#linear-algebra

2 messages · Page 248 of 1

lavish jewel
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and what eigenvalues and eigenvectors are

wintry steppe
#

yes

lavish jewel
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what's the definition

wintry steppe
#

@lavish jewel if you can find values to build a vector from others

lavish jewel
#

you're gonna have to write it down as an equation

wintry steppe
#

like a_1x_1 + ... + a_nx_n = 0 with a_1 = ... = a_n = 0

lavish jewel
#

right, that means that the x_i are linearly independent

wintry steppe
#

yes

gray dust
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"with" should be implies

lavish jewel
#

now notice that that thing you wrote is equivalent to the matrix-vector product $[x_1 x_2 \dots x_n]\begin{bmatrix} a_1 \\ a_2 \\ \vdots \\ a_n\end{bmatrix}$

stoic pythonBOT
lavish jewel
#

where the x_i are vectors

wintry steppe
#

yes

lavish jewel
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if the columns are linearly independent, then the system Mv = 0 only has the solution v = 0

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if the columns are linearly dependent, then Mv = 0 has nontrivial solutions for v

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you could then do elimination and find that the solution is parametrized in terms of free variables

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those solutions are a basis for the null space of the matrix M

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and they have the property that Mw = 0, for any such vector w in the null space

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which is the same as saying Mw = 0w

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or in other words, the vector w has an associated singular value of 0

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all as a consequence of M having linearly dependent columns

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and trivially, Mw = sigma w, with sigma nonzero, means w is a singular vector of M with a singular value sigma

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beyond that, i'll just direct you to the rank-nullity theorem

wintry steppe
#

@lavish jewel i mean you have that the rank is the dim of M - dim ker f

lavish jewel
#

now use that and what i just explained

wintry steppe
#

you remove the number of vectors that build Mw = 0

lavish jewel
#

i don't understand what you mean. remove them from what?

wintry steppe
#

why having Mw = 0w => M having linearly dependant columns

lavish jewel
#

you told me yourself

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that's the definition of linear dependence

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if w is nonzero and we can still get Mw = 0 = 0w, then M must have linearly dependent columns

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since Mw = 0 is the same as the definition of linear dependence that you gave me

lavish jewel
#

just call M = [x1, x2, ..., xn]

wintry steppe
#

wait i'm lost

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I said that but for saying x_i were independant

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not dependant

lavish jewel
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if the a_i can be nonzero, then that means the x_i are linearly dependent

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i mean

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if it's not linearly independent, then surely it is linearly dependent

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i don't think i will be able to explain this to you, i would strongly recommend you just start over from the beginning

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or maybe someone else can explain it here

wintry steppe
#

ok got it

wintry steppe
#

so based on the nullity theorem, rank f = dim E - dim ker f => rank f = number of independant vectors => Mw = sigmaw with sigma != 0

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@lavish jewel so if rank(f) = n, you can find n sigma and w to have Mw = sigmaw with sigma != 0 ?

lavish jewel
#

yes

stable urchin
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k for the sake of conceptual understanding

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take a columnspace of some matrix A

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say the rref of A is equal to some matrix B

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so is it true that the basis of the rowspace of A is equal to the basis of the rowspace of B

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since the rowspace of B is equal to the rowspace of A

lavish jewel
#

no

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the same subspace can have many bases

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as a simple example, [1,0] and [0,1] span R^2, and so do [1,0] and [1,1]

marble lance
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Being a basis for the one is the same as being a basis for the other, since they are the same. The main issue is the use of "the basis" since there is no one basis.

lavish jewel
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the operations you do in RREF are the same as what i did there, just adding (scaled versions of) the basis vectors together in some way

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for the common cases of R^n and C^n, any subspace has infinitely many bases

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except {0}

marble lance
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My snarky {0} reply was sniped sadcat

stable urchin
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i know about the infinite basis thing i just forgot about that when asking the thing

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i meant

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are the sets of bases for row(A) and row(B) equal

marble lance
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You started off talking about a column space, so btw, this is not true for column spaces since col(A) ≠ col(B) in general

lavish jewel
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wdym sets of bases

marble lance
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row(A) and row(B) are the same thing. Everything about them is the same.

lavish jewel
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it's the same subspace, you just found two different bases for the same subspace

stable urchin
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okay cool

wintry steppe
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In any vector space ax=ay implies that x=y . Is This statement True ?

marble lance
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@wintry steppe no

wintry steppe
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Why ?

marble lance
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0x = 0y for any x and y

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If a is nonzero, then yes

wintry steppe
#

Okaay ty !

stable urchin
#

How do I find a linear transformation $T:\mathbb{R}^5\rightarrow\mathbb{R}^3$ such that
$$
\text{nul}(T)=\text{span}\left{\begin{pmatrix} 1 \ 1 \ 0 \ 0 \ 1 \end{pmatrix},\begin{pmatrix} 1 \ 0 \ 0 \ 0 \ 1 \end{pmatrix}\right}
$$

stoic pythonBOT
#

timmmm

stable urchin
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I'm just finding it hard to work from a nullspace

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like I understand that from here you can say that {x1+x2+x5=0,x1+x5=0}

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but like I'm tryna think of how to get a 3x5 coefficient matrix from that

marble lance
#

You can uniquely define a linear transformation by describing what happens to the basis vectors of your domain. So you can extend those two vectors to a basis of R^5, send those two vectors to 0 and the others to something nonzero.

stable urchin
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alrighty so uhm

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it may be nearly 5 am and things are having a hard time penetrating my brain

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but is there a way in which you could elaborate on that just a bit more

marble lance
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Can you give me a basis of R^5 that contains those two vectors?

lavish jewel
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note that you were not given enough info to write a unique transformation T, you'll have to make some stuff up

marble lance
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That's not a basis of R^5

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A basis should have 5 vectors

stable urchin
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ah okay so a basis would be {e1,e2,e3,e4,e5}

marble lance
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Yes, but I want a basis that has as two of its basis vectors, those two vectors

stable urchin
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okay, {<1,1,0,0,1>,<1,0,0,0,1>,e3,e4,e5} i think

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oh wait

marble lance
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Yeah that works

stable urchin
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ooh fun

marble lance
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Now because I'm lazy I will call those b1 b2 b3 b4 b5 in the same order you listed them

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So you can define T(bi) = ci for any ci in R^3 and that will define a linear transformation, do you agree?

stable urchin
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yes

marble lance
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We need T(b1) = T(b2) = 0 so that b1 and b2 are in the nullspace

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So now it's just about sending the other three to something else so that no linear combination of them can map to 0

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Except the zero lin comb

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So 0 ≠ T(a3 b3 + a4b4 + a5b5) = a3 T(b3) + a4 T(b4) + a5 T(b5) unless a3 = a4 = a5

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And that's the same as saying T(b3), T(b4) and T(b5) should be lin independent

stable urchin
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yep

marble lance
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So you can map them to any three linearly independent vectors

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And then that transformation is what you want

stable urchin
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oh okay I'm just gonna take a sec to work with that

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thanks for the guidance

marble lance
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👍

stable urchin
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so would this new basis of dimension 5 be the range of the transformation?

marble lance
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The basis is the basis for the domain

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So it is unrelated to the range

stable urchin
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oh right that makes sense

marble lance
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The basis is in R^5, the range is in R^3

stable urchin
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right so I came up with the transformation
$$
T\begin{pmatrix} x_1 \ x_2 \ x_3 \ x_4 \ x_5 \end{pmatrix}=\begin{pmatrix} x_1+x_2+x_5 \ x_1+x_5 \ x_1+x_5 \end{pmatrix}
$$

stoic pythonBOT
#

timmmm

marble lance
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But T(1,0,0,0,1) = (2,2,2)

stable urchin
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oh shoot

marble lance
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Look over your work again, maybe you made a mistake when converting it to this form

storm fractal
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how do they calculate this? (is this the determinate or something different)

stable kindle
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determinant

storm fractal
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nvm

lavish jewel
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looks like they found the cofactors for the first row

