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00:10
The monolith aliens said stay away!
00:21
Can someone help me understand these lecture notes
is that "given $a \in \mathbb{R}$ and $\epsilon >0$" part meaning to quantify for all $\epsilon>0$ or just fixing some $a,\epsilon$
I'm guessing it's the latter, otherwise $V_{\epsilon}(a)$ would just be all of $\mathbb{R}$
and example 1. how would $\varnothing$ be an open set if there are no points for which the definition applies to?
@Obliv suppose $\emptyset$ is not open, what can you say?
01:27
obliv: do you mean, "how can emptyset fail to satisfy a definition that requires absolutely nothing in the case of the emptyset"? or as sine has phrased it, how could emptyset fail to be empty? (it would, among other things, have to have a point in it, to fail to be open)
 
6 hours later…
07:51
@SineoftheTime So at 4:30 I have the exam, I'll let you know how it goes :)
08:06
@Pizza :)
08:19
All the best @Pizza
 
1 hour later…
09:37
@SoumikMukherjee A thousand thanks !
 
2 hours later…
11:50
I feel silly since I'm almost 100% sure it's a typo, but in this answer, the author writes $\|T^{-1}(y)\| \leq \frac{1}{\alpha}\|T(x)\|=\alpha\|y\|$ where $y=T(x)$, and one of the comments also says that we should be able to deduce $\|T^{-1}(y)\| \leq \alpha\|y\|$, but shouldn't the inequality read $\|T^{-1}(y)\| \leq \frac{1}{\alpha}\|y\|$?
Then it makes sense too that $\alpha$ is some number $>0$.
Otherwise the condition $\alpha>0$ doesn't really have any effect.
12:10
@psie answer?
Question, I mean.
well, what do you think?
I think I'm right :)
right. You don't need anyone to confirm you on such triviality I'm sure
the comments made me insecure
12:14
no need to be so easily swayed by other people
trust your logic
working on it
but thanks
good luck
 
2 hours later…
13:59
When can a Tychonoff space be densely embedded in a non-normal space?
I think I might have an idea
0
A: Properties of Cross Product to infer the null space of this transformation

pwerth You are right; the negative of a linear transformation is negative. Indeed, since $T(x)=-C(x)$ and $C(x)$ is linear we have $$T(x+y)=-C(x+y)=-[C(x)+C(y)]=-C(x)-C(y)=T(x)+T(y)$$ and $$T(cx)=-C(cx)=-cC(x)=cT(x)$$ The null space is the set of vectors whose cross product with $v$ is $\vec{0}$. You m...

is this answer correct?
@AdilMohammed Yes.
my issue is probably with some sites saying its cross product and others saying its dot product (like wikipedia i think). i assume thats probably because of different definitions
14:38
cross product and dot product are two different things, they are both bilinear
The map sending $x$ to $v \times x$ is a linear map $\mathbb{R}^3 \to \mathbb{R}^3$, its kernel is the line spanned by $v$ and its range is the plane orthogonal to $v$ (for nonzero $v$)
The map sending $x$ to $v \cdot x$ is a linear map $\mathbb{R}^3 \to \mathbb{R}$, its kernel is the plane orthogonal to $v$ and its range is $\mathbb{R}$ (again, for nonzero $v$)
14:59
Can a graph be augmented by a line bundle?
15:31
@ModularMindset What does that even mean?
Hi everyone. Why does the Wikipedia article for Holmium-magnesium-zinc quasicrystal say that the faces are true regular pentagons? In what sense are they “true”?
A holmium–magnesium–zinc (Ho–Mg–Zn) quasicrystal is a quasicrystal made of an alloy of the three metals holmium, magnesium and zinc that has the shape of a regular dodecahedron, a Platonic solid with 12 five-sided faces. Unlike the similar pyritohedron shape of some cubic-system crystals such as pyrite, this quasicrystal has faces that are true regular pentagons. The crystal is part of the R–Mg–Zn family of crystals, where R=Y, Gd, Tb, Dy, Ho or Er. They were first discovered in 1994. These form quasicrystals in the stoichiometry around R9Mg34Zn57. Magnetically, they form a spin glass at cryogenic...
