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12:00 AM
local extrema
 
where the induced metric and the subspace metric will not agree upto 1st order, I'm very sure
there's tight corners there
 
I mean take like $f(x)=x^2/\epsilon$ and look near $0$
the tangent plane will approximate the base
so the graph metric agrees to first order with the base metric near $0$
 
Yes, but I mean take $x = -\epsilon$ and $y = \epsilon$. Then the corresponding images on the graph have large distance in the induced metric compared to subspace metric
 
I agree, but you're saying this $\forall x,y$
If you add $\forall x,y$ such that $d_M(x,y)\ge\delta$ then it's fine
(for some $\delta$ that exists)
 
$d_M((-\epsilon, \epsilon^2), (\epsilon, \epsilon^2)) >> \|(-\epsilon, \epsilon^2) - (\epsilon, \epsilon^2)\|$
 
12:04 AM
@BalarkaSen again, my problem is when $x\to y$. I don't doubt that for points far away it's true
 
$-\epsilon$ and $\epsilon$ are far away??
Wut
 
far away compared to $x\to y$
on a length scale of say $\epsilon^\text{googol}$, the graph of $f$ is almost flat
 
Hmmm that is true
 
assuming $\epsilon<1$ ofc...
@BalarkaSen I believe the existence of such a wiggly thing only if $x$ and $y$ are not meant to be too close
 
@0celo7 Maybe this is right...
 
12:06 AM
what does the paper say exactly?
 
And as $\epsilon \to 0$, we could take $\delta$ closer and closer to $0$ of course...
 
right, it should be a usual "given $\epsilon>0$ there exists $\delta>0$ blah blah" thing
@BalarkaSen is this a variant of the statement of the ripple lemma?
 
What I am saying? A special case, I think, yes.
 
well what is this $R$ supposed to be, morally
ok, $\epsilon\ll 1\ll R$
you're saying $R=O(1/\epsilon)$
 
They said pick any given real numbers
I just picked $\epsilon$ and $1/\epsilon$
Seems like a fair choice
 
12:11 AM
oh ok R is given, right
@BalarkaSen While I'm thinking about this, symplectic boy, what is the uniform C^1 topology on the group of symplectomorphisms?
 
Is giving it the induced C^1 Whitney topology from Diff(M) a good idea?
Are symplectomorphisms stable under perturbation?
 
I don't know, if they said that then I'd be happy but the "uniform" bit is strange
the manifold isn't compact...
 
Yikes
 
@BalarkaSen no idea, this is unexpected symplectic stuff, I don't really know anything about it
@BalarkaSen so looking at this figure, I definitely don't think it proves what the authors think it does...
the points near the peaks are definitely not being moved far apart!!
 
Yeah that's strange
But maybe your reformulation is enough idk
 
12:17 AM
"Further we can choose this isotopy to finish with a diffeomorphism
which nowhere shrinks distances"
wot
ok I agree that this curve increases distances
 
Yeah that is fine
but the scaling up by R ...
 
what is it with symplectic topologists giving really vague proofs
 
that only works outside an nbhd of the crit points apparently....
lol
 
drawing a fucking curve is not a correct Riemannian geometry proof
 
page 2
They say it's induced from C^1(M, M)
 
12:20 AM
yeah, thanks
 
@0celo7 what I'm really confused about is how this proves the flattening lemma
I didn't even think much about rippling before you asked about it
 
@BalarkaSen The proof is written so strangely too
Clearly M can be replaced by S via an isotopy which moves points at most
A + 1
ω
. Further we can choose this isotopy to finish with a diffeomorphism
which nowhere shrinks distances, is fixed near {0, 1}, and which outside a given
neighbourhood of {0, 1} scales length up (measured in M ) by a constant scale
factor.
Is he saying one should modify $S$ more here?
 
I think he just wants S to be flat near 0 and 1
 
what does he mean by "scales length up" though??
that might be the key
how is he gonna scale lengths up by a constant factor without stretching the whole thing somehow
 
R*d(x, y), maybe? He says the same thing in a very vague way in the proof of flattening; check it out
page 437
bottom
 
12:25 AM
lmao fuck that proof
 
lololol
 
imagine turning this in as homework
 
"We do this and this and this and the embedding is now as flat as we please"
wtf
 
@BalarkaSen This encapsulates my beef with Russian math perfectly
 
it's written by british people lol
 
12:27 AM
intellectual traitors!
 
