What Maps Belong to Aut(S2)/SO(3)?

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In summary: Intrinsic cohomology is a branch of mathematics that studies the properties of the cohomology of a manifold.
  • #1
lugita15
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Consider Aut(S2), the automorphism group of the Riemann sphere, i.e. the group of bijective holomorphic maps from C2 U {∞} to itself. Clearly some automorphisms of a sphere are the rotations of the sphere, SO(3). But what other maps are in Aut(S2)? To put it another way, what bijective holomorphic maps from C2 U {∞} to itself belong to the quotient group Aut(S2)/SO(3)?

Any help would be greatly appreciated.

Thank You in Advance.
 
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  • #2
The automorphisms of the Riemann sphere are the mobius transformations, so Aut=PGL(2,C). Those which are rotations have a particularly special form - they come from unitary matrices, i.e. they form the subgroup PSU(2) (which is isomorphic to SO(3)). However, PSU(2) isn't normal in PGL(2,C), so it makes no sense to talk about the "quotient group" PGL(2,C)/PSU(2).
 
  • #3
OK, let me put it this way. Any möbius transformation is a composition of an element of PSU(2) and an element of ... what?
 
  • #4
Any more thoughts on this?
 
  • #5
lugita15 said:
OK, let me put it this way. Any möbius transformation is a composition of an element of PSU(2) and an element of ... what?
I don't think there's a nice way of describing "what?" here, in the sense that there is no subgroup complement to PSU(2) in PGL(2,C). This is because you can express each rotation as a composition of automorphisms that aren't rotations (so the "complement" of PSU(2) in PGL(2,C) won't be closed under multiplication); in fact, you can express every automorphism in PGL(2,C) as the composition of dilations, translations and inversions (see here).
 
  • #6
morphism said:
I don't think there's a nice way of describing "what?" here, in the sense that there is no subgroup complement to PSU(2) in PGL(2,C). This is because you can express each rotation as a composition of automorphisms that aren't rotations (so the "complement" of PSU(2) in PGL(2,C) won't be closed under multiplication); in fact, you can express every automorphism in PGL(2,C) as the composition of dilations, translations and inversions (see here).
First of all, you didn't actually put a link in your post. Second of all, is it possible to describe the automorphism group PGL(2,C) of the Riemann sphere in geometric terms, i.e. describing what you're physically doing to the sphere?
 
  • #8
morphism said:
As for your second question: check out this video.
OK, so the video says that every Mobius transformation can be written as a composition of rotations of the complex plane, inversions, translations of the complex plane, and dilations. And according to the video, a rotation of the complex plane is a vertical rotation of the Riemann sphere, an inversion is a horizontal rotation of the Riemann sphere, a translation of the complex plane is a horizontal translation of the Riemann sphere, and a dilation is a vertical translation of the Riemann sphere. So is it safe to say that any automorphism of the Riemann sphere is a composition of rotations of the Riemann sphere and translations of the Riemann sphere?

Also, just like the rotation group of the Riemann sphere can be written in concrete terms as PSU(2), how would you describe the translation group of the Riemann sphere in concrete terms? To put it another way, what is the name of the group of all transformations that can be written as compositions of translations of the complex plane and dilations?
 
  • #9
lugita15 said:
OK, so the video says that every Mobius transformation can be written as a composition of rotations of the complex plane, inversions, translations of the complex plane, and dilations. And according to the video, a rotation of the complex plane is a vertical rotation of the Riemann sphere, an inversion is a horizontal rotation of the Riemann sphere, a translation of the complex plane is a horizontal translation of the Riemann sphere, and a dilation is a vertical translation of the Riemann sphere. So is it safe to say that any automorphism of the Riemann sphere is a composition of rotations of the Riemann sphere and translations of the Riemann sphere?
No. In the video they're keeping track of what happens to the stereographic projection.