Looks pretty beautiful in any case though…
@AlessandroCodenotti for Linelof spaces, I believe I've proved its equivalent to compactness
Compact and zero-dimensional, of course
Maybe I should write a paper on this
16:08
hi
what do u think about the many worlds interpretation of quantum mechanics
16:22
@SohamSaha The relevant context is in the opening paragraph of the article you cite:
> Unlike the similar pyritohedron shape of some cubic-system crystals such as pyrite, this quasicrystal has faces that are true regular pentagons.
The word "pyritohedron" is a link to en.wikipedia.org/wiki/Dodecahedron#Pyritohedron .
> A pyritohedron is a dodecahedron with pyritohedral (Th) symmetry. Like the regular dodecahedron, it has twelve identical pentagonal faces, with three meeting in each of the 20 vertices (see figure).[3] However, the pentagons are not constrained to be regular, and the underlying atomic arrangement has no true fivefold symmetry axis.
And this is important because crystals (structures with translation symmetry) cannot have order 5 axes
17:11
I everyone I was watching how Fabinnoci number and music is related but video took some new turn creating different mathematical expression from the same numbers can anyone help me in getting crux of the video?
I am not a math major but read number theory in my high school and university
17:29
2
Q: Do Stone-Čech compactifications have property that disjoint closed subsets of $X$ have disjoint closures in $\beta X$?

Tereza TizkovaI came across this in Van Douwen´s paper, Characterizations of $\beta \mathbb{Q}$ and $\beta \mathbb{R}$, Proposition 4. Van Douwen writes: "We show that $\gamma H$ = $\beta H$ by showing that disjoint closed subsets of $H$have also disjoint closures in $\gamma H$." ($\gamma H$ is just an arbitra...

a misleading answer (and comment) about Stone-Cech compactifications and their properties corrected
we know closure as the smallest closed set containing a set, and interior as the largest open set within a set, but is there a notion for smallest open set that contains a set?
im not sure if this thing always makes sense
such a thing generally doesn't exist
take a point in $\mathbb{R}^n$, say
yeah I was thinking when two open sets dont contain one other
@BenSteffan makes sense
I wanted to prove this result: If $X$ contains two disjoint closed sets $F_1$ and $F_2$, then there exists open sets $G_1$ and $G_2$ such that $F_1\subseteq G_1$ and $F_2 \subseteq G_2$ with $G_1$ and $G_2$ disjoint themselves
Is anyone aware of anyone who has generalized Ihara zeta functions on k-regular graphs?
@nickbros123 that's false generally
17:42
I shouldve added: in metric space $X$
sorry
a space that satisfies that condition is called normal or T4
I guess Ill have to use some property of distances here. I have been proving most theorems I came across with just complements, closures and interiors etc that I forgot I was doing metric spacess :)
distances should be useful here, yes ;)
a hint is to use distance from a set functions
The point is that a closed set in a metric space is a zero-set (using those functions), and for two disjoint zero-sets $Z_1, Z_2$ there exists a function $f:X\to [0, 1]$ such that $f$ is $0$ on $Z_1$ and $1$ on $Z_2$.
I suppose those Fat Graphs could provide a little generalization
17:48
@SineoftheTime
Anyway I finished, I just didn't manage to do everything unfortunately, I mean I did everything but I didn't finish everything
However, I should have done something well, that is, the exercise procedures are all correct, I think.
I'm working an exercise where the aim is to prove all norms in $\mathbb R^n$ are equivalent. I need the following fact; the unit sphere in the $1$-norm is compact. I guess I need to show boundedness and that it is closed. Or is there a faster way to go about this?
I have no idea how the unit sphere looks like in the $1$-norm.
@Pizza glad to hear that
Was it hard?
@psie it pretty fast to show it's bounded and closed, isn't?
@SineoftheTime The differential equation was easy, I just forgot how to solve the integral, so I left it half done, I'm sad about that because it was easy, now I'll show you the exam
@SineoftheTime but that's not enough to show it's compact :)
unless the question is whether the unit sphere in the 1-norm is compact under the usual norm
Exercise 2 had 2 separate requests
That is, the exercises are not connected
I don't know how much was feasible in 2 hours, the double integral if you try to find what theta varies between is a bit strange but it should be 5π/4 and 3π/2
The first one was easy
The 5, is it done with Stokes' formulas?