But!
"We are very grateful to both Yasha Eliashberg and the referee for comments
which have greatly improved the clarity of the proof of the ripple lemma."
 
hahaaaaaaaaaaaaaaaaaaaaaaaaaa
 
Yes, you did clarify that one very well
 
that's the sound of me having a stroke
 
get stroked
rip
 
12:28 AM
my stomach is growling and my dinner takes > 1 hour to prepare
gtg
hmu if you have an insight
 
for sure
 
I will find the error :)
 
bon apetite
looool
skeptic fuck
 
@BalarkaSen I don't like the statement of the ripple lemma. Try my modified version (no guarantees on its truth, but it's weaker than theirs so shrug) and see if the flattening proof goes through
 
I'll try that. Thanks
 
12:30 AM
@BalarkaSen "compressible" means that the function looks like a graph locally?
er
graph of a nice function locally
^ retarded
 
$M^n$, a submanifold of $Q^q \times \Bbb R^k$ is compressible if $M$ is nowhere tangent to the vertical $\Bbb R^k$
 
yeah I'm reading that
 
Or better, the projection map $M^n \to Q^q$ is an immersion
 
@BalarkaSen ah yes
 
ah ok
 
12:32 AM
always prefer things that can be stated in terms of analysis
 
I prefer some amount of rigor... unless rippling happens
 
ugh, the statement of the flattening lemma is already hard...
 
I can explain if you want. It's pictorial
 
@BalarkaSen if you're up when I'm done eating
I really need food, I don't think I had lunch :/
 
Do eat
 
1:06 AM
@BalarkaSen stage 1 is cooking
figure this out yet?
 
I have been reading their first paper. The ideas there are completely different
Want to hear about the flattening lemma?
 
go for it
 
Suppose $M^n$ is a compressible submanifold of $Q^q \times \Bbb R^k$, i.e., the projection map gives an immersion $M^n \to Q^q$.
Consider the Grassmannian $\text{Gr}_n(Q^q \times \Bbb R^k)$ of $n$-plane distributions on $Q^q \times \Bbb R^k$. We could look at the subspace $H$ of that Grassmannian consisting of "horizontal" $n$-plane bundles
Horizontal means sits inside the $q$-plane distribution $\pi^* TQ^q$ in $Q^q \times \Bbb R^k$, where $\pi$ is projection to the $Q$ factor.
Fix any neighborhood $U$ of this subspace $H$ in the Grassmannian. So elements of $U$ are $\epsilon$-horizontal $n$-plane distributions on $Q \times \Bbb R^k$
 
are these distributions in $T(Q\times R^k)$?
 
Yep
 
1:13 AM
ok
 
Tangent distrubutions
 
ok you keep saying on $Q \times R^k$ which could mean something different
(that's a vector bundle)
@BalarkaSen $\epsilon$-horizontal?
 
Ahhh I see, by on I mean at each point of Q x R^k you have a tangent plane stuck
 
@BalarkaSen ok, the language could also mean you have at each $q\in Q$ a plane of $R^k$ stuck
 
Yeah I realized
Didn't mean that
 
1:15 AM
ok, so epsilon horizontal means?
 
You could make that rigorous because you have a Riemannian metric... but there's no need to. Take it to definitionally mean that it's an element of $U$
 
is $Q$ kompakt?
and $M$
 
It's an element of a fixed neighborhood of $H \subset \text{Gr}_n(Q \times \Bbb R^k)$ consisting of horizontal $n$-plane distributions.
@0celo7 They don't seem to mention that
 
@BalarkaSen I am just wondering if elements of $U$ can get "arbitrarily close" to being vertical.
 
Oh $M$ is compact
@0celo7 I see
Well I mean Q x R^k is noncompact...
 
1:19 AM
yeah true
ok continue
 
Claim: You can produce a $C^0$-small isotopy $h^t$ of $M$ in $Q \times \Bbb R^k$ such that the tangent bundle of the final manifold $h^1(M)$ is restriction of an element of $U$ to $h^1(M)$.
So $Th^1(M)$ is $\epsilon$-horizontal, i.e.
Ah, should mention $ q\geq n + 1$
 
i.e. what??
 
I put the i.e. in the back of the statement instead of at the front.
:P
 
************** Indian English
 
lmao
that's a microaggression
i don't identify as an indian
i identify as jaden smith
 
1:27 AM
I see what the thing is saying, I think
yes, $q>n$ makes sense
well why not $q=n$
 
mhm
 
probably not enough "ripple room" ;)
 
ok so I see what the lemma is saying
have you figured out the ripple yet
@BalarkaSen two new D. Chappelle specials!
 