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since one has to multiply the minors by the corresponding entry in the matrix, this immediately means you're adding 1*(some minor) + 0 + 0

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and the minor should be (-1)^2 det([-1, 4; -2, 8])

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which comes out to 1*(-8 - -8)

winged prairie
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does anybody understand why F^n can be seen as a function, this is from linear algebra done right

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like i thought F^n is just a set

small vigil
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Could you explain the S-lemma? What is it?
Are there any intuitive explanations?

winged prairie
stable kindle
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for example, take a function f from {1, 2, 3} to R

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then:
f(1) might be 3
f(2) might be 5.5
f(3) might be -1

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this function f corresponds to an element in R^3

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the element (3, 5.5, -1)

winged prairie
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ok makes sense

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ty

terse urchin
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For simplex method, how does slack variables transform inequalities into equalities? it makes like no sense to me

lavish jewel
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if, say, x < y, then one could add some c so that x + c = y

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and this c needs to be >= 0

floral thistle
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Good morning

pseudo elm
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Yo I need help

lavish jewel
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what do you need help with

pseudo elm
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How is that a2 = [a][a] = [9 8 9] ..

lavish jewel
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do you know how matrix multiplication works?

pseudo elm
#

Explain it to me

lavish jewel
pseudo elm
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;)

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Come on edddddddd

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Explain it to me

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○_○

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M waiting

lavish jewel
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this image is the only thing i'll provide you with

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google is a thing, and you presumably have a book and/or course material as well

pseudo elm
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Ok done

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I understood

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Thanks

lavish jewel
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otherwise, go to the help channels instead

pseudo elm
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I got the ans

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Arigato

heavy crown
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I don't understand it but I believe it should be simple, help ?

winter harbor
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Let $u \in T^{\perp}$. Then, $\forall v \in T$ we have that $\langle u,v \rangle = 0$. In particular, since $S \subseteq T$, we have that $\forall v \in S$ it is the case that $\langle u,v \rangle = 0$, thus $u \in S^{\perp}$ and $T^{\perp} \subseteq S^{\perp}$.

stoic pythonBOT
#

MISTERSYSTEM

winter harbor
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Was just a matter of using the definition of orthogonal complement.

heavy crown
winter harbor
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Np!

fickle citrus
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Hello all, suppose if I have
$$Av_{1}=v_{1}$$
and
$$Av_{2}=v_{2}$$
then what conditions do I need to say
$$v_{1}=c\cdot v_{2}$$
for $c\in\mathbb{R}$? In other words, Is there a way I would know they share an eigenvalue and indeed the multiplicity of this eigenvalue is hopefully $1$

stoic pythonBOT
#

ShatteredSunlight

fickle citrus
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Hmm, I think in general it's not possible?

teal grotto
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one sufficient condition is that eigen space corresponding to eval 1 is one dimensional

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this guarantees that the geometric multiplicity of eval 1 is 1, but not necessarily the algebraic multiplicity

fickle citrus
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Yeah, indeed, I require the geometric multiplicity to be 1

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I'm not sure if I can show that, so I will have to do my problem using high-power theorems I don't comprehend again...

teal grotto
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this one shouldnt need any other heavy machinery

lavish jewel
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the original question is a bit weirdly formulated

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since v1 = c v2 has nothing to do with the matrix

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you could simply normalize the vectors and then use cauchy-schwarz to show whether they are parallel

fickle citrus
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FWIW I'm doing the doubly stochastic matrix proof of stationary distribution (yet another proof)

A lot of the online proofs basically 'consider solution' and say it is the solution by uniqueness.

For me I don't like how it comes about, so I wanted to see how much I can push it.

The only additional thing I could add is that the vector of all 1s is linearly dependent to the final stationary distribution, given by
$$\mathbf{1}^{T}P=\mathbf{1}^{T}$$
under bistochasticity and
$$\pi^{T}P=\pi^{T}$$
under existence of stationarity

Then Perron-Frobenius says the there is only one eigenvector with all positive entries, so I finally get
$$\pi = c * \mathbf{1}$$

stoic pythonBOT
#

ShatteredSunlight

fickle citrus
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In essence I'd like a more algebraic a priori result of the stationary distribution rather than 'guess and check'

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And no Perron-Frobenius if I can help it, since I didn't prove PF

ionic laurel
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can anyone explain what the minimum rank of any matrix can be?

hard drum
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Will need more context lol but the true minimum across all possible matrices of any size is 0 since dimensions of vector spaces are nonnegative

ionic laurel
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in the context of an nxn, mxn, nxm i mean to say

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like the maximum rank of a matrix cannot extend beyond the # of columns and # of rows

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on the other spectrum

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what would the minimum rank be

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would it be dependent on the type of matrix?

teal grotto
# ionic laurel would it be dependent on the type of matrix?

not dependent on the size of the matrix. any n by m matrix with every entry zero has rank zero. it may depend on the properties of the matrix. for example, minimum rank of all symmetric matrices is still 0, but minimum rank of n by n invertible matrices is n

ionic laurel
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ok

teal grotto
#

?

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y is a function of x. there is no fixed value for y

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y = 2x is saying that given x, y is going to be twice the value of x

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x is not by default 0, whatever that means

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should be y = 6 if y = 2x

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this is not a linear algebra question btw. but still not clear what your question is.

teal grotto
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yes, it’s redundant to write y = 4x + 0

nocturne jewel
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btw, this isnt linear algebra

stable kindle
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google matrix inverse

prisma sail
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oh

nocturne jewel
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Im gonna guess it's wrong

prisma sail
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im dumb alright

nocturne jewel
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since that matrix isnt invertible

prisma sail
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huh

nocturne jewel
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6 6
1 1

This isn't invertible

prisma sail
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right

nocturne jewel
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so its inverse doesnt exist

prisma sail
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not sure how to go about this problem

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the diagonal is right but not the rest

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nvm nvm got it

wooden iris
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can someone simplify this explanation to why the matrix is linearly independent ysadcat

prisma sail
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columns aren't scalar multiples of each other

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and you can see if augment that matrix with the 0 vector
there will be a pivot in each non augmented column thus has only the trivial solution

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note that it can have atmost rank 3 because of the number of columns

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so that 0 row is ignored there are no free variables

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hopefully that helps im not too good at linear algebra

wooden iris
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thank you no it definitely helps!

solid cobalt
#

I need to find the the matrix T, B2_T_B1

I know how to perform the change of base with real numbers but how do I compute this since it involves complex numbers?
Is it the same process as performing the Gram Schmidt process on complex space?

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I have already shown that B2 is an orthonormal basis for C2
although I do not understand why we were asked to show that B2 is an orthonormal basis for C2 in the first place

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any explanation will be greatly appreciated

winter harbor
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What do they mean by T_B2, T_B1 ? Is it asking us to find the matrix of T with respect to the basis B2 and B1?

solid cobalt
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Transforming from one basis to another

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I don't know if I phrased that correctly

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hopefully you understand what I'm trying to say

winter harbor
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Alright

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So, the first column of the matrix T_ B2,T_B1 will be given as follows

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I suppose (1,2) is written in the standard basis of C^2

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So what we have to do

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Is find those coordinates

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With respect to basis B2

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This means that we must find constants a,b

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For which:
$$
\begin{bmatrix}
1 \
2
\end{bmatrix}

a
\cdot
\begin{bmatrix}
1/\sqrt{2} \

  • i / \sqrt{2}
    \end{bmatrix}

b \cdot
\begin{bmatrix}
(1+i)/2 \
(-1+i)/2
\end{bmatrix}
$$

stoic pythonBOT
#

MISTERSYSTEM

winter harbor
#

So we basically want to write (1,2) = a* w_1 + b *w_2

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For some constants a,b

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These constants

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Are the coordinates of (1,2)

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With respect to basis B_2

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These coordinates

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Will be the first column of the matrix we are trying to find

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Are you fine with this?

solid cobalt
#

I see
do I do the same process for the other columns?

winter harbor
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Yup!