I'm sad about the differential equation, the integral was easy but during the test I had a blank
I used the parameter variation method
18:00
I sat in a lecture just earlier today where we discussed the equivalence of norms in a finite-dimensional vector space over any complete valued field
@SineoftheTime What do you think about the exam ?
Ah, for the theory questions I managed to write the Poincaré theorem, instead for the differentiability questions I wrote the theorem and the proof
@BenSteffan hmm, I've already established that the identity map from $(\mathbb R^n,\|\cdot\|_1)$ to $(\mathbb R^n,\|\cdot\|)$ is continuous. Then I'd like to conclude that since the unit sphere in the $1$-norm is compact, and continuous functions map compact sets to compact sets, it is compact in $(\mathbb R^n,\|\cdot\|)$.
Then I'd like to say that the norm function is continuous, and hence attains a minimum on the compact set. This minimum is $\inf\{\|x\|:\|x\|_1=1\}$ and it is greater than $0$, which implies continuity of the inverse of the identity.
I'm using here the equivalence; identity bicontinuous $\iff$ norms are equivalent.
But I'm not sure about the statement "the unit sphere in the $1$-norm is compact".
@Pizza pretty standard
@SineoftheTime Exercise 5, is it done with Stokes' formulas?
@BenSteffan right, I was thinking about the $2$-norm
@Pizza yes
18:08
Oh ok I did it like this
I don't know if you want to try to find out what theta varies between in the integral.
we discussed question 6 a couple of days ago
yes, I wrote the Poincaré theorem there, I did the proof of the differential theorem
Could you do this by making the system where the circle and the line intersect?
$\frac54 \pi \le \theta \le \frac 32\pi$
18:12
I mean, I got confused here because I was getting strange coordinates,
@SineoftheTime Yes I wrote it like that
you used shifter polar coordinates right?
Yes
in which point?
-2 for y
0 for x
18:14
How did you find them so quickly?
I mean theta
if you draw a picture you don't need to do computations
Yes but how do you recognize 5π/4?
note that $y=2-x$ has slope $-1$
and the slope is $m=\tan \alpha$
I had made this system
it's easy to see that the line itercepts the $y-$axis in $-2$ and the $x-$axis in $2$, creating a $45-90-45$ triangle
18:19
That's why I didn't understand, but seeing -√2 and having radius 2 then I understood
geometry is important in double integrals, no need to solve the system in my opinion
if you draw the line and circle, you see easily the angle
no need to waste time solving a system
and yes ... I was used to doing it like that
though the procedure is correct and it's used in the general cases
@SineoftheTime yes but look at the points that come out of the system
That is, y I mean
Anyway, luckily I did well.
@Pizza yes, the points are correct
but you don't need them
18:22
How could "the intersection of a finite collection of open sets is open"
by definition :)
@SineoftheTime yes, but how did I figure out that it was 5π/4 from those points of y?
Wait
can I get an example? I'm thinking this isn't open: $(0,2)\cap(.5,1.5) = [.5,1.5]$ not open
recalculate the intersection, carefully
what you wrote is not correct
oh right
$(.5,1.5)$ doesn't contain the endpoints so it wouldn't be in the intersection
18:24
@Pizza do you mean: from the points you found, how to find the angle?
Yes
everyone uses $(a,b)$, I'm the only one in chat who use $]a,b[$ :((
@Pizza you can find theta such that $(\rho \cos \theta,\rho \sin \theta)=$your point
but this is strategy is not the optimal one
Hi everyone, I got a question about the expected value of the hyperbolic cosine of the standard Brownian motion, which has an answer here, but I would like to someone else to review it since following what I saw in a YT video it could be mistaken (and I aiming to use it).. I left a comment by the way, with the mentioned video
the (second) best way is to use the relations which define $D$
yes nvm
18:31
Will be facing a cyclone today
@SoumikMukherjee In my region there are floods since last week
I hope you are okay
I'm ok, but the area near me is under the water
where you see water, there are usually crops
18:48
Terrible situation
every year is the same unfortunately
is the closure of any open subset of $\mathbb{R}$ just $\mathbb{R}$
why wouldn't it be just the sup/inf of the subset..
@Obliv most certainly not
that's how we're defining it for some reason.