Not yet
@0celo7 Sounds delicious
 
1:53 AM
Angle of contact 180 degrees is same as 0 degrees?
Anyone?
 
@Fawad What do you mean "angle of contact" ?
Anyone know what do the squiggles above dQ and dW mean ?
 
impossible without more info
 
I assume Ocelo's talking to Fawad
 
@HsMjstyMstdn I'm talking to you
 
@0celo7 Oh sheez, alright. It was on a lab writeup, representation of the First Law of Thermodynamics. There is mention in the paragraph before it that neither the Q nor the W can be perfect differentials. Could that be related to the tildes ?
 
2:31 AM
Angle of contact between liquid and solid
 
Unless you're talking about something very specific with regards to directionality, I don't think there's going to be much of a difference between 0 and 180 degrees, Fawad. It just might mean that one is going left to right and the other vice versa.
 
3:08 AM
Huh?
0
Q: Converting radioactivity levels to radiation doses

Mark You stand in an environment where the air is 5% radon-222. How long does it take to absorb a lethal dose of radiation? I'm making the following simplifying assumptions: The only decays that matter are the beta decays of Pb-214 and Bi-214. The alpha decays can be ignored because skin and ...

I make it kilowats per cubic meter. Hundreds of kilowatts per cubic meter.
 
Yeah, the decay heat would be terrific
 
Anonymous
@HsMjstyMstdn Imperfect differentials
 
@Blue Thank you
Does the "imperfect" have any mathematical definition ? Or is it merely an expression of this differential not being perfect
 
Anonymous
 
@Blue Thanks
 
 
2 hours later…
5:21 AM
I am wondering what are Gauss transformations.
 
 
1 hour later…
6:41 AM
@Fawad the contact angle is measured through the liquid:
 
7:34 AM
mornin
Schwartz Witten has a pretty neat history of string theory
I didn't know of the dual mode theory
 
8:10 AM
Hi all... @dexterdev here. I have a question to ask here. Since this is a general chat room, I guess this is the best place for my issue.
I meant general chat room for physics
I recently posted a biophysics question in bio.SE and now I feel it should have been more appropriate in physics.SE
Can any of you guys suggest me what to do regarding my question : biology.stackexchange.com/questions/69321/…
2
Should I delete it and move to physics.SE ?
 
@dexterdev Hi Dexter. That's really physical chemistry and there isn't a physical chemistry SE so it doesn't fit anywhere :-)
I don't know anything about the ripple phase in cell membranes, but I did work as a physical chemist and I did study lamellar phases of surfactants.
And I'd be surprised if the ripple phase was as well defined as the diagram suggests. I would have guessed it was a rather poorly defined intermediate state between ordered and disordered.
I very much doubt it is a travelling wave like a ripple travelling along the membrane because I would guess the dampling is far too fast for a wave to propagate very far.
 
8:29 AM
@john-rennie Hi. As far as I understand ripple state is a meta stable state. Not really sure though. And I observed it in MD simulations. We have no clue why this happened as the temperature was above transition temperature where it should have been in fluid state. There must be some other reasons. Most probably it is not a travelling wave as you mentioned. But in literature sometimes ripple phase is explained along with "undulations".
I will catch you later
 
@JohnRennie Hm, I would have thought it might be okay here, but you know the topic better than I do. Of course it would need some explanation of relevant background information, for people who don't know about lipid membranes.
 
@Blue So, this is another 'general noise type' :) (presumably as a result of uncertainty intrinsic to the system). As a quantum Turing machine uses states (and is entirely equivalent to a classical Turing machine), it's not quite so clear cut as to whether this is taken into account or not. It probably depends how you model the problem or something.
Also remember that you can repeat simulations as many times as you like, so you can recreate the exact state using an ideal quantum simulation, but maybe that's what you're saying. More also: To properly look into this would be very interesting, but would require a fair bit of time delving into it (has anyone properly proven this claim, or is this just another thing that everyone takes for granted?)
 
@dexterdev One thing I'd definitely suggest is narrowing down your post to contain only one question. I'm not sure how much they care about that on Biology but here I would put it on hold as too broad simply because you're asking two questions - that's before even considering whether it's on topic.
 
Oh wait is the span of 2D vectors a plane?
 
8:53 AM
depends on the vectors
span of $\hat{i}$ and $2\hat{i}$ is a line.
(Namely, the x-axis)
 
Oh right...
Course
 
When is it true?
 
