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10:00
@yuggib that's why our work load is like +50% :P
@yuggib na they're synergistic
definitely ^
@ShaVuklia but not +100%, that's the problem
you can do physics without learning math on the side. Most do that. Some choose to do both as well, which can be nice. So use that opportunity to the best
@ShaVuklia you clearly don't know them at a research level; they're miles apart ;-P
10:01
hm yea ok, each to their own
lol ofc not, i'm a first year student:d
well it depends what you want to do
a lot of math isn't properly defined for physics
or it's not rigorously used in almost all of physics
@ShaVuklia What math courses have you done till now?
leave her alone dude
@ShaVuklia I am saying that, as far as I know, focusing on one and then studying the other afterwards if needed yields better results
@yuggib we're scientists here, do you have any supporting evidence of reasonable sample size/
10:03
Depends on the person, yuggi
^
for those who have the capacity, they will be served well learning both simultanously
@Kenshin Well, I have a reasonable sample size in the community at the intersection between math and phys
analysis 1,2a,2b,3:P linear algebra 1, and 2-ish, algebra, basic math, latex/mathamtica, intro to probability theory, and maybe some that i forgot
and btw, what does it mean that you're a "scientist"? :-D
oh and graph theory
10:04
@yuggib we like the scientific method here
@ShaVuklia That's pretty nice. And what? You were TAUGHT latex and mathematica?
lol yea it was a 4-week course
@yuggib a scientist is one who uses the scientific method
like we had to program little stuff
it's a normal course, physicists have it too
not just mathematicians
Damn man, that's great. I had to learn it myself
10:06
yeah don't tell yuggib that you learn't programming as well
@Kenshin interesting, I would define scientist a professional working in a scientific field (with the scientific method, of course)
yea i'm glad i was introduced to it:P otherwise i would have never used it on my own
@yuggib yet many scientists in our history were not professionals working in a scientific field?
Yeah, the more you code, the easier you get with it. Like with all other things
@Kenshin if you say so..
I am looking forward to see your scientific contribution then
10:08
I don't publish my "contributions"
I work in finance dude
why so pretentious?
you said "we're scientist here", not me
yeah because to me a scientist is one who subscribes to the philosophy of the scientific method
rather than a job per se
I believe my definition is more historically accurate
I believe not
and then here you are asking for my "contribution" like wtf
@yuggib perhaps thsi wll help
"A scientist is a person engaging in a systematic activity to acquire knowledge that describes and predicts the natural world. In a more restricted sense, a scientist may refer to an individual who uses the scientific method.[1]"
A scientist is a person engaging in a systematic activity to acquire knowledge that describes and predicts the natural world. In a more restricted sense, a scientist may refer to an individual who uses the scientific method. The person may be an expert in one or more areas of science. The term scientist was coined by the theologian, philosopher and historian of science William Whewell. This article focuses on the more restricted use of the word. Scientists perform research toward a more comprehensive understanding of nature, including physical, mathematical and social realms. Philosophy is today...
The term scientist was coined by the theologian, philosopher and historian of science William Whewell.
I see nothing about "paid professional" here do you?
QED
Do you use a lot of math in finance?
10:20
Yes
@Avantgarde yeah but moreso alot of complex problem solving that may not necessarily involve maths
Mostly stochastic processes
so lots of probability and calculus?