?
you're not defining the closure to be $\mathbb{R}$
18:52
a limit point is any point outside of the set so the set of all limit points of an open subset of $\mathbb{R}$ is its complement
so the closure of this subset is $\mathbb{R}$?
@Obliv no
that's not what a limit point is
wait
it's the point in which ALL epsilon neighborhoods of that point intersects A at some point other than it
this does not say "any point outside the set," now does it? :)
I thought it was for some epsilon neighborhood
ok yes that makes more sense
@Ben TIL: the simplicial category $\mathfrak{C}(\Delta^n)$ considered as a simplicial object in $\mathbf{Cat}$ can be described as a 'comonad resolution' (don't ask me what that means in general) of $[n]$, more precisely its given via $k\mapsto(FU)^{k+1}([n])$, where $F\dashv U$ is the canonical adjunction between $\mathbf{Cat}$ and $\mathbf{Graph}$
18:58
!?
my reaction, too
@Jakobian I think this is one of the criterion for disconnectedness no?
oh never mind i didnt read that properly
@XanderHenderson Take a topological graph embedded on a surface and endow it with a line bundle i.e. a vector bundle
19:25
Let $S^2$ be the 1-dimensional unit circle, and let $G$ be a 4-regular graph embedded into $S^2$. Assume that $G$ is the union of three distinct geodesic loops $\gamma_1, \gamma_2, \gamma_3 \subset S^2$, such that the vertices of $G$ correspond to the intersection points of these geodesic loops. Let the set of vertices of $G$ be denoted by $V(G)$, and the set of edges by $E(G)$.

We endow $G$ with a smooth line bundle $L \to G$, and assume that this line bundle is compatible with the Levi-Civita connection $\nabla$ induced by the Riemannian metric on $S^2$. This means that for each edge $e
more details on that
i made a trivial notational errror. S^1 should have been S^2. I tried to fix it
anyway that is an example I have been thinking about
19:43
This basically gives you electromagnetism
@SineoftheTime In your opinion, which exercise is the most difficult?
Anyway I'll let you know as soon as I know the results
@Pizza maybe the particular solution of the DE
but I should do the computations to judge
@SineoftheTime 2 easy integrals came out, only one for a void I didn't do it and I moved on, maybe the part after that the derivative with arctan etc came out
the derivative had to be done, something quite long came out
what did you use? Variation of parameters?
Yes
19:52
did you do 4 with Gauss Green?
In the end i have to find y'
@SineoftheTime yes, but I was not able to write the result of the last integral, but I did all the parameterizations
did you manage to conclude ex.5 ?
Yes
I did it all
that's good news. What is the minimum to pass? 18?
Yes
I hope I passed, even if I could have done more
19:55
I don't know how the points are distributed, but it seems you did a good job
I assume you did 1 and 2 perfectly
The first one yes, the second one only at the absolute extremes I did all the parameterizations but I was not able to insert all the points due to lack of time
but it shouldn't be a serious mistake, in the end I just had to calculate the points
I did the parameterization part well, then I also calculated the vertices
I'm considering asking my question on the main site, maybe someone there knows what the authors of my book meant when they said "the unit sphere in the $1$-norm is compact." Note, this is on an exercise on equivalence of norms in $\mathbb R^n$, so I can't use that fact.
the parametrizations on the square are straightforward
yes indeed
but I wanted to make sure I wasn't making any mistakes
are you planning to do the oral part?
20:02
@psie what do you mean "what they meant"
the statement is not ambiguous
@BenSteffan well, you were saying earlier checking closedness and boundedness here is not enough
indeed
do you know what the word "compact" means?
it's not closed + bounded
for now I have learned the proof of Schwarz's theorem, differential, Fermat, the whole part on Stokes and divergence (with Gauss Green), and one on Taylor series
But the one about the differential has already been written in the exam, I don't think he Will ask for it
@BenSteffan well, in $\mathbb R^n$ it always is, right? Otherwise, totally bounded and complete.