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Now

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You will see why B2 being orthonormal is so useful

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Notice that, a priori, we would have to solve 3 different systems of linear equations

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But since B2 is orthonormal

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We don't have to

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Notice the following

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Take the inner product with respect to w_1 on both sides

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We will be able to simplify things down as follows

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$
T(v_{1}) = a w_{1} + b w_{2}
$
This implies that:
$$
\langle T(v_{1}), w_{1} \rangle = a \langle w_{1}, w_{1} \rangle + b \langle w_{2}, w_{1} \rangle
$$
But $B_{2}$ is orthogonal, meaning that $\langle w_{1}, w_{1} \rangle = 1$ and $\langle w_{2}, w_{1} \rangle = 0$. So in fact we have that:
$$
\langle T(v_{1}), w_{1} \rangle = a
$$

stoic pythonBOT
#

MISTERSYSTEM

winter harbor
#

So in fact, what we found out is that in order to calculate the first coordinate of T(v_{1}) with respect to B2

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All we have to do is take the inner product of T(v_1) with w_1

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We can do the same calculation to find the second coordinate of T(v_1)

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Just take the inner product with respect to w_2 on both sides

solid cobalt
#

mindblown
Thank you so so much for that explanation, It was spot on

winter harbor
#

Np

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Just do the same thing to find the other coordinates

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Take the respective inner products and so on

solid cobalt
#

will do
thank you so much again
hope you have a great day!

worldly bear
#

why are x4 and x5 0 here

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do you take like -13/6 * x5 = 0 or?

wintry steppe
#

I get that the eigenvectors of a matrix are the vectors that don't get rotated, only get scaled so they're always on their span and the eigenvalues of that matrix are the magnitude of the eigenvectors

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but

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how do I compute them for a given matrix?

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and eigenvalues an eigenvectors should exist for non-square matricies right?

worldly bear
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eigenvalues are only computable for square matrices

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If A is a n x n matrix, you can find its eigenvalues by solving the det(A - λI) = 0

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where I is the identity matrix

wintry steppe
#

what's lambda?

worldly bear
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just a variable

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eigenvalues are typically denoted by lambda

wintry steppe
#

ah so you solve for lambda to get the eigenvalue

worldly bear
#

exactly

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and those are the values for which the matrix A is scaled on its span

winter harbor
# wintry steppe and eigenvalues an eigenvectors should exist for non-square matricies right?

First of all, it doesn't make sense to talk about eigenvalues and eigenvectors for non square matrices, because notice that given a $n \times n$ square matrix $A$ over a field $\mathbb{K}$ we define a non zero vector $x \in \mathbb{K}^{n}$ to be an eigenvector of $A$ if $\exists \lambda \in \mathbb{K}$ for which:
$$
Ax = \lambda x
$$
Notice that this makes sense, because since $A$ is a square matrix, it sends vectors with $n$ entries to vectors with $n$ entries as well, so that asking $Ax = \lambda x$ makes sense. Notice, however, that if $A$ is an $m \times n$ matrix with $m \neq n$, i.e it is a non square matrix, we have that $A$ sends a vector $x$ with $n$ entries to a vector with $m$ entries, so that $Ax$ is a vector with $m$ entries and $\lambda x$ is a vector with $n$ entries, so asking for:
$$
Ax = \lambda x
$$
Doesn't make sense.

wintry steppe
#

ahh okay got it

#

thanks

stoic pythonBOT
#

MISTERSYSTEM

wintry steppe
winter harbor
wintry steppe
#

ah right

worldly bear
#

can a set of vectors give a basis for a certain space if the set of vectors is < the dimension of the space?

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they can right, but not if there are more vectors than the dimension of the space?

wintry steppe
#

I think it's the other way around

blissful trout
#

I have been struggling with my math homework, so basically I have to solve systems of equations using the Gaussian Elimination Methtod but it’s been making my head hurt trying to do it

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Can I send a picture of it?

worldly bear
winter harbor
#

Like

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The dimension of a vector space is defined as the cardinality of a basis set

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The reason this concept is well defined

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is because the cardinality of any basis you take is the same

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It is unique

worldly bear
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so for a set of vectors to be a basis, we have to have the same amount of vectors as the dimension

winter harbor
#

that's one of the requirements, yes.

worldly bear
#

and even if we do, it may or may not be a basis

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yes

winter harbor
#

But they also need to be linearly independent.

worldly bear
#

yes i understand all that

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lin independent and span

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so its not worth checking if a set of vectors form a basis if i have less than the dimension of the space, how would i denote that to my professor

winter harbor
#

What's the exercise, exactly?

worldly bear
#

,rotate

stoic pythonBOT
worldly bear
#

a is not a basis bc it is linear dependent

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b has more vectors than the space so it’s also not a basis

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c has less so i thought i had to check it for linear independence and spanning but you say i don’t have to since it can’t be a basis

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and d is a basis since it’s linear independent, don’t need to check spanning since we have 4 vectors in R^4, so spanning is given

winter harbor
#

You can explicitly show that at least some vector in R^4 can't be written as a linear combination of vectors in the set described by (c)

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If you don't want to use the fact that dimension is well defined

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also

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I am not sure if you professor has discussed the definition of dimension and proved that it is well defined + every vector space has a basis

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So checking things out using the definition would be a good exercise

worldly bear
#

well defined?

winter harbor
#

By well defined I mean the following

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Given a vector space

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We define its dimension as the cardinality of a basis set.

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Now

#

There's two things we have to be careful here

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First of all

#

What guarantees us that every vector space has a basis?

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Maybe there are vector spaces which do not admit basis, so we'd have to verify that.

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Turns out every vector space has a basis, so we are good for now.

#

But there's also another problem we have to check

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Because even if every vector space has a basis

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What guarantees us that a vector space might admit two basis with different cardinalities? It's not obvious at first, and you explicitly made a question regarding this.

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And turns out that the cardiniality of any two different basis sets of a vector space are the same.

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So we can, first, guarantee that every vector space has a basis and the cardinality of any two basis are the same. Thus talking about the dimension of a vector space makes sense, or in mathematical jargon, it is well defined.

worldly bear
#

why are the cardinality of any two basis the same?

winter harbor
#

For finitely generated vector spaces

worldly bear
#

just useful to know?

winter harbor
#

This is a consequence of what is called the steinitz exchange lemma

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And the proof is quite nice

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It doesn't use anything fancy

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You can even prove this result using stuff from system of linear equations

#

The Steinitz exchange lemma is a basic theorem in linear algebra used, for example, to show that any two bases for a finite-dimensional vector space have the same number of elements. The result is named after the German mathematician Ernst Steinitz. The result is often called the Steinitz–Mac Lane exchange lemma, also recognizing the generalizat...

#

The wikipedia article has a proof of this

worldly bear
#

i’m gonna look into it after i finish these review problems i think

winter harbor
#

For vector spaces which are not finitely generated

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We need more tools to prove this

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It involves something called Zorn's Lemma (Or you can be fancier and use something weaker like the Ultrafilter Lemma but shhh)

#

Which usually isn't covered in a first year course

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And is a tool from set theory/order theory

winter harbor
worldly bear
#

i took differential equations before linear algebra and i’ve already seen a lot of the conceptual relationships between them

winter harbor
#

Differential equations before linear algebra ? stare

#

How's that a thing KEK

worldly bear
#

dude i have no idea

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i kinda struggled in it too bc he kept alluding to linear algebra and how stuff works but i didnt know what was going on

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like for systems of diff eqs i was just mindlessly doing the computations bc i didnt understand what the point of finding these eigenvalues was

winter harbor
#

You have to do a lot of diagonalization and jordan canonical form machinery in an introductory differential equations course

#

a background in LA helps a lot

worldly bear
#

yeah it seemed like it would while i was taking it

winter harbor
#

Btw, here's the general theorem

#

This article has a proof for the infinite dimensional case

#

while the other one describes the finite dimensional case

worldly bear
#

im scared to even dip my toes in that

#

the infinite case

winter harbor
#

Are you doing engineering?

