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00:42
facepalm
Just realized that $\sin^2x+\cos^2x=1$ trivially follows from the definition of the unit circle
It's called the "Pythagorean identity" for a reason
 
4 hours later…
04:38
@Danu Allegedly physicists write $e^{iX}$ (with an extraneous $i$) for $\exp(X)=\sum_{n=0}^\infty X^n/n!$. Is this true?
@arctictern where did you see that?
04:56
@arctictern O_o
05:38
@Mike Do the sequences $z \mapsto nz$ (or $z \mapsto z^n$) converge to as maps $\Bbb CP^1 \to \Bbb CP^1$?
I imagine the answer is nothing
SL_2(\Bbb R) is connected but open.
@arctictern Yes, that is correct.
I am pretty sure that this derives from the following combination of facts: (i) physicists like to work with $\mathfrak{su}(n)$ (ii) physicists like to work with Hermitian (as opposed to skew-Hermitian) matrices.
Hermitian matrices represent observables in quantum mechanics, in case you didn't know.
If one wants to describe a particle with spin 1/2, for instance, $\mathfrak{su}(2)$ is useful.
for me hermitian matrices are a linearized version of projective geometry: every hermitian matrix is uniquely a linear combination of projection maps (onto pairwise orthogonal subspaces). the other kind, skew-hermitian matrices, are a linearized version of the oriented grassmanian manifold Gr(2,n): every skew-hermitian matrices is uniquely a convex linear combination of right-angle plane rotations (with respect to mutually orthogonal planes).
(this is in the real case of course) (convex meaning nonnegative scalars)
Right. So projective stuff is related to quantum mechanics (since in quantum mechanics the states of a system are described by rays in a Hilbert space)!
05:47
mmhmm. so Baez tells me.
Is it in the octonion paper? Or another one?
@Mike According to a comment here math.stackexchange.com/questions/633567/… The complex automorphisms of a complex torus are always $GL_n(\Bbb C)$ with the automorphisms of the lattice. In particular in the standard lattice this will contain $GL_n(\Bbb Z)$ as a subgroup (I really mean n here not 2n) which will be an infinite countable group.
I think it's in the octonion paper, and in one of <this week's finds>
Right. Baez always seemed to be right on the border between math and physics.
Until he switched to really different stuff :D
06:13
V= set of all solutions of the differential equations $y'' + by' + cy = 0$ where b,c are real numbers satifying $y(0) = y(1)$ ,then dimension of V is ?
like there are two solutions to the above homogeneous ODE and other possible Linear combination of them are also solutions to the ODE and hence dimension is 2 as the two solutions generate the other solutions and they span the whole set of solutions but then
when we apply initial conditions $y(0) = y(1)$ does that affect the dimension ?
I think that the initial conditions narrow down the solution set to one solution... so the dimension is ???
I would say that a point has no dimension...
but I thought of like this - the two solutions may cross each other
like x axis and y axis
still they are the basis of whole RxR plane
it is not a point
they are the solutions!
are there two solutions?
06:19
It is a 2nd order ODE
If $y$ is a solution then so is $ay$, where $a$ is a scalar. (It still satisfies the initial conditions.)
Oh, then the dimension is $1$
@BAYMAX If you put enough initial conditions on a DE, it will only have one solution (or even no solutions).
yeah
@BAYMAX maybe you meant two linearly independent solutions, which is not present here...
please do not use ambiguous terms
06:21
so if in the question I will not mention the initial condition will the dimension still be one ?
ok will take care @LeakyNun
no
without initial conditions, the solution space is spanned by exp(rt) and exp(st), where r and s are solutions to x^2+bx+c=0.
(well, assuming x^2+bx+c is separable, otherwise the answer needs amending)
So if one specifies initial conditions then it is mandatory that the dimension will reduce ?
like it is intuitive
Can anyone figure out what this means?
they are certain characters of a cartoon ?
every1 has a face
those are letters, not people
06:26
I tend to believe that it is graffiti
oh
Maximum of {$x+y : (x,y) \in \bar{B}(0,1)$}
What is $\bar{B}$?
presumably closed ball of radius 1 centered at 0
I know that maximum of $f(x,y)$ always occurs on the boundary of $B$
Closure of $B(0,1)$
oh
The maximum is the supremum which is $\sqrt2$
06:38
:37317958 yes there is a maximum
cuz the ball is closed
well, don't just give the answer :P
just draw a graph
yes, x+y is the length of the projection of (x,y) onto the line y=x.