lots of probability
stochastic calculus if you work in derivatives
interesting
10:21
@Kenshin it says systematic activity, that does not mean paid, but means that it produces some output
@yuggib no, activity doesn't require output, it merely requires activity
there is actually some links between financial theory and quantum mechanics
activity without output is still activity @yuggib, you should know this
yeah I know
Sometimes called by the name "quantum finances"
10:22
@Kenshin Honestly, that was a fair reaction to you calling him a troll. yuggib has first hand experience in switching between mathematics and physics and I can attest to his claim that if you try to hold physics to the standard of math while learning it you will make yourself very unhappy. Most of math is utterly useless for most of physics (and vice versa), the intersection where the two are reasonably close is very narrow. (cc @ShaVuklia )
@yuggib and output doesn't always have to be published
ty @ACuriousMind
I wonder the success rate (or probability :P) of quantum finance
what's the*
probably not very high
well some people make a fair living with short term financial models
Long term predictions are harder
long term predictions are actually easier
long term diversified stocks rise 8-9%
10:27
market crashes aren't too easy to predict
correct but they can happen in the short term too
but you can usually ride them out over the long term
like houses in the USA are already above what they were before the 2008 crash
or at least very close
When the site tells you one or more questions have changed, is there any way to find out which questions have changed? As it is, unless when you refresh the page you spot a new answer or score change you have no idea what to look for.
?
what site
10:43
a site called "stack exchange"
oh interesting
@Kenshin If you have the PSE home page open then you get periodic notifications that a question has changed (as well as notifications that a new question has been asked).
oh didn't know dat
Guys, the math chat is dead, so I'm hoping I could try here: Say we consider exponential decay $N(t)=N_0e^{-\lambda t}$. Now we can normalize this formula to convert it to a probability density function. We get $\lambda e^{-\lambda t}$, which is the probability density function of the exponential distribution.
This is all fine and well, but I don’t understand why we were converting to a probability density function in the first place, and not for instance to the distribution function? What is the ‘intuitive’ (or maybe even mathematical reasoning) for this?
by distribution function, do you mean cummulative distribution function?
10:47
yes
I much prefer working with probability densities than distribution functions
probability density is not very physically meaningful though
yes it is
well i've learned them as probabilities in my math course, but here in the case of exponential decay, i'm not sure in what way to think
i mean, i can read the answer, but i don't really see why they chose it this way
@Kenshin hm?
10:48
maybe i could think of it as the probability times $dt$ ?
I can't tell you why they chose that way @ShaVuklia, it depends on what they do with the density function
so if it's normalised, that gives us the fraction that we have
@ShaVuklia are you asking what is the meaning of a probability distribution function?
"Has anything precise been written about the Fukaya category and Lagrangian skeletons?"
Lagrangian skeletons???? D:
Very sorry to interrupt in an important discussion. I want to read and get a good hold on the topic of tensors. Can anyone refer a good book on it, perhaps one used in undergraduate level?
10:49
@WrichikBasu i would but not now due to your interruption
lol
same
like, i'm out of my flow now
@ShaVuklia suppose f(x) is a probability density function
(jk, i wouldn't know how to help ya sorry @Wrichick)
and say f(x) is the probabilyt density function of decay, and say x represents time
in my dictionary, probability distribution function <=> cumulative frequency
10:50
@ShaVuklia the probability density $P(x)dx$ gives us the probability that the system has a value of $x$ between $x$ and $x+dx$.
@ShaVuklia then this means that f(x)dx represents the probablity of decay over time dx
yea exactly, I get it
thanks guys
however
:37320876 Oops :-)
Are the group theorists around?
10:51
I don't need any more help. I've understood. I'll help myself as I've always done.
@ShaVuklia
@WrichikBasu iawa jokin
@ShaVuklia it is better in this case however to look at the probabilty density of survival (as opposed tod ecay)
lol @Wrichik that's life. we're all on our own:P
@Slereah you do groups, right?