In $\mathbb{R}^n$, yes
usually the word means "every open cover has a finite subcover," but perhaps your analysis texts take a different view
20:06
Right, that has been mentioned too. But to prove the unit sphere is compact in the $1$-norm, does this argument work? It is bounded, i.e. $\|x\|_1=1<2$ for example and that the preimage of the continuous function $x\mapsto\|x\|_1$ of the closed set $\{1\}$ is closed.
you just acknowledged that closedness + boundedness is not enough
closed+bounded=compact in $\Bbb R^n$ with the usual topology (i.e. the one induced by the $2$ norm)
correct me if I'm wrong @Ben
you're right :)
that's precisely the point: you don't know that the 1-norm generates the usual topology yet, so you cannot use this
but you have another criterion, as you say
Ok.
20:09
Since the equivalence of norm is in fact an equivalence relation, I'd use the $2-$norm instead of the $1-$norm
@Gian'sPizzeria girls
It's really strange, because in my book the Heine Borel theorem has already been proved. So can I simply not use it?
It doesn't apply
Today in the test $y''+2y'+9y=1/sin(x)$ came out, I applied the similarity method with [1/(a sin(x) + b cos(x))], can you confirm that it's right?
Heine-Borel applies to $(\mathbb{R}^n, \lVert \cdot \rVert_2)$
compactness depens on the topology, HB works for the topology induced by the 2 norm.
20:11
oh, I have never realized that. I thought HB works for $\mathbb R^n$ (and any norm). Full stop.
@Gian'sPizzeria are you sure about the text of the problem?
@psie it does, you just might not know it yet
4 mins ago, by Ben Steffan
Heine-Borel applies to $(\mathbb{R}^n, \lVert \cdot \rVert_2)$
sku
sku
have trouble understanding limit points. A point x is a limit point of a set A if every epsilon-neighborhood V(x) of x intersects the set A in some point other than x. According to this definition, all points of (0,1) besides 0 and 1 are limit points? can someone give some intuition on limit points?
Since all norms are equivalent, then they induce the same topology. But you can't use it because that's what you're trying to prove
20:16
@sku 0 and 1 are also limit points.
well, they might be. 'limit point' is relative to the ambient metric space implicit in "V(x)"
i don't mean to confuse the matter. but the x in "a point x is a limit point..." isn't just out there flapping in the breeze
leslie 1 Xander 0
sku
sku
what would an example of not a limit point in the set (0,1)?
@leslietownes Oh, sure. I was assuming that we are in $\mathbb{R}$ with the usual topology. That feels implicit in the notation, i.e. the interval $(0,1)$.
@sku 7.
$\pi$.
between this and the different norms on R^n, lots of metric space particulars today
20:20
$-10^{100}$.
sku: some subsets of metric spaces contain all of their limit points, or have all of their points being limit points. you are not going to find a point in (0,1) that is not a limit point of (0,1). this example or set of examples is likely just testing how you map definitions onto relatively 'familiar' subsets of R. it is not trying to suggest that there is something particularly interesting about the limit point concept for an open interval in R
@sku Assuming that $(0,1)$ denotes the open interval from zero to one, and that the metric defining your $\varepsilon$-neighborhoods is the usual one, anything in the set $\mathbb{R}\setminus[0,1]$ is not a limit point of $(0,1)$.
sku
sku
I guess I am trying to understand why we are learning this concept. It has to be teaching something or a stepping stone to something else...
@sku What class are you taking?
Is this a real analysis class? A topology class?
Something else?
sku
sku
Real Analysis
20:23
@SineoftheTime y''+9y=1/sin(x)
I remembered badly
sku
sku
chapter 3 of Abbotts book
Okay, so do you remember calculus? And how you had to compute a lot of limits there?
sku
sku
yes
And how you dealt with notions like continuity and differentiability?
sku
sku
yes
20:24
@Gian'sPizzeria I'd use variation of parameters
In a more general setting, these things are all defined topologically, i.e. in terms of open sets.
@SineoftheTime I applied the similarity method with [1/(a sin(x) + b cos(x))], can you confirm that it's right?
It does not look right
So you are building the tools which are going to eventually allow you to push through all of those nice calculus theorems.
20:25
you use asin x+ bcos x for a particual solution of y''+9y=sin x
for 1/sin x, it's not enough to search a soln in the form 1/(a sin x+bcos x)
sku
sku
I see. one qq. in [0,1], is 1 not considered a limit point?
@SineoftheTime So if I wrote like this I automatically got everything else wrong?