Also, just like the rotation group of the Riemann sphere can be written in concrete terms as PSU(2), how would you describe the translation group of the Riemann sphere in concrete terms? To put it another way, what is the name of the group of all transformations that can be written as compositions of translations of the complex plane and dilations?
Translation doesn't move the sphere around. Don't confuse what the video was showing (i.e. the interaction of mobius transformations on the plane and stereographic projection) with the the automorphisms of S^2. When you talk about Aut(S^2), you're thinking of intrinsic automorphisms. A translation in this sense translates points on there sphere to other points. If you view the Riemann sphere as ##\mathbb C \cup \{\infty\}## then a translation is just a map of the form ##z\mapsto z+b## (for some ##b \in \mathbb C##). This is fairly concrete. Similarly, a dilation looks like ##z \mapsto az## (##a \in \mathbb C\backslash \{0\}##).

The subgroup generated by these is simply the group of all automorphisms of the form ##az+b## (## a \in \mathbb C\backslash \{0\}, b\in \mathbb C##). Note that every such automorphism fixes the point ##\infty##, so it is simply an automorphism of ##\mathbb C##. In fact, this is precisely the group of automorphisms of the plane. So you can call it ##\text{Aut}(\mathbb C)##.
 
  • #10
morphism said:
No. In the video they're keeping track of what happens to the stereographic projection.
But I thought the stereographic projection IS how we understand the Riemann sphere as a sphere.
Translation doesn't move the sphere around. Don't confuse what the video was showing (i.e. the interaction of mobius transformations on the plane and stereographic projection) with the the automorphisms of S^2. When you talk about Aut(S^2), you're thinking of intrinsic automorphisms. A translation in this sense translates points on there sphere to other points. If you view the Riemann sphere as ##\mathbb C \cup \{\infty\}## then a translation is just a map of the form ##z\mapsto z+b## (for some ##b \in \mathbb C##). This is fairly concrete. Similarly, a dilation looks like ##z \mapsto az## (##a \in \mathbb C\backslash \{0\}##).

The subgroup generated by these is simply the group of all automorphisms of the form ##az+b## (## a \in \mathbb C\backslash \{0\}, b\in \mathbb C##). Note that every such automorphism fixes the point ##\infty##, so it is simply an automorphism of ##\mathbb C##. In fact, this is precisely the group of automorphisms of the plane. So you can call it ##\text{Aut}(\mathbb C)##.
Would it be correct to say that the transformations in PSU(2) correspond to rotations of the stereographic projection? Also, would it be correct to say that transfomations in the automorphism group PGL(2,C) of the Riemann sphere can be written as compositions of elements of PSU(2) and elements of Aut(C), the automorphism group of the complex plane?
 
  • #11
lugita15 said:
But I thought the stereographic projection IS how we understand the Riemann sphere as a sphere.
Stereographic projection, in its traditional form, tells you that if you delete the north pole from S^2 (a.k.a. the point at infinity) you get the plane. That is, stereographic projection is a map ##S^2 \backslash \{\infty\} \to \mathbb C##. An automorphism of the sphere doesn't necessarily respect this map: it could move the point ##\infty## around, i.e. the point at infinity could go to a point in the finite plane and vice versa.
Would it be correct to say that the transformations in PSU(2) correspond to rotations of the stereographic projection?
There seems to be some confusion in this thread. When you say rotation, what do you mean? Note that the map ##z\mapsto 1/z## is a dilation of the plane. But applied to the sphere, this map is a rotation.
 
  • #12
morphism said:
Stereographic projection, in its traditional form, tells you that if you delete the north pole from S^2 (a.k.a. the point at infinity) you get the plane. That is, stereographic projection is a map ##S^2 \backslash \{\infty\} \to \mathbb C##. An automorphism of the sphere doesn't necessarily respect this map: it could move the point ##\infty## around, i.e. the point at infinity could go to a point in the finite plane and vice versa.
OK, then I mean stereographic projection in an extended sense, i.e. including the point at infinity.
There seems to be some confusion in this thread. When you say rotation, what do you mean? Note that the map ##z\mapsto 1/z## is a dilation of the plane. But applied to the sphere, this map is a rotation.
I mean rotations of the stereographic projection of the Riemann sphere, which is a sphere S2. I want to know what transformations correspond to this, for which you seem to be saying that the answer is PSU(2). And the video seems to be saying that Aut(C) corresponds to translations of the stereographic projection. So I want to know whether the automorphisms of the Riemann sphere can be written a compositions of elements of PSU(2) and elements of AUT(C), i.e. rotations of the stereographic projection S2 and translations of the stereographic projection.
 