>implying probabilities make sense in a non-frequentist sense
oh really? @Kenshin
10:52
yeah
Bayesians get out
if f(x) is probablity density of survival
@EmilioPisanty To some degree
then integral of f(x)dx is probability of survival over range of integration
then if youw ant probabilty of death/decay
it is probabilty of surving * probability of dying just after
this will hopefully make sense as you progress through the topic maybe
lol i'm only asking because of this mean time :P
10:53
just keep in mind, the probabilty of surviving from A to B and Bto C is the multiplicative
@Slereah I'm looking for some reference that classifies the subgroups of $U(1)\times U(1)$
but this doesn't work for dying
@ShaVuklia yeah these concepts are required to derive mean time
in principle shouldn't be too hard, right?
but it's turning out very hard to google
I'm obviously doing it wrong
okay but i get it @Kenshin because for dying, you first need to have lived
10:54
so you multiply
Wouldn't the subgroups of $U(1) \times U(1)$ just be the product of the subgroups of $U(1)$?
like probablity of dying at time between X and dX is probabilyty of surving to X then dying between X and dX
I think the subgroups of $U(1)$ are mostly gonna be discrete rotations
yes got it
Although there's also the... rational rotations, I think?
And irrational rotations
10:55
coolz
@Slereah I'm mostly looking for copies of $U(1)$ which "wind" multiple times
Those also form subgroups
@EmilioPisanty Sure, S^1 x S^1 is as a group isomorphic to R^2/Z^2.
Take a line with rational slope on R^2, and quotient down.
@BalarkaSen so I should just google for R^2/Z^2?
Or maybe it's just subsets of the type $\{(e^{ip\theta},e^{iq\theta}):\theta\in\mathbb R\}$ for $p,q\in \mathbb N$, and no more mystery?
oh well
@EmilioPisanty Those are the closed non-discrete subgroups. You still have to take account to the discrete ones (which are all isom to Z/m x Z/n)
There are also non-closed subgroups (which are all isom to R)
11:03
I'm looking for a graduate level solid state textbook with emphasis on mesoscopic physics, topics such as nanowires for example. Anyone here particularly fond of a specific book? I've had a look at Semiconductor Nanostructures by Thomas Ihn, which is nice and rather elaborate in that a lot of topics are covered, but quite superficial. I'd look for a little more detail perhaps.
@BalarkaSen Is that the rotations by $\theta \in \Bbb R \setminus \Bbb Q$
@Slereah a rotation is not a subgroup... it is quotient of a line of irrational slope on R^2, yes.
It's a real line which wraps around the torus a lot. Eg in Emilio's representation, plug in $p = 1$, $q = \sqrt{2}$.
@BalarkaSen Any clue of the name of the theorem relating sections of bundles and their retracts?
Having a hard time finding much
I think I just answered you that? The retraction info is totally irrelevant.
OR IS IT
Because I don't think it's actually a subbundle
11:12
Well, then what you told me to prove is wrong :P
Since I don't think $Gr(n,1)$ is a subspace of $O(n) \times Gr(n,1)$
It is just a retract of it
Hence you cannot form a subbundle of it
$Gr$ isn't a vector space, right?
Or the space of metrics, for that matter
Er, no, it isn't. What is it relevant?
Aren't subbundles supposed to be subspaces of a vector space?
... bundles are not vector spaces. I don't understand that comment.
I am usually confusing the bundle and the fiber :p
But you know what I mean
11:15
Fibers of a bundle is not usually a vector space. Those are vector bundles.
Yes
Don't subbundles only apply to vector bundles?
Which I do not believe the space of metric is
@Slereah Nah.
What is a subbundle then
is it just any bundle with a fiber that's a subset of another bundle's fiber?
Ah yes
Then I think it should be fine because I think you can define the subbundle with fiber $\{ I \} \times Gr(n,1)$
11:18
what is your fiber bundle?
(and what's the base space?)
No vector bundle
The original bundle is $\pi : S(n,k) \to M$, the bundle of symmetric matrices of signature $k$
With the identity $S(n,k) \approx O(n) \times Gr(n,k)$
Ok. And you're working with $k = 1$?
Well Steenrod's theorem is for arbitrary $k$, but $1$ is the one of interest for GR
@Slereah What is Gr(n, k)? Grassmannian of the tangent bundle of $M$?