Just for all vectors which aren’t on the same line right?
I guess mathematically when $\lambda v_1\neq v_2$
 
For all $\lambda$. Yes.
What if you have more than 2 vectors? How would you state it mathematically, then?
 
It depends if you want a plane of like a cube right
 
8:57 AM
You're in $\Bbb R^2$.
 
So for a plane two would have to be in the same line with the other not
Oh yeah oops
Sorry I went 3D there.
 
Well, two need not be on the same line. Consider $\hat{i}, \hat{i}+\hat{j}, \hat{j}$.
The three span the whole of $\Bbb R^2$.
None of them are on the same line.
 
Ah right
 
So (1) state the property (2) write down the mathematical version
 
So to span the whole of R^2 there just need to be at least 2 vectors not on the same line?
 
8:59 AM
Good, yes.
 
Now mathematically...
 
There's a clean way to write this down without using quantifiers.
i.e., without saying "there exists" or "for all"
 
Hmmmm
Okay
 
Should I spoil it?
@0celo7 I got it. I understand the idea of the proof of flattening.
This ain't bad actually, but they should have been way more rigorous about it
 
Hi. Is there any possibility any of you knows some matlab? When a problem asks to simulate the change of particles inside a box as a function of time, is it ok to just define the appropriate vectors and make the plot or does it mean something else? Thanks.
 
9:10 AM
that's an old ass string theory paper
"particles coupled through imaginary coupling constants are usually referred to as "ghosts" and are according to our last axiom, highly undesirable in any theory"
Why does QFT have so many ghosts
 
@Slereah that paper is incredible
That's a famous article, I love how he sticks to Nambu-Goto through and through
I don't get what he's doing in I.70 to I.75 properly, kind of bluff with another perspective
My eyes keep glazing over when I try to find out about dual models and the links to qcd
 
9:31 AM
@DavidZ OK . I will do so.
 
"An additional property of the model emerged namely that the no-ghost theorem held only if the dimension of spacetime was smaller or equal to a critical dimension (26 in the conventional model)."
How strange!
Oh man it has pomerons
I completely forget what those are
 
@BalarkaSen Sorry I had to go to school assembly (yes We still have those ugh). I’ll think about it and if I can’t think of anything I’ll probabky end up asking you later... Thanks for your help, tho :)
 
Possible example of a pomeron
 
@CooperCape For sure
 
@DavidZ I will ask one question here. But can I post it in physics.SE now? I dont have necessary tags even here. :(
 
9:37 AM
"In early particle physics, the 'pomeron sector' was what is now called the 'closed string sector' while what was called the 'reggeon sector' is now the 'open string theory'."
 
@Slereah if you ever see section I.6 explained similarly but better elsewhere let me know
 
Hm, did Nambu really invent the point particle action in 1970?
Seems fairly late
Action of a point particle seems like an important thing to model from the beginning of GR
Even SR
Oh wait, Nambu only did the string action apparently
Who invented the point particle action
 
point particle action existed for ages
I think Loren(t?)z or someone back then did it
 
Do you mean Lorentz, Lorentz or Loren
 
Another paper like this is the GGRT paper they reference, but this one is more of an overview
 
9:51 AM
GGRT?
 
footnote on page 4
 
10:31 AM
@dexterdev If you can't find appropriate tags for your question, that's usually a sign the question is off topic.
 
The Lorentz–Lorenz equation, also known as the Clausius–Mossotti relation and Maxwell's formula, relates the refractive index of a substance to its polarizability. Named after Hendrik Antoon Lorentz and Ludvig Lorenz. The most general form of the Lorentz–Lorenz equation is n 2 − 1 n 2 +...
 
10:59 AM
why does string field theory have a trilinear form
The hell is $\langle \Psi, \Psi, \Psi\rangle$ supposed to mean
 
11:22 AM
@Slereah kong the savage?
@JohnRennie cool representation. So does it mean 0 degrees and 180 genres are different?
 
@DavidZ So where do you post biophysics usually involving lipids? bio.SE has tags, but physics.SE is more active! :(
 
@Slereah : FWIW, it is part of a Chern-Simons-like action.
 
@Fawad yes. 0º means the liquid perfectly wets the surface while 180º means the liquid doesn't wet the surface at all.
i.e. with a 0º contact angle the liquid spreads out on the surface to form a thin film. With a 180º contact angle the liquid rolls up to from a drop.
 
12:07 PM
Oh apparently it's $\langle \Sigma, \Psi_1 \star \Psi_2 \rangle = \langle \Sigma, \Psi_1, \Psi_2 \rangle$
for some operator $\star$
"An explicit description of the second-quantization of the light-cone string was given by Michio Kaku and Keiji Kikkawa."
First time I actually hear of Kaku on a real thing!
 
