple in the gauged theory?
 
you forgot your $
A massless fermion field is basically two fields
In effect, it does couple to the "axial current"
 
how do you show this?
 
But of course, the Maxwell equation is still gonna be $\approx j_R + j_L$
If you want a gauge theory that couples to the axial current, you need a different gauge
 
It seems strange because QED conserve parity and an axial current transforms with a minus sign
 
$\psi(x) \rightarrow e^{i\gamma^5 \alpha(x)} \psi(x)$
That's the axial gauge
 
9:49 AM
try to be more specific
what you wrote is an axial transformation
the axial gauge should be a condition on the photon field
that is $A_\mu^3=0$
 
Well that's a gauge transformation
You won't couple to the EM field with the regular $U(1)$ gauge
 
@0celo7 Why not? It is nowhere claimed that $T_x M$ is a vector subspace.
 
Hey @ACuriousMind
 
Heyhey
 
Tell me
Do you know what mathematically the difference is between a commuting spinor field and an anticommuting one
 
9:54 AM
@0celo7 I think you're implicitly supposed to choose $L$ surjective.
 
Is a commuting spinor field still a Clifford/Grassman algebra
 
@Slereah Sure, it's the same classical field
 
Whaaaat
 
The commuting/anti-commuting property is something you impose on its quantization
 
I thought the Grassman algebra was specifically to make it anticommuting in the quantum limit
I mean I'm talking about path integral quantization here
There is no CCR defined
 
9:56 AM
Oh...let me perhaps think a bit more, then
 
I have this suspiscion that if we have a commuting spinor field, then maybe it's not a part of a Grassman algebra, and maybe not a Clifford one???
But that's all vague hunches
 
Wait, when even is a "commuting spinor field"?
 
Yeah that's part of what I wonder
 
You can't have a spinor field that commutes and have a well-defined quantum theory, that's the whole reason people turned to the anti-commutator, no?
 
Well you can have a commuting spinor field in QFT
It just has a few problems
 
9:59 AM
what you can have is anticommuting scalars (e.g. FP ghosts)
 
No lower bound of the Hamiltonian and break of causality
Also I think the path integral diverges
But I'm interested more classically here
 
@Slereah That's a called "not having a well-defined quantum theory" :P
 
I'm wondering the exact link between the spin group, the clifford algebra and the grassman algebra
Like is it mandatory that the spin group's rep is associated to a clifford algebra?
 
@Slereah Classically, it's just a Grassmann-even valued field transforming as a spinor, then
 
But if it's Grassman, isn't it anticommuting
 
10:01 AM
@Slereah Grassmann-even.
 
Like are we not imposing anticommutation because of the quantum theory
 
The anticommuting things are Grassmann-odd.
 
Hm
 
@Slereah No. E.g. the Weyl spinors are not reps of the Clifford algebra
It's the Dirac spinor (and only the Dirac spinor) that is obtained as the unique irreducible representation of the Clifford algebra
 
Is there a direct link between the clifford algebra and the grassman algebra, too?
Isn't the clifford algebra a type of grassman algebra (or one of its subalgebra)
 
10:05 AM
You can see the Clifford algebra as a deformation of the Grassmann algebra (the Grassmann algebra is a Clifford algebra for a "metric" that's just zero)
I don't think the appearance of the Clifford algebra for the Dirac spinor and the Grassmann algebra for anticommuting things in general are related, though
@FrancescoS The gauge field always couples exactly to the current that is conserved by the global version of the gauged symmetry.
 
Know what couples to the axial current tho?
Torsion.
 
The axial current is not conserved anymore as soon as you gauge the vector symmetry due to the ABJ anomaly, so if you try to gauge the axial symmetry, you get an inconsistent theory (gauged symmetries must not be anomalous)
 
why do spinors have so many groups and algebras involved
"Clifford (1878) introduced his ‘geometric algebras’ as a generalization of Grassmann algebras, complex numbers and quaternions"
good ol' Clifford
Was he related to Clifford the big red dog
Are there any use of spinors in physics outside of fermions, by the way
Oh wait
you can do GR with spinors
 
10:30 AM
@ACuriousMind But in the massless limit, the global symmetry group is $U(1)_V \times U(1)_A$ not? So there are two independent currents which are conserved
 
@FrancescoS No, there aren't. Gauging the vector symmetry makes the axial symmetry anomalous.
That is, you are not allowed to make both of these symmetries gauge symmetries because gauge symmetries must not be anomalous (anomalous global symmetries are fine)
 
Anomalies can be cool, tho
The scale anomaly lets you violate the ANEC!
 
Well, but an anomalous gauge symmetry is just doomed because the unphysical d.o.f. no longer decouple
 
So I'm trying to show that Robert Low's spacetime does indeed feature compactly generated CTCs without any closed null geodesics
But this involved the most awful thing
BASIC GEOMETRY
It's just showing that lines will not intersect!
 
10:51 AM
It is quite odd that his solution is so simple
It's your basic Minkowski surgery wormhole, but
rotated 90°
 
11:11 AM
"Formally currents behave like (Schwartz) distributions on a space of differential forms. In a geometric setting, they can represent integration over a submanifold, generalizing the Dirac delta function, or more generally even directional derivatives of delta functions (multipoles) spread out along subsets of M."
lolwut, multipole is directional derivative of Delta function? You can define delta functions on more than a point, but on a submanifold???
 
11:30 AM
@ACuriousMind It actually is
@ACuriousMind Mike Miller helped me figure it out
It's retarded
for some reason "$f^{-1}(y)$ corresponds, under $F$, to the hyperplane $\{y\}\times\mathbb R^{m-n}$" does NOT mean $F(f^{-1}(y))=\{y\}\times\mathbb R^{m-n}$ like any reasonable person would think
rather, it means $F^{-1}(\{y\}\times\mathbb R^{m-n})=f^{-1}(y)$
 
12:06 PM
@ACuriousMind Ok perfect, I understood that was the axial anomaly the problem. Thanks
 
12:21 PM
@ACuriousMind so, the local axial transformation is not a symmetry of the gauged theory, right?
Because the gauge field transforms only under the vectorial gauge U(1); right?
 
@FrancescoS No, it is not
 
@ACuriousMind it is not right or it is right what I said?
eheh :)
 
It's correct that the local axial transformation is not a symmetry.
The global one is, but only classically - it's anomalous in the quantum theory.
 
ook
yes, i know
perfect. thank you
 
What is the axial anomaly, btw
What is not symmetric in the quantum theory by an axial gauge transformation
 
12:28 PM
@Slereah In the path integral formalism, it's the fermionic measure that is not invariant.
 
Dang it, Grassman algebra again!
 
So, the global axial transformation in quantum theory is again not a symmetry?
 
In the canonical formalism, you just find that a certain triangle diagram that corresponds to the axial current conservation doesn't vanish
 
I could check I suppose
My Peskin is right next to my keyboard
But Stephani is on top
And my wrist is sprained
So it's hard to lift it
 
weak
 

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