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03:00
if a vector space is of more than one dimension, then by definition it has orthogonality between it's members.
user143442
that why you are so upset
By definition?
@theDoctor do you know what orthogonal means?
What definitions are you using, man
03:00
i use orthogonal in two senses: 1) the sense of independent variables.
user143442
dont be like that, be the nice guy
and 2) the sense of completely unrelated dimensions. like geometry to whole numbers.
look
everything in math has a precise definition
you must use the definitions we all use
a 3d vector has 3 elements (x,y,z} that can be projected into the space R^3.
or communication will be difficult
user143442
03:02
I cant start MathJax :(
that's another thing - often vector spaces are conflated with coordinate vector spaces. not every vector is a coordinate tuple.
Well, you can use other definitions, but you should communicate that beforehand
fucken mechanics question its like 10 pages of algebra
what the hell lol
what other possible sense is there of a vector if not a tuple?
user143442
but every finite dimension vector space may be seen as a coordinate vector space
03:03
yes #user
user143442
just use the coefficients of its representation in the basis
@theDoctor a vector is just any element of a vector space. you can look up "vector space"
@anon so you're using the term vector in an abstract, non-numerical sense of a force?
user143442
infinite dimension vector spaces are studied in functional analysis
see any abstract algebra text
03:04
What is "the basis" @user ?
I'm FINALLY BACK! :)
user143442
the basis you pick
How has everyone been?
user143442
now tell me how to use MathJax please
user143442
03:05
I can't install it
has anyone considered negative dimensional spaces? \
@theDoctor vector spaces are still numerical in the sense that you multiply vectors by scalars (often numbers, specifically), but the physics interpretation of force is just a physics interpretation. like I said, look up vector space.
or imaginary spaces?
you mean space with complex-number dimension
answer: sort-of
ah I see @anon. you are using non-euclidian sense of abstract vectors.
user143442
03:06
i think $\emptyset$ has dimension $-\infty$
@anon yes.
@theDoctor non-euclidean is not the word you should be using - that refers to curved spaces in geometry.
thats what I'm working on
no, non-euclidean can mean more than a curved space which still implies a 2d field.
user143442
start ChatJax
^^drag this^^ to your bookmark bar or right click on it to add it as a bookmark.
03:07
@ForeverMozart sweet.
user143442
I can't drag it :S
user143442
don't be a drag just be a queen
Right click it?
user143442
i also did that but it doesnt show the option add it as a bookmark
03:09
@ForeverMozart Mentaculus?
@user, what do you mean you can't drag it?
@Krijn yes ;)
user143442
I see the little circle of forbidden
which is to say non-euclidean is more than just Reinmann spaces, for exmample
fractional dimensions are considered in fractal geometry, supervector spaces can have negative dimensions, and one can consider formal linear combinations of vector spaces and extend dim linearly so it can take (say) complex values (or alternatively interpret dimension as the character of a representation evaluated at id, then interpret chi(g) for different g as "twisted" dimension)
user143442
03:10
Antonio tu hablas español
user143442
dime en español
No, sorry, only English :)
user143442
malinchista
I know a little though from growing up in California.
non, mais je parle Francais
user143442
03:11
moi aussi
@anon:
user143442
mais un peu
i like the new idea of "twisted" dimension.
Je ne parle pas francais bien
@user, right click on the "start chatjax" link, then click copy link address
03:12
as if defining a curved line space as opposed to a curved surface.
i will publish that
then create a new bookmark with the title "start chatjax" and paste what you copied as the location
user143442
ya
user143442
no se que diablos es bookmark
user143442
in spanish
user143442
03:13
es marcadores?
user143442
how do i create a new bookmark? :(
These things are bookmarks: i.imgur.com/FVeHZ7w.png
user143442
you are from chihuahua
user143442
i catched you
haha no, I want to buy this for a friend: themountain.com/chihuahua-face-t-shirt
03:15
God, thats horrendous
I know, it's great
user143442
it's horrendous
in chrome, to create a new bookmark, right click up there, then click "add page..."
I don't know what it would be in spanish
user143442
agregar pagina
Did it work?
user143442
03:17
nope
user143442
i dont know where to click
are you using chrome?
user143442
my bookmark bar is different
user143442
yes
click anywhere that is gray
right-click*
03:19
i'm not sure i buy into the idea of negative dimensions being related to supervectors, though.
user143442
here's my bookmark bar
oh no
thanks, that was a good laugh ;)
user143442
?
anyway, i think math has gotten very confused about the notion of domains, because of how physics seems to relate to the abstraction of number itself.