projection of a point onto a line
?
yes
(orthogonal projection)
that's for geometric intuition
you can just use calculus or whatever to prove it
polar coordinates -> maximize cos(theta)+sin(theta), derivatives, blah
any other intuition to this lik any other approach
06:51
I gave you the most straightforward "student do what she's told" approach - use calculus. the most fundamental intuition is geometric, which is the orthogonal projection one.
any line x+y=c is perpendicular to y=x, and they intersect at (c/2,c/2). thus, x+y is the signed length of the orthogonal projection of the point (x,y) onto the line y=x. if you draw a closed circle, you want to find the point on the circle that is as far along in the direction of that axis as possible, which is (1/sqrt2,1/sqrt2) just by looking at the circle (and using pythagorean theorem or trig to get coordinates).
@PVAL Good point with the torus example. It makes me want to restrict to simply connected a little.
thanks@arctictern
 
3 hours later…
09:34
Hi there ! I had a very simple question in Lagrangian multiplier ...
When defining new $u_1$ and $u_2$ in Lagrangian relaxation :

$$u_1=\max(0,u_1-tL_1),u_2=\max(0,u_2-tL_2)$$

what is $t$ ? How much is it ?
 
1 hour later…
11:06
Hi. I got a $K^2 \times K^2$ matrix $A$ that consists of $K^2$ block matrices of size $K\times K$, each of which is symmetric and with real entries from [0,1] (mostly zeroes). Can I say something about positive-defiteness of $A$ in such a case? I'm aware of lots of results when $A$ has only 4 blocks, but in this case $K$ could be large.
hello
@Vrouvrou bonjour
bonjour
11:39
salut
Guys, why is the expected value a time and not the size of the expected population? I mean, it isn’t the time that is decaying, but the population..? I don’t really understand the conversion to a probability density function. So I’m guessing if we’re given a nonnegative $f(x)$ (whatever meaning that its values may have), we somehow end up with the distribution of the $x$, instead of the distribution of the values of $f$.
So what really happens when you normalise a function? (except for the obvious, which is calculating this normalising constant)
Oh maybe I see it. So by normalising a function, you basically write it as a scalar multiple of a density function. Then whatever the argument is in the function (say $x$), these $x$'s will be the possible values of the random variable associated with the distribution.
12:12
In any case, I've formulated my question here: math.stackexchange.com/questions/2276252/…
Might we worth noting that, in the case of the exponential, you're integrating from $0$ to $\infty$, not $-\infty$ to $\infty$
technically, you integrate from $-\infty$ to $\infty$
it's just zero on $-\infty$ to $0$
Indeed, but writing $N(t) = $N_0 \exp^{- \lambda t}$ doesn't state that (although, to any experienced user, it's of course clear from the context)
yea okay, fair enough
And, in regards to your question itself: isn't it just the distribution of the lifetimes?
As in, I'm assuming this is some exponential decay thingy from $N(t)$
12:20
well it must be, but the only reason I know that, is because I read that the mean is considered as the mean life time
so I know it "in hindsight"
I would kind of like to interpret it on a little more abstract/general level, so that I can recognise it on my own
Well, in a very vague way: $N(t)$ is the number of particles. You normalise everything, so it's unitless, but then you integrade w.r.t time; so the unit is time
okay, that already helps a bit
so whatever we were working first, it will get normalised, so it loses its dimension, and that's why we end up working with the input technically
I think your answer "distribution of lifetimes" is indeed what I was looking for actually
Oh yea, because is if you consider some time $t$, then $N(t)$ will give you the amount of particles that are still present at that time, so it gives you the amount that have a lifetime that is $\geq t$
How would you interpret it if we're considering the "decay" of an amplitude? So say we have $C(t)=C_0e^{-\gamma t}$. Like, what is the mean life time of the amplitude then? :P
(this is where my question originally came from actually)
13:05
Hello why math.se is not opening? Anyone else facing same?
it works for me
and for me also
Ok, working now
13:42
The distance of the plane 3x-4y+12z=3 is 1/2 . Am I wrong?
from the origin
14:06
@VenkiPhy6 why is it 1/2?
14:29
One of my maths friends said there is no general formula that can compute all possible carry overs for a base n system. If that's the case, I hope I can at least find a second best option that can model the "dynamics" of carry overs in base n.

