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15:01
pwoooff
I have arrived.
@Alizter Did you see the geometric not-so-rigorous analog of galois theory above ?
@BalarkaSen whare?
just above
You wrote?
from the place where the snapshots begin.
from here
15:06
@BalarkaSen Do you have the geogebra link?
I want to play with it.
try it
the best way to understand is to do teh experiments yourself and observe.
How do I plot stuff :P
ok, what do you see in the window?
Create your own
click on algebra
15:09
ok
now click on points and place a point.
place another point and right click on it and click on properties
what do you see?
15:10
Basic, Color, Style etc.
do you see anything like "define"?
or "definition"?
ok. is it a textbox?
then click on the textbox, remove all that is in there and replace by "sqrt(A)"
15:11
invalid input
your original point was named "A" right?
ok try clicking on A then and properties
click on "Algebra" tab
and change cartesian to complex
now try changin the definition of B
to just "sqrt(A)"
15:16
working now
ok, good
@Alizter now shift A from the first coordinate to the 3rd
i mean, from the upper left to lower left
the curve traced by B is discontinuous, right?
now place another point and define that to be -B
move A similarly : B and C will switch places
15:18
nice
that rather looks like a galois automorphism acting doesn't it?
Or more like a branch?
yes, but that is teh complex analytic way of saying it.
look at it as a galois automorphism
it is your classical galois theory
@Alizter now start a new algebra sheet. or rather delete your B and C.
leave A alone.
I changed it to cube root
ok, try it
you'll get similar.
15:22
how can I get all the roots of unity to show up
it was easy for sqrt because of -
-1/2 +/- sqrt(-3)/2
@Alizter I'd recommend you to do something else. Try drawing a point A and B = A^2 on the complex plane. note that you need to make B loop twice around the origin for A^2 to come back to where it started.
you can try similar for B = A^3.
i.e., whilst A loops once, B loops twice.
however, this works only if A loops around some point on the negative real axis.
ach why is it so slow
hmm yes
it works faster if you cancel out the properties tab
15:30
That is silly
@Alizter what is?
That the properties tab is causing slowness
no it is not
@BalarkaSen I feel like I am playing with keplers laws
the props tab shows you the coordinates
that takes time
@Alizter hah
well play with B = log(A)
that is more funny
15:32
that branch
mmhmm
the usual log is defined by abs arg log < pi
if there hadn't been that restriction, you could have seen B going above and above and notcoming back
@BalarkaSen I like to think of log as a drill bit
:P
well, back to buisness
think of B = A^2
B=1/A is also interesting
look how chaotic it is near 0
mildly.
15:34
but does nothing every where else
it's the riemann sphere, dude
I knwo.
ok, where was i?
right B = A^2
A loops once, then B loops twice
@BalarkaSen on the imaginary axis
correct.
well, in prticular on the origin
15:36
B=A^3 A loops once then B loops thrice?
yes.
and this reminds a bit about cyclic grousp, don't they?
B = A^2 seem to have a correspondence with $\Bbb Z_2$
let's look at the picture :
How can I create a circle for it to slide on?
@Alizter bah it's right there
above. there is a picture of a circle.
then right click and vanish the points you don't want to appear in your work
uncheck the show object box, i.e.
in any case, the picture above should be given some importance. there are two sheets, as you see and cut and pasted togather through the imaginary real axis
@Alizter here's how it's relevant : take two sheets, corresponding to two copies of complex plane
now let $\sqrt{z}$ and $-\sqrt{z}$ act on the two sheets
the first on the bottom, the next on the upper
15:41
yup
we branch the two sheets at $0$, as $\sqrt{0} = -\sqrt{0}$
i.e., paste the two sheets at the point $s = 0$.
@Alizter now the two functions are both discontinuous in their sheets, when $z$ moves from the upper left sheet to the lower left sheet.
^ the pic on the right
alright
to preserve continuity, one possible solution would be to cut both sheets through the negative real axis, and paste the A part with A' part, and the B part with B' part.
15:45
yep
this gives you the surface at the left
of course, intersection happens when this is done in R^3 but it can be avoided in R^4
@Alizter now, let $z$ be a point on the bottom sheet on the surface on the left
for $z$ to loop once around the origin, it needs to go above to the upper sheet and then come back, right?
as there are pastings through the negative real axis/
but that, when seen from above by a flying kite, say, it'd look as if you are revolving twice around 0!
that is precisely what is happening in geogebra with A and B = A^2!!!
15:49
ohh
interesting
so now Galois theory what does this mean?
so the surface on the right is the surface on which $\sqrt{z}$ is continuous.
it is not C, but a subset of C^2!
@Alizter coming to the point. first, rigorously the surface is $\{(a, b, c, d) \in \Bbb R^4 : (a + ib)^2 = c + id\}$.
to verify this, cross-section the surface.
you'll get $y = x^2$, the standard graph
^
you like that picture :P
well it's intuitive :P
and i ain't have anymore picture of riemann surface of that!
15:51
@BalarkaSen I cut one out of paper infront of me
proceed
@Alizter so you wanted connection with galois theory, right?
in the graph A and B = A^2 in geogebra, B must loop twice for A to come back, right?
15:54
ye
that relates to the cyclic group of order 2
Was about to type that
now what about 4?
in other words, $w^2 - z$ has corresponding group $\Bbb Z_2$
@Alizter B = A^4?
Yeah is it Z/4Z or Z/2Z^2?
15:55
how can we tell?
or rather construct klein 4?
just draw it out in geogebra to verify
@BalarkaSen What polynomial has klein 4?
that i'd leave you to figure out.
just to add, these groups are called monodromy groups
and in fact it can be proved that monodromy groups = galois groups
'=' is here the isomorphism
@Alizter now recall A and B = log(A)
@BalarkaSen Hmm, how would geoegebra?
I think klein 4 would be $x^4+ax^2+c$ or something
more or less. just make a good guess from galois theory
what is an extension of Q which has galois group Z_2^2?
16:01
Q(i)?
wait
that'd have gal group Z_4
so no
ahh I have not done this in a while
how about Q(2^1/2, 3^1/2)? does that work?
yeah
then take, say, B = (A^2 - 2)*(A^2 - 3)
the two branch points are 2 and 3 on the complex plane
it'd be interesting to play with it
fiddle on! =)
16:06
It cycles every two
oops i mean branch points are sqrt(2) and sqrt(3)
that is weird and cool
What do symmetric groups look like
haha i see you've got a hang on it
@Alizter ah, that
16:09
x^5-x-1 i think has that
well B = A^5 - A - 1
unless i cant remember
oh
yes, indeed
@Alizter ok i have to go. fiddle with it
just before i leave,
what i explained to you is called topological galois theory, in it's full rigorous form
16:10
It makes a flower :D
it can actually be used to prove abel-ruffini theorem in a totally different way. using topology and geometry.
If you look at $x^5-x-1$ on the unit circle
Indeed
it plots a flower with 4 petals
The riemann surface is complicated
16:11
thats valentines day sorted. Here you go S_5
hahaha
ok i am out
sadly only 0.1% of the female population would get it
have fun with it
@BalarkaSen Thank you.

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