03:21
try right-clicking to the right of where it says "Importar marcadores ahora..."
in the blank gray space
and people use R like they do Z, even though they are completely different domains.
user143442
yess :D
user143442
thank you so much
no problem
user143442
y de nada por la risa jaja
03:24
oh sry, i thought this was a math chatroom./
It is, but the discussion is tiresom
And not fruitful
you telling me you've thought of dimensions beyond integer?
user143442
@theDoctor are you the one of your picture?
@user sure.
i can tell you practical applications of negative and imaginary dimensions.
03:26
yes, son.
lol
you people need some guidance.
but you speak in too much generality
you have been getting lost in the byways of math.
You say that like it's a bad thing
03:28
yes that is true
it's not too much, you just need to understand domain theory.
wtf is domain theory??
but consider this, if there was not some imposed structure on math, it wouldn't exist.
most mathematicians are platonists and would disagree
domain theory relates different dimensions of number, like dimensions specifies different fields of geometry.
03:30
dimension theory is an area of topology
but I never heard of domain theory
Domain theory is a branch of mathematics that studies special kinds of partially ordered sets (posets) commonly called domains. Consequently, domain theory can be considered as a branch of order theory. The field has major applications in computer science, where it is used to specify denotational semantics, especially for functional programming languages. Domain theory formalizes the intuitive ideas of approximation and convergence in a very general way and has close relations to topology. An alternative important approach to denotational semantics in computer science is that of metric spaces....
that definition is too constrained. R is not an ordered set nor a poset.
yes it is!!!
R gets an order by being related to Z, after that.....
Your obsession with $\mathbb{R}$ being somehow completely misunderstood by all mathematicians here is really...
03:31
i know, hard to believe.
but that's because they've been dealing with abstract albebraic expressions, never the real numbers.
functions, in otherwods
otherwords.
99% of mathematicians will disagree with you
Yep, I'm out. Good luck @ForeverMozart!
get those bastards on the line.
03:32
2 hours ago, by anon
you're very trolly/cranky.
and we'll talk some real (sic) math.
@Krijn well it was sortof entertaining
i'm not trolling, sometimes a premise is wrong.
Does anyone ever feel like they're right and everyone else is wrong?
or, let's say, not wrong, which make shiver's down Chaitin's back, but less pleasing.
03:33
You are either trolling, or you should take a class in Real Analysis
haha, real analysis is a joke.
it's like a subject taken by Cthulhlu.
to try to understand the world above water.
Chaitin is way out on the fringe, and does not actually contribute to mathematics.
after only ever knowing the world within water.
he is messing up your mind I think
haha, what counts as a contribution to you?
no, he's is awesome. if you want to understand yourself some philosophy of math, check it out.
if you just want to get lost in the byways of math, well, there's SE.
03:35
he talks a lot about philosophy
but he doesn't actually do math
EXACTLY! where number has been for quite awhile.
you are partially right, depending on whether you consider compsci math.
out of curiosity, what is your native language @theDoctor ?
computational math, math.
native language is English.
i know, i don't talk with the semantics of most math, but that's because i've gotten a new religion, so to speak.
it's like
Pythagoras.
On a different note, would anyone be willing to try out a small userscript for Math.SE I've been working on? I'm trying to add live previews for when you post a comment.
@theDoctor I think you should collaborate with John Gabriel. I would be interested in the result.
03:39
hmm, will look into that....
Hahaha I am tempted in a question that involves physics to say by maple and some algebra we get the following
go ahead
its like 1 page equation
I am not gonna go through hrs of algebra to get solution lol
there has to be more to the problem than just algebra
yeah ofcoz
setuping it up and stuff
it involves Lagrangian mechanics
but I am just lazy to do the algebra i already did the steps that goes through the algebra
if your interested the question reads as follows
03:43
@anon: I am both intrigued and repelled by John Gabriel page you gave me.