This is because one reason I found number theory so confusing is because most of the weirdness (such as n parasitic numbers, last digit of a given natural number, divisibility etc.) all seemed to have something to do with the carry overs
For an illustation on what I am trying to say , consider the following:
You might find this paper interesting, Secret
(I shared it before, I don't know if you saw it)
Hey all, I have to shorten a formula. my formula looks like this z = xyyyy. Y is either 0 or 1 but each Y represents different values. Is there a way to shorten that formula something like z = xy^4?
(but it might be related to what you want)
Probably not read before, it looks very unfamilar on opening the pdf. Reading it now cause today my chemistry calculations are screwing up and they cannot be fixed until tomorrow, thus I had some free time with the maths today
@user1091558 Welcome to the chat! Do you have LaTeX on? (There's a link on the top-right in the room description)
14:35
No, let me turn it on
To answer your question: If they're all different values, maybe you'd want to write it as $z = x y_1 y_2 y_3 y_4$ (with subscripts) to differentiate all of them
@LeakyNun because of formula here(mathinsight.org/distance_point_plane). I am asking because a multiple choice question that I am solving doesn't have 1/2 as the option...
Awesome @ShaVuklia, how are you doing?
@Hippalectryon hey! How is it going?
@VenkiPhy6 can you show me how you got 1/2?
@Waiting Great :D what about you ?
14:39
Akiva, Thanks. But is there a way to shorten that formula like $z = xy(subscript)4$ and tell my readers explicitly that first y represents a, second y represents b etc ?
@Waiting Haha, I'm good:P how are you?
@Hippalectryon Glad for you! Good in some sense, and less good in other sense. Overall, I'm doing some research and preparing to publish something. :D
@ShaVuklia Cool!:P Still at uni, learning some new interesting stuff? Me? Not that bad, there is room for improvements. :P
@Waiting Yay :-) btw what happened to the other articles you wanted to have published ?
@Hippalectryon It's going to be published these days. It's just a matter of days.
@LeakyNun In the formula in the link I gave I used the following: (x1,y1,z1)=(0,0,0); A=3; B=-4; C=12 and D=3 and thats how I got 1/2...
14:42
:D @Waiting
@Waiting yea, still doings physics
@VenkiPhy6 firstly D=-3, and I don't see how that formula gives you 1/2.
@Hippalectryon Perhaps I shouldn't say that about my work, but it's damn awesome. :D
@Waiting Don't forget to send me a link to the articles when it's out :-)
@ShaVuklia Nice! Looks like you have a great time there. :P
14:43
btw, some Jason is looking for you:P @Waiting just letting ya know
@LeakyNun Okay I'm sorry I just found out what I am doing wrong... I was not doing 12^2 at all! Sorry again for wasting your time. Thanks, anyways
@Hippalectryon OK OK OK
@ShaVuklia Who is Jason?
Let me check.
uhm i donno, he changes his user name i think
@ShaVuklia I got it. It's OK.
good:d
14:59
Hi @PaulPlummer
@BalarkaSen Hey
(modulo the cohomology section which I only partially understood) It seemed to be more or less a rigorous version of my sketchy attempts on that carry over problem this afternoon (where I tried to write a natural number as a finite string, and then noticing how carry over occurs whenever the units sum larger than the base), as they formalise whether a carryover occurs with the map $z(b_1,b_2)$.

So yes it is quite relevant. Now to figure out how to generalise $z$ so that it can handle carry overs that occurs when we multiply two digits together, if we can do something like that, then solvin
I also notice from reading the paper that the phenomenon of carry over is "nonlocal" (i.e. it depends on all digits of smaller powers of base $b$ before it). I wonder if something similar can be found in arbitrary summations, that might help me to better understand how to decompose infinite series...
Now a completely unrelated question:
$$\epsilon_0=\sup(\{0,1,\omega,\omega^{\omega},\omega^{\omega^{\omega}},\cdots \})$$
When we build those $\omega$ power towers, are we acting the exponentiation from the left or the right side?
That is, to go from $\omega$ to $\omega^{\omega}$ to $\omega^{\omega^{\omega}}$ do we put our new $\omega$ beneath the old one or above the old one each step?
Guys, this is probably very stupid, but given that $\gamma>\omega$, I don't see immediately how $\gamma-\sqrt{\gamma^2-\omega^2}<\omega$. Maybe I could show that $\sqrt{\gamma^2-\omega^2}>\gamma-\omega$. However, $\gamma-\omega=\sqrt{\gamma^2+\omega^2-2\gamma\omega}$, so that's not helping either.