  • #13
I think you're missing my point about stereographic projection...but anyway, yes every automorphism of the Riemann sphere is a composition of elements of PSU(2) and elements of Aut(C). (In fact, you only need one element in PSU(2): namely the inversion z->1/z.) This is just a reformulation of the fact that everything is a composition of inversions, translations and dilations.
 
  • #14
morphism said:
I think you're missing my point about stereographic projection...but anyway, yes every automorphism of the Riemann sphere is a composition of elements of PSU(2) and elements of Aut(C). (In fact, you only need one element in PSU(2): namely the inversion z->1/z.) This is just a reformulation of the fact that everything is a composition of inversions, translations and dilations.
OK, then can you give me an example of a transformation in the automorphism group of the Riemann sphere that cannot be written as a composition of just inversions and translations i.e. a transformation that requires dilations as well? Or equivalently, why can't dilations be written as compositions of inversions and translations?
 
  • #15
lugita15 said:
OK, then can you give me an example of a transformation in the automorphism group of the Riemann sphere that cannot be written as a composition of just inversions and translations i.e. a transformation that requires dilations as well? Or equivalently, why can't dilations be written as compositions of inversions and translations?
You really should be able to figure this out yourself.

There are probably faster and more sophisticated proofs, but one low-level approach would be to write down the matrices corresponding to z->az, z->1/z and z->z+b, and show that no matter how you multiply out matrices of the latter two types, you'll never get a matrix of the type to z->az (unless a=1).
 
  • #16
morphism said:
You really should be able to figure this out yourself.

One approach would be to write down the matrices corresponding to z->az, z->1/z and z->z+b, and show that no matter how you multiply out matrices of the latter two types, you'll never get a matrix corresponding to z->az (unless a=1).
OK, first of all how in general do I find the transformation matrix corresponding to a complex function f(z)?

Second of all, based on the video it looks like all automorphisms of the Riemann sphere correspond to rigid body motions of the stereographic projection. But any rigid body motion can be written as a horizontal rotation plus a horizontal translation, which correspond respectively to inversions and translations in the complex plane. So how is it that a dilation, corresponding to a vertical translation of the sphere, cannot be written in that way?
 

FAQ: What Maps Belong to Aut(S2)/SO(3)?

What is Aut(S2)?

Aut(S2) refers to the automorphism group of the two-dimensional unit sphere, S2. It is the set of all isometries (rigid transformations) that preserve the structure of the sphere, such as rotations and reflections.

What is SO(3)?

SO(3) refers to the special orthogonal group in three dimensions. It is the set of all rotations in three-dimensional space that preserve orientation and have a determinant of 1.

What does it mean for something to belong to Aut(S2)/SO(3)?

To belong to Aut(S2)/SO(3) means that the element is a member of the quotient group formed by dividing Aut(S2) by SO(3). This group contains all the isometries of the sphere that are not just simple rotations, but also include reflections.

How do you determine what belongs to Aut(S2)/SO(3)?

In order to determine what belongs to Aut(S2)/SO(3), one would need to analyze the properties of the element in question and see if it satisfies the conditions for an isometry of the sphere that is not a simple rotation. This may involve performing calculations or using geometric reasoning.

What are some examples of elements that belong to Aut(S2)/SO(3)?

Some examples of elements that belong to Aut(S2)/SO(3) include reflections across the xy-plane, reflections across the yz-plane, and reflections across the xz-plane. These elements are not simple rotations, but they still preserve the structure of the sphere, making them members of the quotient group.

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