A point particles moves in space under the influence of a force derivable from a generalized potential of the form $U(r,v) = V(r) + \sigma . L$ Find components of the force in both cartesian coordinates and polar and show that the components are related to each other
lol wtf is that john gabriel @anon
@anon: I suppose you'd need to define volume for me to agree. But either way the lack of a group "SSp(2) = S^7" is annoying in a number of ways; first that S^7 isn't actually a group; second that if there was one, then we (should) have H^*(BSSp(2)) = Z[x] where x is in dimension 8, but this is entirely impossible
(analagous to H^*(BSU(2)) = Z[x], x degree 4; H^*(BSO(2)) = Z[x], x degree 2)
dunno cohomology or classifying spaces, so, I have no idea what's annoying about that
but I believe you
it annoys me personally i suppose
@KarimMansour someone who tried evangelizing on m.se a while back but to no avail.
03:48
@anon: it's just annoying in the same way that any pattern breaking is
Do $\Bbb F$-automorphisms of $\Bbb F(\alpha)$ take roots of $\alpha$ to other roots of the minimal polynomial of $\alpha$ and fix everything in $\Bbb F$?
yes
try to prove it
Which means that any $\Bbb F$-automorphism of $\Bbb F(\alpha)$ couldn't possibably take an element to the root of the minimal polynomial of $\alpha$ unless it was already a root of the minmial polynomial of $\alpha$
(well, being an F-auto by definition entails fixing F pointwise)
right
03:53
Good good good, yes I will prove this thanks
04:25
Hey just @anon is it true that intersection of all maximal subgroups of Z is actually isomorphic to $Z_2$ right ?
just making sure
the maximal subgroups of Z are pZ for primes p, and their intersection is {0} (under +, that's the trivial group)
yeah pZ
is maximal subgroup of Z
oh yeah
Z doesn't have any (nontrivial) finite subgroups, so in particular none iso to Z2
I see
I have a question can we have uncountable group and a countable maximal subgroup of it ?
no
If G is uncountable and H<G is countable, then picking any g in G\H we have that <H,g> is countable and bigger than H.
04:30
oh I see
why is it bigger than H ?
@anon hello.
1 sec thinking
@KarimMansour I mean H is proper in <H,g>
@BenLim hey
@anon wassup?
04:32
yeah makes sense
@BenLim thinking about accidental spin groups
I see. I've been busy with grad school crap lately so haven't been on here or MO
no worries
which grad school you go to @BenLim
@KarimMansour Stanford.
04:34
nice
Ayo @anon
You in the mood for some Dedekind domains?
meh
You in the mood to help me?
by grad school crap you mean teaching incompetent calculus students?
:)
@ForeverMozart I mean handling three weekly assignments and being a CA
04:39
I'm wondering why every prime ideal being maximal in a dedekind domain implies that the CRT holds on powers of prime ideals
what is a CA?
@ForeverMozart course assistant
@anon In particular, I don't see why powers of prime ideals are pairwise coprime.
@Anthony Ok. you agree that if p,q are prime ideals, then p +q = (1) yea?
I actually don't know the proof of this either.
But I know it's true.
04:40
@Anthony So we just need to show the following. Suppose, I,J are such that I + J = (1). Then for all $n$, $I^n + J^n = (1)$.
I mean couldn't the powers be different?
Ok sure if you'd like
@Anthony This is easy enough. Suppose $I^n + J^m \neq A$. Then we can find a maximal ideal $m$ with $I^n + J^m$. Then in particular $I^n \subseteq m$ and $J^m \subseteq m$. Hence $I \subseteq m$ and $J \subseteq m$, so that $I+ J \subseteq m$, contradicting $I+ J = (1)$.
@BenLim Thanks. Give me a moment will I try to read this. I guess there's a bigger problem though, because I can't think of why the sum of two prime ideals should be (1).
@Anthony Well you know in this case that your prime ideals are maximal.
If $P$ is prime ($\Rightarrow$ maximal in dedekind domains) $P\subseteq I$ implies $I=P$ or $I=(1)$. Apply this with $P,Q\subseteq P+Q$ with $P\ne Q$ prime ideals and you get $P+Q=(1)$.
04:46
Oh, d'oh.
Thanks, ya'll.
@BenLim Why does $I^n\subseteq m$ imply $I\subseteq m$?
Choose $x \in I$, Then $x^n \in I \subseteq m$, so $x^n \in m$. Now $m$ is maximal, hence prime so that $x \in m$.
lol
Thanks.
#lovealuffi
Huy
Huy
ok
Huy
Huy
04:52
Julian you are surely interested in studying functional analysis with me
nice to see you again @Huy
??