#

If you are doing physics

#

At some point you will have to

worldly bear
#

i am not

#

just a general mathematics major with a minor in comp sci

winter harbor
#

Oh nice stare

#

At some point you will have to get yourself used to this zorn's lemma machinery and so on

#

It's not as hard as it sounds

#

Plus, infinite dimensional vector spaces are as useful as finite dimensional ones

worldly bear
#

im sure ill cross that bridge at some point

winter harbor
#

they appear everywhere

worldly bear
#

yeah they seem more real life based then finite dimensional spaces

#

maybe im wrong though

winter harbor
#

Idk what real life based mean

#

But it's just that a lot of the vector spaces we care about in mathematics, in particular analysis, are spaces of functions which are in a major part infinite dimensional

#

Like the L^2 space, which is the main framework where one does fourier analysis

#

Or the space of real valued smooth functions on a manifold

#

or the space of continuous functions on the real line

#

Or the space of entire functions on the complex plane

#

and so much more

worldly bear
#

i appreciate your help and insight

winter harbor
worldly bear
#

@winter harbor i think i found the proof lol

winter harbor
#

What theorem is it referring to when it says "the above theorem"?

worldly bear
#

not sure, maybe one on a previous page

winter harbor
#

I hope so

#

It's prolly a version of Steinitz Exchange Lemma

ionic laurel
#

Is it possible for a finite set to span an infinite-dimensional vector space?

#

i am confused on that

#

there is a true or false that says

#

and this is false

#

but i am unable to understand how that is possible

#

if anyone could help that would be greatly appreciated

teal grotto
teal grotto
#

which is always finite

flint cloak
#

@teal grotto hey i was wondering if u could help me on this problem

#

I pinged helpers multiple times but i think there's no one available rn

flint cloak
#

there's 2 problems but they're very similar

flint cloak
#

do you know what the answer should be, im running out of time almost xD

#

i know the idea that for 1-1 u gotta get 2 polynomials to equal the 02x2 matrix but idk how to figure it out because the matrix given to us has all variables in each slot

#

so u cant even isolate for a degree

#

@teal grotto do you know how to do it

teal grotto
#

wow this is brutal

#

set a = -b and c = d = 0

#

just choose some random a, like a = 1

flint cloak
#

for 1-1?

teal grotto
#

ye

flint cloak
#

so <1,0,0> = [0,0,0,0]?

teal grotto
#

no, consider the polynomial x^3 - x^2

#

what is its image under T

flint cloak
#

0

#

if x = 1

teal grotto
#

what?

#

no, what is T(1*x^3 + (-1)*x^2 + 0x + 0) ?

flint cloak
#

idk

#

my brain honestly fried after 50 attempts

#

of different maps

#

r^3 p2 m2x2

#

lol

teal grotto
#

just set a = 1, b = -1, c = d = 0 and compute brah

flint cloak
#

so whats the other polynomial

#

that = [0,0,0,0]

teal grotto
#

the zero polynomial. all its coefficents are 0

flint cloak
#

what

#

so just T(0)?

teal grotto
#

yea

flint cloak
#

like this ^

teal grotto
#

yes

flint cloak
#

ah ok

#

and for onto

#

do u know if its onto or not

teal grotto
#

well, it wont be

flint cloak
#

and any y that satisfies

#

in matrix form

teal grotto
#

uhhh idk

flint cloak
#

would 1,1,1,1 work?

teal grotto
#

idk try it

flint cloak
#

i dont want to get it wrong because itll put me on a diff question then

#

lol

#

yolo

teal grotto
#

wait

flint cloak
#

alright

wintry steppe
#

is e^x the eigenvector of the derivative and the integral operator?

#

e^nx to be a bit more general

flint cloak
#

im going to just do {3,1,0,0}

#

worked

teal grotto
#

wow

#

actually insane

flint cloak
teal grotto
#

was that a guess

flint cloak
#

it was an educated guess

#

because

#

i just looked at row echelon

#

and just went w putting non zero on dependant basis vectors

#

just need help with this now

#

^

teal grotto
# flint cloak

for injectivity, check if the matrices are linearly independent. if not, then its not injective.
for surjectivity, check if the matrices are spanning. if not, then its not surjective.
this is a general way to do this

flint cloak
#

yeah im just pressed for time rn otherwise i'd do it the normal way

teal grotto
#

use symbol lab or something and put the matrices in as column vectors to check linear independence. like, put them in a four by four matrix. if it has zero determinant, then you know the matrices are linearly dependent. otherwise, theyre linearly independent and your matrix is injective and surjective

flint cloak
#

yh just did that

#

this thing has rank 3 so its lin dependant

#

just need to find an example of not 1-1 now

#

lol

#

thats the hard part

#

and an example of not onto

#

do you know an example that could work

winter harbor
# wintry steppe is e^x the eigenvector of the derivative and the integral operator?

Yup, it is! Notice that if we have an open subset $U \subseteq \mathbb{R}$, we can think about the space:
$$
C^{1}(U) := {f : U \rightarrow \mathbb{R} , \vert , \text{f is differentiable with continuous derivatice} , }
$$
Notice then that the derivative can be seen as the operator:
\begin{align*}
D : & C^{1}(U) \rightarrow C^{1}(U) \
f & \mapsto \dfrac{d f}{dt}
\end{align*}
Which is a linear operator. Now, $C^{1}(U)$ is an infinite dimensional vector space. In any case, the definition of eigenvalues and eigenvectors stays the same, i.e we define a function $f \in C^{1}(U)$ to be an eigenvector of $D$ if $\exists \lambda \in \mathbb{R}$ for which:
$$
D(f) = \dfrac{d f}{dt} = \lambda f
$$
And as you can see, the function $ f(t) = e^{\lambda t}$ satisfies this since:
$$
D(f) = D(e^{\lambda t}) = \lambda e^{\lambda t} = \lambda \cdot f
$$

flint cloak
#

@teal grotto do u know of any that would work

winter harbor
#

Yeah, one thing with operators on infinite dimensional vector spaces tho

wintry steppe
#

how does C^1(U) work? like I have never encountered that notation before

#

that text going off the screen lol

teal grotto
winter harbor
#

UGH

lavish jewel
#

i like my functions continuou

stoic pythonBOT
#

MISTERSYSTEM

winter harbor
#

It's still going offscreen

lavish jewel
#

must now interject with "derivatice"

wintry steppe
#

Lol

winter harbor
#

Anyways

#

If we take an open of the real line

wintry steppe
#

$$C^1(U) := {f\colon U \to \bR : f \text{ differentiable, } f' \in C(U)}$$

stoic pythonBOT
#

TTerra

wintry steppe
winter harbor
#

Yup

#

Differentiable functions with continuous derivative

wintry steppe
#

does the 1 indicate that it only has 1 continuous derivative?

winter harbor
#

We can talk about C^k functions too

#

Which are functions wich are k times differentiable

wintry steppe
#

ahh

winter harbor
#

And all its derivatives are continuous

#

Naturally

#

We can also talk about C infinity functions

#

Which are functions whose all derivatives exist

#

And all of them continuous (trivially in this case)

wintry steppe
winter harbor
#

Yup

#

They are one of the nicest examples

#

The exponential function is also C^infinity

#

Sine and cosine too

#

In fact, they are analytic

lavish jewel
#

the poly mention ties nicely into taylor's theorem

winter harbor
#

Which is stronger

wintry steppe
lavish jewel
#

there's real analytic too, which is weaker

#

rn everything was real

winter harbor
#

In this case, I mean that they have a Taylor series expansion everywhere

wintry steppe
#

ahh okay

winter harbor
#

Btw

#

I was about to talk about the spectrum of an operator

winter harbor
#

Which is a detail we have to care about when we are dealing with operators on infinite dimensional vectors

winter harbor
wintry steppe
#

ohh

winter harbor
#

Basically

#

In infinite dimensional vector spaces, some of the stuff we know about eigenvalues breaks down

wintry steppe
#

oh how?