I don't see it. I also can't do something like this; $\gamma-\gamma\sqrt{1-\omega^2/\gamma^2}<\omega$
15:20
@Secret I am not sure I understand the question. Are you asking whether the notation $a^{b^c}$ means $(a^b)^c$ or $a^{(b^c)}$?
@user1091558 $z=x\prod\limits_{i=1}^4y_i$ would work, I think. You can learn about summation and product notation here.
@MartinSleziak well it's kinda related. cause the power tower can be built either by raising the index by omega on the right for each step, (which corresponds to the left associative case $((a^b)^{{}^c})$) or by attaching a new base omega beneath the power (which will correspond to the right associative case $(a^{(b^c)})$). so the question is that for the definition of $\epsilon_0$ how is the $\omega$ power tower built, from the left or from the right?
Hi chat
hi @Astyx
@Secret On the left. If you did it on the right, you'd just end up with $((\omega^\omega)^\omega)^\omega\dotsb$
which would equal $\omega^{\omega^\omega}$.
15:27
Ah I see
never mind, I showed it!
$x-y<\sqrt{x^2-y^2}$ $\Leftrightarrow$ $(x-y)^2<(x-y)(x+y)$ $\Leftrightarrow$ $x-y<x+y$
oh yea I did it like this: $$
\sqrt{\gamma^2-\omega^2}>\gamma-\omega\iff \gamma^2-\omega^2>\gamma^2+\omega^2-2\gamma\omega\iff\omega^2<\gamma\omega
$$
What's up ?
15:33
not much, how about you?
Finished my written exams 30 minutes ago
@ShaVuklia Take care! I have to leave now. One thing: follow your intuition (in general, you can't be wrong). ;)
@Waiting alright, see ya!
It feels so relieving
oh sorry I got interrupted irl :P
i wanted to say: congratz!
15:47
Haha don't worry
I got interrupted for that question about graphs that i asked here yesterday or the day before yesterday. We think that we have a solution now:P
but it's too easy, so I'll ask my teacher if it's correct
so you finished everything now?
Care to tell me ?
or your written?
do you remember the question? it was: if we have a 8-regular graph, show that is a spanning subgraph that is 4-regular.
@ShaVuklia $\gamma-\sqrt{\gamma^2-\omega^2}<\gamma-\sqrt{\gamma^2-(\gamma)^2}=\gamma<\omega‌​$
Note that, to maximize $\gamma-\sqrt{\gamma^2-\omega^2}$ (keeping $\gamma$ fixed), you want to minimize $\sqrt{\gamma^2-\omega^2}$ which means you want to maximize $\omega^2$.
oh cool, thanks @Akiva!
15:49
And if $\omega<\gamma$, then to maximize it you'd substitute in $\gamma$.
Only my written, I'll get the results mid June and then I'll know if I have oral exams (and I really hope I do, the contrary meaning I failed everything)
ohh gee:P that's a long time
but it's normal i guess
anyhow, about the question:
we thought of making an Euler-cycle
and then removing each other edge
then we are left with a graph that has degree 4
Why is that ?
oh shit
DAMN:P
it's not
Lol
15:51
we already tried this actually
but this friend came over and told me another person told him this solution
scheiße
nm
Sorry :/
I'm not sure I understand the question really, you mean there is a subset of edges $E'\subset E$ such that $(V, E')$ is 4 regular ? @ShaVuklia
@ShaVuklia Wait, ignore what I said
That was nonsense
@Akiva lol I already didn't get it entirely to be honest :P
at least
the last part
actually
i donno. my brain is mush
@Astyx yes!
apparently this answer I found on stack
is really the way to go
i contacted my teacher
so yea
15:55
(Sorry)
I'll give it some thoughts once I get some paper under my hand @ShaVuklia
Sure! Though it's really a matter of me understanding some specific steps in the proof. When I start studying for my exam on graph theory (which is in 1.5 months), I'll probably get back at it
Avika, Thanks. Thats what I was after :-)
Will you start studying in 1.5 month ? Or is the exam in 1.5 month ? Or both ?
