imagine this as the prototypical example: on the real axis, cycle (-1 0 1 inf), fix i and -i, and bend the imaginary axis to the unit circle and the unit circle to the imaginary axis. (draw this for aid.) this prototypical example can be postcomposed with a rotation around 0, and that rotates the axes around.
i and -i are fixed points in the prototypical example I'm talking about
they're treated like antipodal points on a sphere, and the real axis is like the equator
the left side of the unit circle buckles inwards for -1 to go to 0, while the right side of the unit sphere explodes outwards for 1 to go to inf
meanwhile, the imaginary axis inside of the circle bends to the right to become the right half of the unit circle, while the outside parts of the imaginary axis fold inwards from the left to become the left half of the unit circle
well, the left side of the unit circle becomes the line segment between -i and i. the point 1 goes to infinity. so what do you think happens with the rest of the right side of the unit circle?
now keep pushing it outwards more and more. keep in mind, the arc will always be anchored to +i and -i. so, let's say we keep pushing the arc more and more outwards. so much so, 1 ends up at infinity. where does the rest of the arc go?
the rest of the arc must be connected to +i, infinity, and -i...
the arc between 1 and +i blows up to the top part of the imaginary axis, and the arc between 1 and -i blows up to the bottom part of the imaginary axis
altogether, the unit circle is mapped to the imaginary axis
the pattern in which it colors the points of the plane isn't really important (that has to do with crazier stuff), what's important is to notice how the points are flowing under the "hyperbolic" rotation
so, start the video, and imagine a vertical line through the fixed point. what happens to that line as time passes?
@arctictern Is it true that $f(z_1) = \frac{1}{f(z_2)}$ if $z_1, z_2$ are symmetric with respect to a line or circle $C_z$ that gets mapped under a Möbius transformation $f$?
Two points $z_1$ and $z_2$ are said to be symmetric with respect to a circle $C$ if every straight line or circle passing through $z_1$ and $z_2$ intersects $C$ orthogonally
Hm okay then it makes sense
Can you construct a circle that goes through $0$ and $\infty$?
How can I get the common area here please? ctrlv.in/868116 Should I first subtract the circle from the petal to get the outside petal, and then subtract the outside petal from the whole petal to get the inside petal?
my problem was "How many injections $f: \{1,2,...,n\} \to \{1,2,...,z\}$ exist where $\nexists i \in \{1,2,...,n\}$ such that $f(i) =i$ and $n \leq z$?"
Let $Exp_t^{[y]} (x) $ denote the $y$ th iteration of the exponential function with base $t$ : $t^x.$
For example $Exp_t^{[1]} (x) = t^x. $
Let ~~ denote best fit.
Now as $x$ Goes to positive infinity and a pair $(a,b)$ with $e<a<b$ Is given , I wonder how to find the best fit base value $C$ ...
with normal integrals you can add the outputs, with elements of the lie algebra you can scale them by \Delta h, exponentiate and multiply in some order. if the outputs are just elements of a barren set, say...