winter harbor
#

In the following sense

#

In infinite dimensional vector spaces

#

Not every linear operator is continuous

#

We usually call continuous linear operators bounded operators.

wintry steppe
#

oh that's strange

winter harbor
#

Yeah, and turns out because of this

#

And some other technical details

#

It is more fruitful to talk about the spectrum of an operator

#

Rather than its eigenvalues

#

Its basically a generalization of what an eigenvalue is

#

In the finite dimensional case we don't have to care about this

winter harbor
#

This is the detail I wanted to mention

wintry steppe
#

wow functional analysis is so cool

winter harbor
#

But this is basically the only difference between dealing with eigenvalues on an infinite dimensional vector space

#

The definition is the same

#

But turns out that

#

We can talk about more general things in the context of infinite dimensional vectors

#

Which comes with the spectrum and so on

#

Its quite nice

wintry steppe
#

so the spectrum of on operator works even if the operator is not continuous?

winter harbor
wintry steppe
pallid yarrow
#

hello i am having trouble computing jordan normal forms

winter harbor
#

So I don't know

wintry steppe
#

me neither, I was just curious

pallid yarrow
#

i know how to find algebraic and geometric multiplicity. so i can find the jordan normal form up to reordering of the jordan blocks on the diagonal. is this sufficient to find a matrix's normal form?

#

i.e. are all jordan normal forms of a given dimension similar.

winter harbor
#

So this should not be a trouble.

pallid yarrow
#

i thought this just means that if a matrix has two jordan forms, they are the same but reordered on the diagonal. how does that show that the two jordan forms are similar?

#

like is there a matrix P such that PJP^-1 reorders the blocks or something?

winter harbor
#

Permutation matrices are invertible

#

And I think you can work out the details

pallid yarrow
#

hm. my textbook (artin's) says unique up to reordering of the jordan blocks on the diagonal. i dont think permutation matrices alone can reorder jordan blocks of different dimensions on the diagonal.

lavish jewel
#

i'm pretty sure you can set up block permutation matrices

pallid yarrow
#

would u mind showing me a quick example on a three by three jordan form with say, dimension 2 and dimension 1 blocks? i tried for a bit and got kinda stuck

lavish jewel
#

smth like this for a MWE

#

and of you call these T

#

you'd get smth like PTT^-1JT^T T^T,-1P^-1

#

terrible notation lol

#

$P T T^{-1} J T^\text{T} (T^{-1})^\text{T} P^{-1}$

stoic pythonBOT
pallid yarrow
#

whoa lol

lavish jewel
#

where, for clarity, the Ts on the right of the J can be different from the ones on the left

#

but that shouldn't happen here since you wanna move blocks along the block diagonal

#

then just associate as needed to get an equivalent form

#

if you're more familiar with it, perhaps, it's the same as why singular value decompositions are unique up to rotations

pallid yarrow
#

im not familiar with those

pallid yarrow
lavish jewel
#

yeah

pallid yarrow
#

what is P?

lavish jewel
#

oh, i guess i mixed up your notation

#

one second

pallid yarrow
#

yep np

lavish jewel
#

let's say there is some matrix A whose jordan normal form is PJP^-1

#

then another equivalent jordan normal form is the one i gave above

#

what i did was construct a similarity transformation between some J1 and another J2

pallid yarrow
#

ah thats what i thought

lavish jewel
#

some of the transposes and inverses can be removed from what i wrote, thanks to the properties of permutation matrices

#

yeah, you can remove the transposes on the right of J. then, if desired, replace the inverses with transposes (for the T only)

pallid yarrow
#

but why would there be transposes? J' being similar to J just means there is X such that XJ'X^(-1)=J

lavish jewel
#

because permutation matrices are orthogonal

#

so X^-1 = X^T

#

i think i put in the original transposes by mistake tho, to be honest opencry

#

$P T T^{-1} J T (T^{-1}) P^{-1}$ so this should do

stoic pythonBOT
lavish jewel
#

and you can replace T^-1 by T^T

#

there you can see that there's a similarity transformation acting on J, and that the resulting P' = PT matrices are the same as the original, but with shuffled columns

pallid yarrow
#

im not sure if we are talking past each other or not

#

im trying to show that any two jordan normal forms which are the same except the blocks on the diagonals are shuffled are similar

lavish jewel
#

that's exactly what is written up there?

pallid yarrow
#

TT^-1 J TT^-1 is just J lol. thats not a jordan normal form with different ordered diagonal blocks

lavish jewel
#

bruh

pallid yarrow
#

maybe im just being slow.

lavish jewel
#

$(P T) (T^{-1} J T) (T^{-1} P^{-1})$ how about now

stoic pythonBOT
lavish jewel
#

now let $(P T) (T^{-1} J T) (T^{-1} P^{-1}) = P_2 J_2 P_2^{-1} = A = P J P^{-1}$

stoic pythonBOT
lavish jewel
#

then you can solve for J in terms of J_2

pallid yarrow
#

oh! lmao

lavish jewel
#

and the result will be T^-1 J T = J_2

#

give it a shot

errant mist
#

I want to write that the abs. value of eigenvalue is less than or equal to the sum of each row in a matrix in mathematical notation . Would I just notate this as .: $|\lambda | \leq \sum_{i=1}^n A_{ij}$? Or does this sum over the entire matrix what I have written?

stoic pythonBOT
#

Fredrikpiano

lavish jewel
#

what you wrote adds the elements in a column

#

idk if that's what you meant

#

pick a column and add up all the entries in it

#

and if you wanted to say that this should work for any column, i would toss in a \vorall 1 <= j <= no. of cols.

errant mist
#

Its related to Gergorin's disc theorem where I have a symmetric matrix and I want to give a bound for the eigenvalues. If I understand correctly then the eigenvalue should satisfy being less than or equal to each row in the matrix as well as for each column.

#

This is what I'm trying to convey in mathematical notation

lavish jewel
#

sure

#

well, fixing j and iterating over i in the sum adds up the entries of a column

#

on the other hand, fixing i and iterating over j adds up the entries of a row

serene solstice
#

Find det(A). I'm thinking of partitioning, but how?

lavish jewel
#

so if you take what you wrote and add \forall j, this would say that the absolute value of an eigenvalue would be larger than the sum of the entries of any column of the matrix

#

i'm guessing you also have to specify an eigenvalue though

#

unless you mean this holds for all of them

errant mist
#

so, I add a $\forall j = (1,2,\dots, n)$ columns and $\forall i = (1,2,\dots, n)$ rows right?

stoic pythonBOT
#

Fredrikpiano

lavish jewel
#

one or the other, depending on what you're adding up (entries of columns or entries of rows)

errant mist
#

yes, thank you

#

means I will write the expression twice. Once for adding columns and once for adding rows

teal grotto
# serene solstice

this matrix is equal to (a-b)I + bJ where I is the 4 by 4 identity matrx and J is the 4 by 4 matrix with all entries set to one. try figuring out the eigenvalues of J and how many times they occur

serene solstice
teal grotto
#

they’re really helpful here : (

#

well, i guess it’s small enough to do laplace expansion

near crescent
#

Hello,
how can i show that
R3 ⊆ {(2, 1, 0), (-1, 2, 1), (0, 3, 0)}

where R3 means real numbers in 3 dimensions

dusky epoch
#

this is very clearly false as stated

#

did you by any chance mean to ask how to show R^3 ⊆ span {(2, 1, 0), (-1, 2, 1), (0, 3, 0)} ?

near crescent
#

yes

#

@dusky epoch sorry, i should have been more clearly

marble lance
#

Let (x,y,z) be an element of R^3. We want to show that (x,y,z) is in the span. So find a,b,c such that
(x,y,z) = a(2,1,0) + b(-1,2,1) + c(0,3,0)

near crescent
#

is it (0, 0, 0)?

marble lance
#

Is what (0,0,0)?

near crescent
#

(x, y, z) = (0, 0, 0) when a = b = c = 0

marble lance
#

That's true

#

But (x,y,z) has to be an arbitrary vector of R^3

#

Because you want to show that every element of R^3 is in the span

#

Now you have to find a b and c in terms of x y and z

near crescent
#

So that its not 0,0,0?

marble lance
#

No

#

It's an arbitrary vector

near crescent
#

you mean like this?: (2a - b, a + 2b + 3c, b)

marble lance
#

You cannot give it specific values

#

Well, if you simplify the RHS, that is what you get

#

So (x,y,z) = (2a-b, a+2b+3c, b)

#

Now you need to find what a b and c makes that true

near crescent
#

I have no clue beside from a = b = c = 0

marble lance
#

You are not understanding what you have to do

#

If you want to show that a set A is a subset of another set B, then you have to show that every element of A is also an element of B.