Huy
Huy
I'm looking for someone to study with so I have more motivation
Huy
Huy
are you working on a lot of other things currently?
not really
Huy
Huy
04:53
you have enough time?
you mean now?
Huy
Huy
in general
I mean ya
i guess
Huy
Huy
what's your background? sorry I don't quite remember @Julian
Real Analysis, Topology, Category Theory (current), Alg. Top. (trying :/), Abstract Alg
Huy
Huy
04:58
well if it doesn't interfere with your studies I'd be happy if you'd join me
I would love to join
What does studying functional analysis entail here?
Huy
Huy
@JulianRachman: dl.dropboxusercontent.com/u/2098511/FAnotes.pdf I'm using my professor's draft of his textbook. I'm currently revising some measure theory in the appendix and going through chapters 2-4. I want to focus on chapters 10-11 eventually, so after 4 I'll check what else I need to start with 10. You can diverge of course.
@GaloisintheField: What do you mean by that?
Ok
I will take a look and start reading
I mean what functional analysis are you studying, but I guess your link answers that
Huy
Huy
05:00
@JulianRachman: I think it's quite nicely written and has lots of motivation, but maybe that's just me.
Ok. So what do you what me to go over so that we can discuss?
Huy
Huy
idk, I've never done this before, online :D
Should you be posting his textbook draft online?
Huy
Huy
@GaloisintheField: The link is available from his website.
I didn't mean to offend(if I did)
05:01
What to email me?
Why go straight to 10?
Huy
Huy
@JulianRachman: Maybe you can go through (parts of) chapter 2 and next time we meet you tell me where you're at? I'll have a bit of a head start but I'm sure you'll catch up quickly.
I think I am going to start with motivation so that I get a feel
Ok sounds good
Huy
Huy
@GaloisintheField: Because I'm mostly interested in the spectral theory of self-adj unbounded ops
05:03
@Huy Fair enough, and you already know chapter 5 and 6?
Huy
Huy
I've seen most of the results already during my studies, but it was a while ago, which is why I will go through it again, just not as much in detail as with the other things.
TBH, I have not learned anything about fundamental analysis so it is good for me to start from some motivation then go from there
Huy
Huy
@JulianRachman: I really like his explanations on ODEs and PDEs, made me understand those two topics much more in a very short time even though I've been dealing with such equations for years.
Ok Ill take a look and see if I will be on the same page with you
did you print this pdf or did you just go digital
Huy
Huy
I always read digitally
but that's just my personal preference
05:06
Oh ok
Maybe you should make another chat room for this? I think I would be interested in following your progress
lol I like to write on stuff
Huy
Huy
@JulianRachman: I usually just write it down and then have hundreds of pages of notes :P
Cool. @Huy can you make the room/
(and maybe participate when I have time
05:08
Do you go notebook or loose leaf paper?
^ the debate :/
I throw out all of my notes
@GaloisintheField lol
05:45
Hey @GaloisintheField, I'm sorry I couldn't answer last time
Did you manage to solve what you were doing?
 
2 hours later…
08:15
@Krijn I don't know, I am mainly just working through understanding stuff
08:28
@GaloisintheField Cool username.
@robjohn here is an amazing question I created last night. Proving that (in a very easy way)
$$\int _0^1\int _0^1\int _0^1\log \left(x^2+y^2+z^2-x y-x z-y z\right) \ dx \ dy \ dz=\frac{1}{3} \left(\sqrt{3} \pi -11\right).$$
Sure, here is also a basic thing to prove for beginners: Prove that $$x^2+y^2+z^2-x y-x z-y z\ge0$$
08:43
@Chris'ssistheartist $\frac92\left(\frac{x^2+y^2+z^2}3\right)-\frac92\left(\frac{x+y+z}3\right)^2$ and Jensen's Inequality
@robjohn Yeah. However, the left side, after multiplying by $2$, can be viewed as a sum of squares.
@BalarkaSen So, what are you up to currently?
@Tobias I was mostly preparing for exams (you know, high-school stuff) the whole week. Finally, I'm all free.
@BalarkaSen Cool. How did it go?
Pretty good.
Now that I am free, I am planning to do some multivariable calculus, relearn commutative algebra and revise algebraic topology, putting a stress on calculus since I have ignored it for so long and now I can't study the cool stuffs (differential topology) without it.