I'd say so. Did you manage to find a particular solution?
20:30
Yes, but I'm getting something very long
why did you not use variation of parameters?
Because I saw the sin and the similarity method immediately came to mind
sku: does every interval of the form (1 - e, 1 + e), e positive, intersect [0,1] in some point other than 1? that's the question
sku
sku
Clearly the answer is yes. since 0<1-e<1
I mean it intersects wirh 1 also. I guess we mean intersect a point not including 1. Then no. I think I got it
I was confused with language. Thank you all
@Gian'sPizzeria this would have worked if it was =sin(x)
20:39
Why?
because this is not how differentiation works
@Jakobian interestingly there is an answer from 3 years ago claiming that it is a characterization of beta X for normal X but it has been deleted
Hello, I have a question about eigenvalues and eigenvecttors
Is there an intuitive way to prove the first statement
without calculating the eigenvalues and then the eigenvectors and then comparing them
?
Could I argue that if the scalar product of the two is zero than they are eigenvectors that correspond to differen eigenvalues
hence proving the statement
@AlessandroCodenotti it is
Ah yeah
imbaf: a very low tech approach would just be to write out what Hx = lambda x (where x is your (u, v*)^T vector) would mean in terms of a system of two scalar equations in u and v. it turns out to imply, without too much rewriting or effort, the system of scalar equations that tells you Hy = -lambda y (where y is that other vector)
20:53
But how is implied that
-v , u* is the eigenvector to -lambda ?
y is the other vector?
@leslietownes I thought of considering the complex conjugate in both sides
yes but to make sense of this, if you are stuck, it may help to write this out as a system of scalar equations that you complex conjugate
if rewriting the vector equation as a vector equation isn't seeming to lead you anywhere
I did write them as two equations
$\epsilon u + \Delta v*=\lambda u$
$\Delta* u -\epsilonv*=\lambda v*$
Is there a math problem solving channel ?
21:13
@sku 1 is a limit point of $[0,1]$.
The idea is that if $x$ is a limit point of $A$, then any punctured neighborhood of $x$ must intersect $A$. In the language developed for you thus far, $x$ is a limit point of $A$ if for any $\varepsilon > 0$, the set $$ \left[ (x-\varepsilon, x) \cup (x,x+\varepsilon) \right] \cap A$$ is nonemepty.
Every neighborhood of $x$ intersects $A$ at a point other than $x$ (it might also intersect at $x$---it certainly will if $x \in A$, but that doesn't matter).
sku
sku
Thank you so much @XanderHenderson and @leslietownes. I can see how this would relate to continuity in a future chapter.
imbaf: if you label those as (1) and (2), if you conjugate both sides of (1) and multiply through by -1 you get - delta' v - eu' = -lambda' u' which i will call (3), and if you conjugate both sides of (2) you get delta u' - v epsilon = lambda' v, which i will call (4). (4) and (3) are respectively the first and second entries of the vector equation Hy = -lambda' y, where y = (-v, u')
i'm writing ' for conjugate because asterisk sometimes triggers emphasis formatting in chat
imbaf: so Hy = -lambda' y. and since H is equal to its hermitian transpose it has real eigenvalues, so lambda' = lambda.
there might be some sign errors or misplaced ' in my calculation, but something like that is the idea. you won't need to evaluate what the eigenvalue lambda actually is, but you might need to know that it's real
(implicit in all of this, i think, is that epsilon is real)
21:31
@leslietownes I might need a moment to understand this
But you are complex conjugating both equations in both sides
its tempting to want to do this all in terms of matrix algebra and not write components, but you then need to 'matrix-ify' the operation of producing (-v, u') from (u,v'), which is still going to make express use of the fact that we have only two components
so it sort of amount to a system of two things anyway
imbaf: yes, if a = b (as complex numbers) then a' = b'
the prime is representing the conjugation?
yes, as explained previously i am not writing * for conjugation because repeated stars in chat sometimes cause things to be emphasized instead of to appear as stars
Let me try it
and rather than keep track of what will or won't set off people's chatjax formatting i often choose to just avoid triggering it :)
if i don't type $ or * the evil formatting can't get me
21:38
Ok so I tried it and this is where I am
So i had:
$\epsilon u + \Delta v'=\lambda u$
$\Delta' u -\epsilon v'=\lambda v'$

I did:
$-\epsilon u' - \Delta' v=-\lambda u'$
$-\Delta u' +\epsilon v=-\lambda v$
I see, so you are trying to recreate the unchanged components of the matrix, while complex conjugating the expression where u is?