#

We now want to show that R^3 is a subset of the span of those 3 vectors

#

So you must show that every element is also an element of the span

#

The elements of R^3 look like (x,y,z) where x y and z are real numbers

#

The elements of the span look like a(2,1,0) + b(-1,2,1) + c(0,3,0)

#

So you have to take an ARBITRARY element (x,y,z) and show it belongs to the span

#

And the way to do that is to write (x,y,z) in the form a(2,1,0) + b(-1,2,1) + c(0,3,0) where a, b and c depend on what x y and z are

#

So you are not working with specific values for x y and z

#

So you cannot just say it is 0

near crescent
marble lance
#

I will do an example

#

Let's say we wanted to show that (x,y,z) is in span {(1,2,0), (0,3,0), (0,0,1)}

Then (x,y,z) = a(1,2,0) + b(0,3,0) + c(0,0,1) = (a, 2a+3b, c)

So we get
a = x
2a+3b = y
c = z

Subbing a = x into 2a + 3b = y, we get
b = y/3 - 2x/3.

So,
(x,y,z) = x(1,2,0) + (y/3 - 2x/3) (0,3,0) + z (0,0,1)

#

This shows that (x,y,z) belongs to the span since we have written it as a linear combination of the three vectors.

near crescent
#

thank you for the great example, ill try it on my own

marble lance
#

👍

near crescent
#

2a - b = x
a + 2b +3c = y
b = z

Subbing b = z into 2a - b = x, we get
a = 2/z + x

Subbing a = 2/z + x into a + 2b + 3c = y, we get
c = 1/3( -(2/z + x) - 2z + y)

So,
(x, y, z) = 2/z + x, 1/3( -(2/z + x) - 2z +y), z

runic snow
#

If (3x-1) is a factor of x^2+17x+k what is the numerical value of k?

marble lance
#

(x,y,z) = the linear combination of the vectors with those coefficients

#

(x,y,z) is not (a,b,c)

marble lance
near crescent
#

@marble lance can you tell me where my mistake slies in the 1st part?

Subbing b = z into 2a - b = x, we get
a = 2/z + x

#

or was the method right and i just twisted some numbers?

runic snow
marble lance
#

You can use other methods yeen

#

2a - z = x does not lead to a = 2/z + x

near crescent
#

a = 1/2(x + z) whoops, my bad, thank you

wintry steppe
#

why is the 0 vector not considered the eigenvector of every matrix?

marble lance
#

Because it doesn't have a single associated eigenvalue

wintry steppe
#

thanks

marble lance
#

It belongs to every eigenspace

#

👍

chilly shard
#

this proposition is in artins. but for the matrix $A=\begin{bmatrix}0 &1\ 1&0 \end{bmatrix}$, i think this is false(???). the eigenvectors of A are exactly those on the diagonal, which is a 1d subspace. but A is similar to a diagonal matrix. how can there be a basis of $F^n$ of eigenvectors?

#

dunno where i'm going wrong with this.

stoic pythonBOT
#

shortcut

chilly shard
#

(to be clear A is a matrix over the reals)

hard drum
#

The proposition is certainly true

#

For starters saying the eigenvectors are on the diagonal must be a mistake, do you mean eigenvalues? And that's unfortunately incorrect too as that's true only for triangular matrices, which this is not

#

The eigenvalues of A are 1 and - 1 as the characteristic polynomial is x^2 - 1

chilly shard
#

omg lol.

#

im very silly.

hard drum
#

(you might be confusing this diagonal (ig the antidiagonal) with the main diagonal)

chilly shard
#

||or tired||

hard drum
#

dw

pallid rampart
#

How do I show this?

#

Number 13

#

Preferably just a hint

zinc timber
#

||Orthogonalize||

wintry steppe
#

I am trying to understand any vectors v in the vector space V can be uniquely defined by its coefficients in the decomposition. I know if V has a basis then every v can be expressed as v = $\sum a_kv_k$.

stoic pythonBOT
#

Outlander

quasi vale
#

suppose that a vector can be represented in two(or more ways) by different coefficients, then try to come up with a contradiction

sick sandal
#

do you understand what the basis does?

wintry steppe
sick sandal
#

each vector can be represented by its coefficients in an ordered basis
these are just namely its "coordinates" wrt the basis

#

and its convenient to use

quasi vale
#

@pallid rampart I did this recently, xd. Try to use the Riez Representation Theorem

sick sandal
wintry steppe
sick sandal
#

its a basis with more information provided namely which vector comes 1st and 2nd etc so if you have some basis B={v1,v2...,vn} and you have a vector v=c1v1+c2v2+..cnvn the scalars c1,..,cn are the coordinates of this vector
and you can identify each vector using them only when the basis is ordered which should be clear to see why this would not apply to any basis
or in other words we can say there is a 1 to 1 correspondance between each vector v-->(x1,..,xn) to all of n tuples in F^n

wintry steppe
#

I see, it still a confusing but I understand why we can represent a vector with its coordinates with respect to a basis. Thanks.

sick sandal
#

or creates/determine is the proper word i suppose

#

the n-tuples will naturally be unique by this

#

you can ofcourse prove that anw

wintry steppe
#

by 1 to 1 correspondance you mean for each vector v we have a n-tuple (x_1,...,x_n) in F^n. So a basis allows us to have that.

#

but ordered basis? why does it only work for it.

sick sandal
#

take some unordered basis and try to assign some coordinates

#

lets say you get
2v1+3v2 and 2v2+3v1

#

are these the same?

wintry steppe
#

we don't know.

sick sandal
#

can you identify a vector with its coordinates

sick sandal
wintry steppe
#

ok.

sick sandal
#

moreover its not unique

#

this only works when you know for a fact

#

the 1st vector is v1

#

the 2nd is v2

#

so on

#

else the whole concepts fails

#

beauty of this is each n tuple assigns a vector in V for some ordered basis

#

and you can do addition and scalar multiplication normally as mentioned

sick sandal
# wintry steppe ok.

this might be a bad example but imagine the coordinate system and you want to assign a point (1,2,3)
would this work if the coordinate system wasnt ordered as (x, y, z) in that order?

wintry steppe
#

oh I see it would be confusing. Ok let me see I get it. For a basis B is a just a collection of vectors. There could be different linear combination of B for example if B = {e,b,d}, so for any v in V can be a_1e + a_2b + a_3d or a_1b + a_2d + a_3e etc. But if B was ordered we know which comes first.

#

Meaning a ordered basis is just a n-tuple of vectors. Am I getting it right?

sick sandal
#

eh sounds about right

#

should be clear why order is important to represent vectors as coordinates

wintry steppe
#

yeah. thanks for much.

wintry steppe
#

Ok I want to deeper insight why a system of vectors v_1, v_2, ..., v_n in V is linear independent if only the linear combination of the zero of V is trivial? Also what should I be doing when I encounter definitions that I understand but I do not understand why that definition was considered?. Sorry for the questions.