16:04
lol the exam :P
i hope I don't start when the exam is XD
quick question guys:
One way to show that $e^{i\omega t}$ never vanishes, is to consider it as the polar form of some complex number with modulus 1. However, is there also a trigonometric approach? So we have
$$
\cos\omega t+i\sin\omega t=0\iff i\tan\omega t=-\frac{\cos\omega t}{\cos\omega t}.
$$
However, now that I come to think of it... why are we even allowed to divide by $\cos\omega t$?
oh wait
I have to consider cases of course
i completely forgot about that
you can divide by anything as long it is not 0 (in usual context)
yea, i forgot that i could simply consider cases
I however forgot where the complex roots of cos x were
complex roots?
well, if you are considering $e^{i\omega t}$ then naturally you need to consider the trig functions on the complex plane
16:11
I don't think cos x has any non-real roots
of course it has
for example?
I said non-real
sorry
i misread
too many negations dude :P
sorry
16:14
I don't think it should, cause we could rewrite it as $e^{2i \theta}=-1$, and a non-real number in the argument would make the modulus of the LHS not one.
ah ok
@Tim you referring to what I said?
because maybe I should have specified that we're only dealing with real $\omega$ and $t$
@ShaVuklia Referring to there being no complex roots of $cos(x)$. Not strictly to what you said.
16:40
You get a quadratic in an exponential term using euler
You only need to show the roots have modulus 1
The quadratic is $X^2-1=(X-1)(X+1)$ so that's settled
Nevermind that's exactly what Tim said
Hello ... I need help interpreting an algebra question
Let $G$ be a finite abelian group. If $G$ has at most $m$ elements of order dividing $m$ for each divisor of $m$ of $(G:1)$, show that $G$ is cyclic.
what does $(G:1)$ means?
Probably the cardinal of G
hmm ... this is problem from this book jmilne.org/math/CourseNotes/FT.pdf
page no 25
thanks ... i'll take that into account and think about it.
17:02
Uh, I don't follow what @Astyx is saying actually
and I don't understand why Tim takes $e^{i2\theta}=-1$
i'm kinda curious tho
Do you know Euler form for cos ?
ohh
yea give me 1 sec
i need to write it out:P
${e^{ix}+e^{-ix}\over2}=0$
haha yea that
Then mutliply by $2e^{ix}$
Qed
17:05
ohh
Just keep in mind that $e^{ix}$ is never zero.
lol yea that was the entire point no? xD
(I hope my latex is okay, i have no poit)
yea it's fine
Showing e^anything isn't zero is easy
17:06
lol wasn't that the entire point??:P
You just need to shiw there's an inverse
like, what were we doing then?
oh
Discussing cos
no i donno
Yeah I'm just pointing it out to be pedantic
17:06
oh yea
pedantic is good :P in math
because then i usually learn some tricks/details
You show that exp is a morphism from (R,+) to (R*, *)
Actually take C and C* instead of R
And that's done thanks to Cauchy
Funnily (or kinda) this is how you show the exponential of a matrix is invertible
17:29
Guys, say we're given $Ae^{i\theta}$. I would like to write this number in its complex form $a+bi$. I know that $a^2+b^2=A^2$. Now I also know that $\tan\theta=b/a$. So I guess I could write
$$
a^2+a^2\tan(\theta)^2=A^2\implies a=\sqrt{\frac{A^2}{1+\tan(\theta)^2}},
$$
and then obviously $b=\sqrt{A^2-a^2}$, where we substitute our $a$. Is this the only possibility? Or is there a cleaner expression possible?
Hello there chat!
and hi @Daminark
How's it going?
well i'm not dead, so i think good?
you?
Hi daminark
@sha can't yiu just use e^it = cos t + isin t ?
17:31
lol I thought you were talking to a chinese person for a sec :P
but ok i'll try i guess
Almost dead, but not yet. And it's scav so ('-')/ woo
oh wait, yea of course
Sorry, i struggle too much with my autocorrect when typing mathjax on my phone
As this message demonstrates :P
what's scav? @Dam
17:33
Especially since it's in french
haha I feel for ya @Astyx
It's a big scavenger hunt we have each year
It's the main feature of our school's existence
lol I think I'd hate such an activity XD
but I hope you have some fun then:P
Well it's not really a scavenger hunt, it's more about building stuff and cracking codes than searching for items lmao
hahah oh K :P
17:34
But yeah, in part for that reason I think I shall say adieu
Hi chat
Hibye @Eric
hi eric
Ew @Daminark I hate scav
lol :P
17:35
gasps
That's like, the reason why this place is great. That and HvZ :P
No one showers during it
And in my dorm they obstruct my path to the laundry room
17:36
And there's a reason for that, because there are higher priorities at play
Lol @Daminark I also dislike hvz
Nah sorry that's gross
@Eric I need to train your tastes more :P
Anyway I will actually get back to it now, I'm a page captain so I need to be on top of my shit, so see you!