@leslietownes but shouldn't you only complex conjugate:$\epsilon u + \Delta v'=\lambda u$ without changing sign
and complex conjugate and change sing for this $\Delta' u -\epsilon v'=\lambda v'$ ?
writing x = (u, v') and y= (-v, u'), if i had to describe it in short words, i wrote Hx = lambda x as a system of scalar equations in u and v'. i then complex conjugated both of those equations to get a system of scalar equations in u' and v. i then "noticed" (by just rearranging those equations) that this turns out to be, or give, a system of equations equivalent to the vector equation Hy = -lambda y
some of the way you're talking about it suggests that maybe you're focusing in on pieces of these equations and somehow "transforming" them individually, or that you think i might be doing that, and i'm not
i'm using tools like "if a and b are complex numbers and a = b, then a' = b'" and "if a and b are complex numbers and a = b, then -a = -b"
and other stuff like "if a and b are complex numbers, then a + b = -(-a) + b"
If i do complex conjugation on both and sign change on the first, I end up with one extra minus
there are a lot of operations going on here where there is an opportunity to make something resembling a sign error. note that the matrix H itself has one minus sign in it, and the eigenvalue the question is asking us to derive things about also has a minus sign in it
Since H is hermitian I can consider $\lambda$ not to change , it's real
but I don't get the expression
But how can something so trivial be so difficult
I don't think you can show what the exercise is asking that way
@leslietownes I dd it
Thanks
22:02
hooray :)
And if I need to argue what i did
would it be ok to say that I Tried to recreate the matrix on the LHS
and that led to an eigenvalue expression that showcases the other eigenvalue and its corresponding eigenvector
well, yes, the idea is definitely to rewrite the complex conjugate of H (u, v')^T = lambda (u, v')^T as another matrix equation that expressly involves the matrix H (rather than, for example, the entrywise complex conjugate of the matrix H)
and if you're careful, you find that you get what the exercise is asking for
I understand
the key is that whether we refer to it as 'rewriting' or 'recreating' or whatever else, the process is not one of just rearranging symbols to get the desired result, but actually deducing new true equations from old true equations using things like "if a = b then a' = b'"
but that holds only if a and b are the same in value and both real
no?
22:15
they can be complex too. the only use of anything being real in the above was in using things like epsilon' = epsilon and lambda' = lambda above, i.e. that epsilon was real and that lambda was therefore also going to be real
I've struggled with understanding why the unit sphere in the $1$-norm is compact. I turned to the main site, but without success so far.
you can get a matrix-ification of the calculation by doing something like letting e.g. K = [[0,-1],[1,0]] and checking that K^2 = -I and (from the way your particular H was defined) KHK = H', where H' is entrywise complex conjugate. the matrix calculation is then, from Hx = lambda x, conjugate both sides, use H' = KHK and then left multiply by K to deduce H Kx' = -lambda' Kx', so that if x is an eigenvector for lambda, Kx' is an eigenvector for -lambda'
a slight generalization of the exercise. where the opportunity for all the sign errors is baked into the computation that KHK = H'
22:55
@psie before this exercise, have you proven that if $\|\cdot\|_a$ dominates $\| \cdot \|_b$, then the open sets of $(V,\|\cdot\|_b)$ are open in $(V,\|\cdot\|_a)$ ?
I want to show $(E^{\circ})^c = \overline{E^c}$ so I started by analyzing the set definitions: $(E^{\circ})$ is the set $\{x\in E: \exists V_{\varepsilon}(x)\subseteq E\}$, so the complement is the set $\{y: y\notin E^{\circ}\}$ but idk how I'd define the complement of the interior of $E$.
@SineoftheTime hmm, I don't think so :( what were you thinking?
by dominate you mean $\|\cdot\|_b\leq c\|\cdot\|_a$ for $c>0$ I assume
I think in negations and logic statements so when I see complement I think of negations of set definitions, that's why I'm doing it this way
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