@TobiasKildetoft What are you upto?
08:53
@BalarkaSen Updating/rewriting my research statement. I need to start applying for jobs again soon
Ah. Must be a boring work, updating research statements.
@BalarkaSen Yeah, though it was interesting to read the old one again and see what I needed to change
I have had to remove several things that I have not actually thought about at all since writing the old one (making them perhaps not the best inclusions back then)
09:45
please in $(\mathbb{R},|.|)$ how to prove that $\overset{\circ}{Q}=\emptyset$ ?
10:11
er, @robjohn. I think you have a dinosaur on your keyboard.
@robjohn :
111
Q: How can I keep my cat off my keyboard?

Tom MedleyThis is a common scenario when typing: When the family assembled for Sunday dinner, With their minds made up that they wouldn't get thinner On Argentine joint, potato^DR&FTGYB`kuhadrggoy867rt98wouth4bfgdhjlkhdsfghhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhhf This happens beca...

10:24
Has anyone in here studied transformational plane geometry ?
@robjohn can you help me please
@Hippalectryon
@Chris'ssistheartist o/
o/
$$\int _0^1\int _0^1\int _0^1\log \left(x^2+y^2+z^2-x y-x z-y z\right) \ dx \ dy \ dz=\frac{1}{3} \left(\sqrt{3} \pi -11\right).$$
@Hippalectryon ^^^
 
1 hour later…
Huy
Huy
11:44
@DanielFischer: My prof asked me whether I knew the "invariant measure" and I hesitated and he said "it's just $1/y^2$". Of course I know the Riemannian metric, but that's not the same, is it? He then told me that what's interesting is that $1/y^2$ isn't invariant on tangent vectors, but the standard one is. Do you know what he means by this "invariant measure on $\mathbb{H}^2$"? Invariant under what? Möbius transformations?
12:09
@Huy Invariant under automorphisms, typically. In this case, those would be Möbius transformations (and maybe compositions with reflection in the $y$-axis, depends on whether you are also interested in orientation-reversing maps or not), since the orientation-preserving isometries are Möbius transformations.
I assume you're doing this in differential geometry, since you speak of a Riemannian metric, so the pertinent concept of automorphism is isometry, and you're using the standard constant-curvature metric. In the context of (locally compact) topological groups, "invariant measure" would refer to "the" Haar measure.
Huy
Huy
@DanielFischer: but does that rule out Haar measure, since hyperbolic plane isn't a topological group?
I'm a bit puzzled because usually he is very correct with his wording but "measure" didn't quite make any sense for me
(he asked specifically about "the invariant measure on H^2")
12:32
@Huy Well, $H^2$ is homeomorphic to $\mathbb{R}^2$, so you could make it a topological group. I just mentioned Haar measures to have another example of what "invariant measure" can mean. It's not so different, since in both cases you have a bunch group of maps, and you want the measure invariant under those maps.
Huy
Huy
@DanielFischer: and then would the Haar measure look anything at all like $1/y^2$?
@Huy I don't think so. Under the obvious homeomorphism, you'd get $\frac{1}{y}\,dx\,dy$. I don't see how you could make it a topological group in a way that $1/y^2$ becomes the density of a Haar measure. And by the way, saying $1/y^2$ is the measure is an abuse of terminology. It's the density of the invariant measure with respect to the Lebesgue measure on $\mathbb{R}\times (0,+\infty)$.
Huy
Huy
@DanielFischer: and can you make anything out of his statement that "$1/y^2$ isn't invariant for tangent vectors, but the standard one is"?
@Huy Not really. What "standard one"?
Huy
Huy
@DanielFischer: I think he said "x+y" which is why I thought he meant the Euclidean metric (and then the 1/y^2 also made more sense to me, but then again I didn't understand why he'd say measure)
12:43
Can't make heads nor tails from it. I can't even fathom what "invariant for tangent vectors" could mean in connection with a measure.
13:14
Can we do operations on matrices that have elements from different fields? How much can we extend that?(my terminology is a bad attemt to translate greek math to english math)
I mean we can multiply the matrices $A\in\Bbb Q^{m\times n},\; B\in\Bbb R^{n\times r}$
@UserX How do you define multiplication of two elements of $F$ and $F'$, two different fields?