The guy came up with it
Unbelievable
 
it's pretty rare for a dude to be a pop science icon and actually known for your contribution to physics
Feynman and Hawking are probably the two good examples
 
Weinberg I'd say too
 
@JohnRennie thanks. Surface tension concept is tough for me :(
 
Bill Nye another /s
 
12:19 PM
Does Weinberg do pop science?
 
He writes popular articles, talks with Dawkins on video etc
Oh yeah he wrote 'the first 3 minutes' an awesome pop sci book I read ages ago
He's got a section in his 'intro' string book on 2nd quantization, one chapter in it on lightcone field theory, another chapter on brst field theory, there's an element of magic to the way he writes
as in 'insane path integral $\sim \delta$ function' and voila, answer!
 
breast field theory you say
 
Well he does know how to write for the masses...
 
@Slereah Neil deGrasse Tyson
 
(Lot of interpretations there :p)
 
12:26 PM
counterexample right in your face
 
@BalarkaSen Have you ever actually seen a paper by Tyson
I'm sure he wrote some
But I've never seen one
Let's see
Neil deGrasse Tyson (; born October 5, 1958) is an American astrophysicist, author, and science communicator. Since 1996, he has been the Frederick P. Rose Director of the Hayden Planetarium at the Rose Center for Earth and Space in New York City. The center is part of the American Museum of Natural History, where Tyson founded the Department of Astrophysics in 1997 and has been a research associate in the department since 2003. Born and raised in New York City, Tyson became interested in astronomy at the age of nine after a visit to the Hayden Planetarium. After graduating from the Bronx High...
it's all boring astrophysics
snooze
 
That part of his book comes after teichmuller spaces, moduli spaces, spinors and trees, superconformal ghosts, etc etc so yeah the guy is a maniac (in a good way)
 
Oh no
the worst ghosts
Does he use interuniversal Teichmuller universes
 
Maybe in his crazy advanced string book for all I know
 
physicists like moduli spaces
it's like their spirit animal
their pop dream
I have yet to learn the right definition of a moduli space
It's too komcplicated
 
12:35 PM
I don't know what a moduli space is
 
it's a space which parameterizes objects
 
that's pretty broad
Is it like a configuration space?
 
yeah it's a philosophy rather than a definition
exactly so
 
o
Is it exactly a configuration space?
 
every point corresponds to certain arrangement/configuration/object
@Slereah Not really
A configuration space is an example of a moduli space.
 
12:37 PM
what's a moduli space that isn't a configuration space
 
For him he takes the space of constant curvature metrics after quotienting out overcounting by diffeomorphisms to be the moduli space, and then, in spinor like fashion, if we instead throw away only diffeomorphisms connected to the identity, we get a Teichmuller space
 
@Slereah There's the moduli space of conformal structures on surface of genus $g$, eg.
 
Interactions are Riemann surfaces, RS's are conformally equivalent to constant curvature surfaces, etc
 
Although it's not a very interesting space if $g \geq 2$
It's just $\Bbb R^{6g - 6}$ I think
 
Still haven't gotten close to interacting string theory properly, that Scherk article gets you there pretty fast as an intro but I of course got side tracked
 
12:41 PM
It's not the moduli space that's interesting to be honest, it's how you model it
The "usual" model for moduli space of conformal structure on surfaces of genus $g \geq 2$ is to consider the length function on the induced hyperbolic metric on the surface
 
@bolbteppa something something sum over manifolds
 
Space of circles is a moduli space where the moduli speecifying different circles is the radius (= modulus) or something
Now we are just in 26 dimensions with insane spacetime 'circles' :p
 
Also, the topology matters. You want to understand how the objects change if you move around points in the moduli space
It's a cool reformulation of various changing shit
@Slereah Oh yeah the simplest example is of course projective spaces
 
They always say that Polyakov for non-string doesn't work but I'd like to see the actual proof of it sometimes
Like why membrane theory no works
 
I need to learn measure theory
 
12:49 PM
ask @0celo7
he'll tell u all about it
 
No doubt
 
What do you mean Polkakov for non-string doesn't work? In BBS they show Polyakov doesn't work with a cosmological constant term for strings and only works with a cosmological constant term for non-strings i.e. branes, maybe that?
 
I usually read that if you try to have 3D Polyakov theories (or more), you end up with divergences
Hence why there is no membrane theory or SHAPE theory
 

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