Hibye @N3buchadnez
haha g'luck
Hi newly arrived people
And bye Dami
I know it is a bit fraudulent to ask about mathematics in chat :p However I have a question more along the lines of formulating a proposition in a clear matter, rather than the mathematics behind it.
If I have two inequalities $a < C b$ and $d < D e$, how can I say that the two inequalities are equivalent? Meaning that one holds if the other holds and vice versa.
17:41
You mean how can you prove it ?
No, just state it
$a < Cb \Longleftrightarrow d < De$
Isn't "$a <b$ iff $c <d$" good enough ? (Sorry my internet isn't very good)
I guess iff could be used, was just a bit unsure
Thanks =)
Np
17:48
Hi. $A$ is a symmetric, real, indefinite matrix with entries from [0,1] and nonzero diagonal terms, that I'd like to make positive definite (without affecting the diagonal). I tried "smoothing" off-diagonal terms: decreasing "highest" entries and increasing "lowest" ones with some matrix $B$. It happens that $B$ also, at least sometimes, is indefinite, but I still get the desired result. So indefinite + indefinite = positive-definite. Any intuition or results on how this happens?
Is B still symmetric ?
And what do you mean by indefinite ?
Neither positive definite, negative definite, positive-semidefinite, nor negative-semidefinite. And yes, $B$ is still symmetric. Both $A$ and $B$ have lots of zeroes, the entries of $B$ sum to 0
Since they are symmetric you can diagonalise them. Suppose the basis of the eigenvectors of A is also a basis of eigenvectors of B
Ola
Ola
Yellow.
Then the eigenvalue of the sum are the sum of each couple of eigenvalue from A and B
You want these to be all positive, which does not require the eigenvalues of B to be positive
Does this help ?
To see it clearly suppose both matrices are diagonal
17:58
Last night dream involve a very bizarre triple index notation for expressing a string of symbols in some compact form:
$$\mathbf{S}^i\vcenter{\tiny{j}}_{_k}=S^i T\vcenter{\tiny{j}}U_k=(((S)S)\cdots S)TT\cdots T(U \cdots(U(U)))$$
So for example $(T^2S)\vcenter{\tiny{4}}$ expands to $(((T)T)S)(((T)T)S)(((T)T)S)(((T)T)S)$
Well, I guess it will only be useful if some given nonassociative algebra have some nice rules despite nonassociativity
This dream also inspired an idea: I wonder whether a nonassociative derivative make sense...?
Non associative ?
Well, I guess something like either left associative or right associative, or a mix of them but never (ab)c=a(bc) for any a,b,c
But what do you mean by derivative then ?
We can potentially define a differential operator $d$ such that the product rule is obeyed i.e. $d(ab)=a(db)+(da)b$ (that's the minimal requirement for an element to be a differential operator). But on top of that, we also need to worry about where to place brackets when you have more than one $d$ in the expression
@Astyx, so $A=CDC{-1}$, $B=EFE^{-1}=EGG^{-1}FGG^{-1}E^{-1}=C(G^{-1}FG)C^{-1}$ and then the eigenvalues of the sum are the diagonal of $D+G^{-1}FG$, right? If so, this shows how this can happen. What about this "smoothing" of non-diagonal terms? It seems to be quite hard to relate it to the eigenvectors basis
18:10
So one possible way to construct such thing may be to generalise a differential algebra from a ring to some structure such that the multiplicative group becomes a loop (for example)
Let $D$ some countably infinite set in the plane $\mathbb{R}^2$. Is $D$ closed? If not, please don't provide a counterexample; I would like to find my own.
The usual topology of $\Bbb{R}^2$?
@Secret Yes.
@Julius not sure what you mean by smoothing here
@user193319 no
I mean that $B$ is such that it decreases relatively high nondiagonal elements of $A$ and slightly increases the zero ones. In this way reducing the variance of nondiagonal entries
18:15
@Astyx Thanks! I'll have to think about it, and if I can't resolve the problem--I will definitely be back.
@user193319 Can you find a counterexample in $\Bbb R$?
It also feels like if it were, proving it wouls be rather intuitive
@Julius and I meant codiagonalisable matrices, whereas you did something more general
What you said is not true : the eigenvalues of the sum are not the diagonal of the matrice you wrotr.
What you said is not true : the eigenvalues of the sum are not the diagonal of the matrice you wrote.

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