#

it's another way of saying that you can't solve for any of the vectors in terms of the others as a linear combination

#

Also what should I be doing when I encounter definitions that I understand but I do not understand why that definition was considered
try to understand through examples

#

definitions aren't made out of thin air

#

there's always some reason something's defined

#

ok thank you.

autumn kraken
#

Hello

#

I have a simple function R -> R, x -> x², how can I test if it's surjective?

#

I tried writing down f(x) = x² but got no further

#

dunno how to start

stable kindle
#

iff it's not surjective, there's some y such that no x in R satisfies x^2 = y

autumn kraken
#

oh

#

so any negative y 😄

stable kindle
#

mhm

autumn kraken
#

if it was surjective, how would you start there?

stable kindle
#

well it's not

#

but just explicitly find an element

#

like if it were x^3

#

show that cbrt(y) works

autumn kraken
#

cbrt?

#

x->x³ is actually the 2nd exercise lul

#

I will try

stable kindle
autumn kraken
#

okay

#

I also need to prove that the functions are well-defined

#

for the x->x² function, I just said that if x in R, then x² in R

#

is that enough? 😅

winter harbor
#

First of all

#

A function has 3 informations

#

A domain, a codomain and an assignment

#

For the x->x^2 function, I assume you are taking as domain and codomain R

#

So we have f : R->R which maps x->x^2

#

To check this function is well defined

#

We have to verify that for every element in the domain

#

I can assign f(x) to it

#

And we can do that in this case

#

For every real number we can assign its square

#

As a counter example

#

Consider g : R -> R given by x->√x

#

This is not well defined

#

Because we can't assign a real square root to a negative real number.

#

If we changed the domain say working with the non negative reals R+, then yes, g : R+ -> R which maps x->√x is well defined.

#

After checking if the domain makes sense

#

We have to check that the codomain makes sense

#

Namely

#

We have to check that the function indeed assigns an element in the domain to an element in the codomain and not another different set

#

For instance

#

Consider the negative reals R-

#

And the "function" f : R -> R- which maps x->x^2

#

This is not well defined

#

Since the square of a real number is always non negative

#

Or the "function" f : R -> [0,1], where x->x^2

#

This is not well defined

#

Because the square of a real number might be bigger than 1

#

Ofc, f : R -> R x->x^2 makes sense, since the square of a real number is always a real number

#

And similarly, f : R->R+ x->x^2 is well defined since the square of a real number is always non negative.

#

We have so far only checked that the domain and the codomain make sense.

#

Now we have to check if the assignment makes sense

#

Namely, if there's no ambiguity

#

For instance, the assignment f : R -> R where x->x^2 makes sense

#

Because the square of a real number is always unique

#

An assignment that has ambiguities is the following one

autumn kraken
#

Is it enough for me to say that every x² is unique?

#

I don't need to prove that right

#

I mean for ambiguity

winter harbor
#

But consider this one

#

\begin{align*}
f : & \mathbb{Q} \rightarrow \mathbb{Q} \
\dfrac{a}{b}& \mapsto a + b
\end{align*}

stoic pythonBOT
#

MISTERSYSTEM

winter harbor
#

This assignment is not well defined

wintry steppe
#

what's the connection between the dual of a vector space and the inner product defined in that vector space?

winter harbor
#

Why? Well, it seems that the domain and codomain make sense

#

But notice that 1/2=2/4

#

While f(1/2) = 1+2 = 3

#

And f(2/4) = 2+4=6

#

Which are different

#

A function must assign a unique value to every element in the domain

#

So we must check that

#

And in this case, it doesn't.

#

But that's basically all the technicalities you must be careful about @autumn kraken

wintry steppe
#

oh nice

winter harbor
#

Namely

#

Something called "Riesz Representation"

#

Let's work over a finite dimensional vector space, for simplicity

autumn kraken
#

thank you @winter harbor

#

for surjectivity of x->x³, I just said that for every x³ in R, there is cbrt(x³) in R, which means every element in R has at least 1 archetype/prototype (??? I don't know the English term, in German it's Urbild). Is this correct or not sufficient?

stable kindle
#

no

#

cbrt

#

pls

#

it makes sense

autumn kraken
#

yeah square root to the power of 3 is kinda dumb ngl lol

winter harbor
#

Let $V$ be a finite dimensional vector space over $\mathbb{R}$ or $\mathbb{C}$ where $V$ is endowed with an inner product $\langle \cdot, \cdot \rangle$. Notice that we can define a function:
\begin{align*}
\flat : V& \rightarrow V^{\ast} \
v& \mapsto v^{\flat}
\end{align*}
Where $v^{\flat}(u) = \langle u,v \rangle, \forall u \in V$.
\
\
Notice that since $\langle \cdot, \cdot \rangle$ is positive-definite, in particular it is non degenerate and so if $\exists v \in V$ for which $v^{\flat} \equiv 0$, this means that $\forall u \in V$ we have:
$$
v^{\flat}(u) = \langle u, v \rangle = 0
$$
Thus, $v = 0$ (by non-degeneracy) and as such $\flat$ is an injective linear map. Since $\text{dim}(V) = \text{dim}(V^{\ast})$ and both $V$ and $V^{\ast}$ are finite dimensional, this implies (by rank-nullity) that $\flat$ is an isomorphism. So notice that an inner product on $V$ induces a canonical isomorphism (that does not depend on a basis) between $V$ and its dual.

stoic pythonBOT
#

MISTERSYSTEM

winter harbor
#

This is a baby version of what we call the Riez Representation Theorem for Hillbert Spaces

#

Turns out that in the infinite dimensional case

#

A Hillbert Space is also canonically isomorphic to its continuous dual (i.e the space of continuous linear functionals on V) via the musical isomorphism $\flat$

stoic pythonBOT
#

MISTERSYSTEM

winter harbor
#

Yes

#

We call $\flat$ a musical isomorphism, its inverse is called $\sharp$.

stoic pythonBOT
#

MISTERSYSTEM

wintry steppe
#

oh wow really?

#

nice

winter harbor
#

These are the so called musical isomorphisms

#

Yup

wintry steppe
#

wait I'm a bit confused by that notation of v^bflat

wintry steppe
winter harbor
#

What is confusing?

wintry steppe
#

there's a function bflat mapping stuff from V to it's dual and what does v^bflat denote?

winter harbor
#

Ah

#

v^flat denotes a linear functional

#

What it does

#

Is that it takes an element in u

#

And what this functional does

#

Is take the inner product of u with v

#

v^flat(u) = <u,v>

#

This is what v^flat does as a linear functional

wintry steppe
#

ah okay

winter harbor
#

And flat maps V into its dual via v -> v^flat

#

So it indeed sends vectors to linear functionals

#

And we can show that this map is injective, and thus an isomorphism

winter harbor
wintry steppe
#

shouldn't it be bijective for it to be an isomorphism?

winter harbor
#

Yes, but an injective map between finite dimensional vector spaces of the same dimension is always an isomorphism.

#

So we don't even have to explicitly write down an inverse.

wintry steppe
#

I see

winter harbor
#

Just for completeness

#

The inverse of flat does the following

#

\begin{align*}
\sharp : V^{\ast}& \rightarrow V \
f \mapsto f^{\sharp}
\end{align*}
Where $\f^{\sharp}$ is the unique vector in $V$ such that $\forall u \in V$:
$$
f(u) = \langle u, f^{\sharp} \rangle
$$

stoic pythonBOT
#

MISTERSYSTEM
Compile Error! Click the errors reaction for more information.
(You may edit your message to recompile.)

winter harbor
#

So in some sense, this tells us that every linear functional on a finite dimensional vector space

#

Can be represented by a unique vector

#

Where the linear functional is just given by taking the inner product with this vector.

wintry steppe
#

ah

#

well thanks

winter harbor
#

Np, you can search up "musical isomorphisms" or "Riesz Representation" for more information.

wintry steppe
#

I do not know how a) and b) can be done but I know that c) and d) follows from a and b.

winter harbor
#

What is the 0 vector in the vector space of polynomials?

lavish jewel
#

use the definition of the kernel and the 0 element in the codomain

#

or if it helps you, you can write a larger matrix that transforms a vectorized form of M_22 into a vector isomorphic to a poly in P1

wintry steppe
#

[(a+b); (c+d)] = [0;0].
I tried this.