11:21
Hey everybody can somebody explain me meaning of this mathematical ststement
f(x) - f(u) > -infinity
for more context
u is set of values for which f(x) is minimum/haslocal minimas
@Slereah The identity you're giving is a diffeomorphism of the total space S(n, k) with O(n) x Gr(n, k). In what sense is the latter a bundle over M?
There's some detail-thrashing I am worried about here.
If there's a diffeomorphism between the two fibers isn't there a diffeomorphism between the two bundles?
Diffeomorphism between two total spaces, you mean?
(1) in this case, I don't even know in what sense O(n) x Gr(n, k) is a bundle over M (what is the bundle map?) (2) no :P
6
Q: Nonisomorphic vector bundles with diffeomorphic total spaces

Balarka SenWhat's an example of two non-isomorphic vector bundles $E,F$ over the same base such that the total spaces $Total(E), Total(F)$ are homeomorphic? Assume that rank of these bundles is the same as dimension of the base manifold. (EDIT: Mike Miller brought up the excellent point that I need to loo...

11:26
Well Steenrod has more details but I'm in class right now :p
Like he spends a bit doing some witchcraft with the local trivializations
But I forget what
Alright, let me know if you end up looking at S-dawg or want to thrash detail
I'll try
But if there's a diffeomorphism $\psi$ between the fibers, wouldn't $\pi \circ \psi : E \to M$ be a fiber bundle of fiber $O \times Gr$?
or something, I'm not sure
I slept like 4 hours
user228700
YES! Coldplay is releasing their new EP at the end of June!
You do get a diffeomorphism S(n, k) = O(n) x Gr(n, k) between the total spaces, but when you compose that to get O(n) x Gr(n, k) as a bundle over M, is it clear what the fibers are? I am not so sure.
Gr(n, k) --> M may not be a subbundle of that.
(Which brings us back to your original worry)
I guess Steenrod probably has the details
Though I'm not gonna read steenrod tonight I think
Too tired
11:32
Hm, I still don't understand entirely... I see that if we normalise a function, we get a density function. But I don't see why it is the density function of the distribution that belongs to the function? Like, in my eyes, it's kind of random.
fair me neither
Assuming it is a bundle, tho
And there's a retraction to something like $\{ I \} \times Gr$
Which also forms a bundle
Does that mean that a section of $Gr$ implies a section of $S(n,k)$
If I x Gr/M is a subbundle of S(n, k)/M, you get a section. Totally, yup.
Well, that is some progress, at least
Thanks
(oh I think I see it. We then recognise it as the scalar of a density function)
11:34
I guess I also need to show that $Gr$ having a section is equivalent to the Euler characteristic thing, but that's a worry for another day
the hairy balls
You're onto nonzero sections too?
$Gr$ isn't a vector bundle, no?
I don't think it even has a zero
Yeah it isn't. So I am not sure I get what you mean by the Euler char thing
I hear that $Gr(n,1)$ is equivalent to nowhere vanishing vector fields
11:37
So that this would imply the hairy ball theorem wrt the metric
I guess I haven't thought about it. fiber bundles are too hard man
literally no structure
I'd say too much structure!
If I can just prove that theorem I will have done more work than every GR book ever written :p
you should write a new book then
That is what I am doing
#brekthru
11:39
Just a big block of GR theorems
gotcha
It ain't easy
Some are hard to track down
Also QFT stuff because I am a glutton for punishment
I just want to do semiclassical gravity :c
And yet I have to deal with functors and wavefront sets
I'm not even sure why they bother with wavefront sets since they have to renormalize anyway
the good products are all divergent
glad i dunno this stuff man
11:46
basically you just define the QFT on open sets of the spacetime and then piece them together
So that the QFT is the same if an open set is in the chronological future of another
that kind of stuff
the net of algebra, as it is called
and that regions that can't be joined by causal curves have operators that commute
so that everything is nice and local
The hard part comes when you have to renormalize everything
isee.png
Since there are several ways to renormalize everything
then you use the Wald big list of probably reasonable conditions for renormalization

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