It works for $\Bbb R$ and $\Bbb Q$ because $\Bbb Q$ is a subfield of $\Bbb R$
Do the corresponding fields have to be connected with one being a subfield to the other and the matrix we get is in the largest field? That's what makes sense for me.
If one of the field is subfield of the other, it is clear how to multiply elements of the two fields, thus you can define multiplication of the matrices with values from those fields too.
That's what I thought @BalarkaSen. Are there any other circumstances where it may be possible?
Huy
Huy
@DanielFischer: I'll just ask him asap. :P
13:23
@UserX Depends on what you mean. If $F$ is a field, $F'$ is another field, there is generally no natural way to define a multiplication between elements of $F$ and elements of $F'$ unless you're inside some bigger field already. That is, $F$ and $F'$ must be subfields of some bigger field $F''$
Otherwise, you have to define for me what multiplication even means.
@Vrouvrou note that $(\sqrt2+\mathbb{Q})\cap\mathbb{Q}=\emptyset$ and since $\mathbb{Q}$ is dense, so is $\sqrt2+\mathbb{Q}$. What can you say about $\overline{\mathbb{Q}^C}$?
Dumb question:

If I take $f(x) + \langle g(x)\rangle$ and $g(x)$ is degree $n$, why do I always get a degree $\leq n-1$ remainder?
Huy
Huy
@DanielFischer: I got an answer by email (German): "Das invariante Mass ist 1/y^2 dxdy (glauben sie mir nichts und überprüfen Sie dies). Eigentlich ist die obere Halbebene keine Lie Gruppe sondern bloss ein homogener Raum (genauer G/K=SL_2(R)/SO_(R)). Aber andererseits kann man die Gruppe der obere Dreicksmatrizen (fast) mit der oberen Halbebene identifizieren, denn diese wirken einfach transitiv (wenn man entweder nur positive Zahlen auf der Diagonale zulässt oder durch -I dividiert).
Doch bei dieser Identifizierung muss man mit dem y-Parameter aufpassen, vielleicht liegt hier die Verwirr
13:42
lol!
3
(it was originally posted in the homotopy theory chat. it's hilarious, so i thought i might link it here too)
@Huy I think they mean that when you identify the half-plane with the group of triangular matrices (modulo $\{\pm I\}$) then $1/y^2\,dx\,dy$ becomes the Haar measure. Sounds credible. I still have no idea what the tangent vectors have to do with anything.
Huy
Huy
@DanielFischer: I'll try to work it out in detail until tomorrow and see if I can understand what is meant with the tangent vectors.
14:05
@GaloisintheField polynomial division
14:48
@Huy SL(2,R) acts transitively by mobius transformations on the upper half plane. with the poincare metric dxdy/y^2, they are the orientation-preserving isometries (and we get the poincare upper half plane model of hyperbolic geometry). the stabilizer of the point i is SO(2,R), so we can identify SL(2,R)/SO(2,R) with it. Integrating over a region in SL(2,R)/SO(2,R) amounts to pulling the region and function back to SL(2,R) and integrating with Haar measure I think.
Also SL(2,R) acts (sharply) transitively on the bundle of unit tangent vectors, making H=SL(2,R)/SO(2,R) an isotropic manifold (the space "looks the same" while standing at any point looking in any direction).
(Disclaimer: I can't read a lick of german, I'm just guessing what's being said based on the symbols, and Daniel's response.)
You didn't say what question the email was an answer to.
15:10
ah, there is discussion between you and Daniel further up. I see.
err, I meant (dx^2+dy^2)/y^2 is the Poincare metric, which induces the volume form dxdy/y^2, which agrees with the Haar measure pushed from SL(2,R) down to SL(2,R)/SO(2,R)=H^2.
also not sure what is meant by "invariant measure for tangent vectors"
15:29
Does anyone have any idea what this quote (from V.I. Arnol'd) is referring to?
Sir Michael Atiyah once told me that he was always delighted by the way Petrovskii dealt with algebraic geometry in his works on PDEs. One of these, the paper on the lacunas of hyperbolic PDEs, was later rewritten by Atiyah, Bott, and Gårding in modern terminology in two long papers in Acta Mathematica. It is a far-reaching generalization of the well-known fact of the impossibility of acoustic communication in the even-dimensional spaces (for instance, in the “plane” world), while in our three-
(when talking about the work of Petrovskii)

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