#

and I got { a = -b, c = -d, b and d are free in R }

lavish jewel
#

$\begin{bmatrix} a + b \\ c + d \end{bmatrix} = \begin{bmatrix} 1 && 1 && 0 && 0 \\ 0 && 0 && 1 && 1 \end{bmatrix} \begin{bmatrix} a \\ b \\ c \\ d \end{bmatrix} $

stoic pythonBOT
lavish jewel
#

this represents the same thing

#

and it's possibly easier to find the kernel of

#

at least easier in the sense that you already have the intuition for it

wintry steppe
#

then I'll reduce that to rref then check for linearly independent columns?

lavish jewel
#

if you don't see why this is equivalent, though, i strongly recommend you stick to the original formulation and follow mistersystem's tip

wintry steppe
#

I got dim(ker(L)) = 2.

autumn kraken
#

f: R->R, x²->x
this function is not well defined, is that correct?

#

because (-3)² != -3 for example?

winter harbor
#

It is not well defined because if you take 9

#

Then 3^2 = 9

#

And so f(9) = 3

#

But (-3)^2 = 9

#

So f(9) = -3

#

The same input gets mapped into different values

autumn kraken
#

oh

#

I thought the x has to be the same

#

but you can do f(3^2) = 9 ?

#

I don't understand

wintry steppe
#

it's not one-to-one then?

winter harbor
#

That's not what f does

wintry steppe
#

how do i do that?

autumn kraken
#

let x=-3, then f((-3)^2) = -3 <=> f(9) = -3, which is fine, but also for x=3 we get f(3^2) = 3 <=> f(9) = 3

#

ahh I see

#

thanks

winter harbor
#

Yup

#

Also

#

This is not really linear algebra

autumn kraken
#

dunno my module is called linear algebra 1 lul

wintry steppe
#

so I got dim([a,b; c, d]) = 4.

winter harbor
winter harbor
ionic laurel
#

I have a small question

#

the dimensions of the column space is the same as the dimensions of the transpose of the column space correct?

#

and this same concept applies to the row space

marble lance
#

What is the transpose of the column space? Do you mean the column space of the transpose?

#

Because that would just be the row space of the original matrix

ionic laurel
#

yeah my bad

#

i mean to say like

#

dim(ColA) = dim(ColA)^T

#

but yeah that makes sense

#

the column space of the transpose is the row space

#

and the dimensions of row space and column space are the same

marble lance
#

Yes

autumn kraken
winter harbor
#

If it is related to vector spaces and linear maps somehow

ionic laurel
#

Sort of a dumb question but does anyone know whether this is true or false?

The dimension of the vector space of signals, §, is 10

#

It's a true or false question in my textbook and I have not read anything about vector spaces of signals but yeah if this is sort of irrelevant then feel free to tell me 😅

lavish jewel
#

depends which signals lol

winter harbor
#

What is a space of signals stare

lavish jewel
#

same as usual. can be a vector space of some specifically shaped vectors in R^n, or something like that

#

signal usually only means it has some property or another that makes it more or less easy to fourier transform

ionic laurel
#

its all good

#

i doubt that type of specificity will show up on a exam

lavish jewel
#

there needs to be more context or it makes no sense

#

if that is all there is, the correct answer is "what the fuck"

ionic laurel
lavish jewel
#

what is \mathbb{S}

fickle citrus
# fickle citrus FWIW I'm doing the doubly stochastic matrix proof of stationary distribution (ye...

Update on this, I have considered alternative algebraic proofs which use 1-pi, and later on use the normalisation equation and distribution uniqueness later on to solve for a unique pi. There is no use of Perron-Frobenius, but rather on Kolmogorov Axioms/Probability axioms. In a way, this is nice in showing the resulting stationary distribution is a uniform discrete distribution.

However, I have decided to use Perron-Frobenius due to what it allows me to say: the linear dependence on the stationary distribution vector with the vector of all 1s, as achieved for every doubly stochastic matrix, means having a uniform discrete distribution as the stationary distribution happens only for the the family of all doubly stochastic matrices. In essence, there is a converse result achieveable with use of Perron-Frobenius which I think is a good addition.

#

In other words, by probability axioms and uniqueness of stationary distribution,
$$\text{Doubly Stochastic}\implies\text{stationary distribution is uniform discrete}$$

But Perron-Frobenius additionally says
$$\text{Doubly Stochastic}\iff\text{stationary distribution is uniform discrete}$$

stoic pythonBOT
#

ShatteredSunlight

fickle citrus
#

Probability axioms cannot do the converse for it says nothing of the dimensionality of the eigenspace of Perron root of ergodic transition matrices, and so cannot comment too much on the linear dependence of vector of 1s with the final stationary distribution

#

That said I really should look at a proof of Perron, and see if I can really 'get it'

pallid rampart
winter harbor
# pallid rampart I figured out a way in the end, but I’m interested to see how you did it with ri...

Let $\lambda_{1}, \cdots, \lambda_{m} \in \mathbb{R}$ be distinct positive real numbers and $V$ a Hillbert Space.
\
\
Let $f \in V^{\ast}$ be such that $\forall i \in {1, \cdots, m}$ we have:
$$
f(v_{j}) = \lambda_{j}
$$
And whose support is the closure of $\text{span}(v_{1}, \cdots, v_{m})$.
\
\
Since $v_{1}, \cdots, v_{m}$ are linearly independent vectors in $V$, this in fact induces a unique continuous linear functional on $V$ and thus $f$ is well defined. By Riesz Representation Theorem/Musical Isomorphism $\exists ! f^{\sharp} \in V$ for which $\forall v \in V$ we have:
$$
f(v) = \langle f^{\sharp}, v \rangle
$$
In particular, $\forall j \in {1, \cdots,m}$ we have that:
$$
f(v_{j}) = \langle f^{\sharp}, v_{j} \rangle = \lambda_{j} > 0
$$
Thus, by taking $w = f^{\sharp}$ the result follows ; $\square$

stoic pythonBOT
#

MISTERSYSTEM

winter harbor
#

I didn't take as hypothesis that V is a finite dimensional vector space. Which makes things harder because we have to guarantee f is continuous in order to apply the Riesz representation theorem.

#

And I think I was a bit handwavy there when making f vanish outside of the closure of the span of v_1, ...,v_m.

#

Because idk if it is straightforward if, in this way, we make f continuous.

#

But I suppose we can do something along these lines.

#

The finite dimensional case is more straightforward

noble swan
#

Hey, just making sure I understand basis' correctly. A certain set is the basis if the determinant != 0, right?

silent dune
#

How do I find two orthogonal vectors that are orthogonal to themselves and the plane? I can't figure any out that work

lavish jewel
dusky epoch
#

are you sure you phrased correctly what you are looking for?

#

'two vectors orthogonal to themselves and the plane' sounds sus

#

even if you replace 'themselves' with 'each other'

silent dune
#

ah maybe I wrote it wrong but the dot product of the two vectors has to be 0, and they both must be orthogonal to the plane

lavish jewel
#

they must be orthogonal to the plane's normal

#

not to the plane itself. they must be ON the plane

silent dune
#

right

#

but still I can't figure out two vectors that are

lavish jewel
#

you only need one. you could find the second using a cross product, which will by definition satisfy the conditions you're looking for

#

constructing just one is simple enough

silent dune
#

cross product?

lavish jewel
#

say (-3, -1, 1)

silent dune
#

ya

lavish jewel
#

at any rate, you can write is as a system of equations and use the techniques you already know