math 3230 abstract algebra i sec 5 2 the orbit stabilizer
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Math 3230 Abstract Algebra I Sec 5.2: The orbit-stabilizer theorem - PowerPoint PPT Presentation

Math 3230 Abstract Algebra I Sec 5.2: The orbit-stabilizer theorem Slides created by M. Macauley, Clemson (Modified by E. Gunawan, UConn) http://egunawan.github.io/algebra Abstract Algebra I Sec 5.2 The orbit-stabilizer theorem Abstract


  1. Math 3230 Abstract Algebra I Sec 5.2: The orbit-stabilizer theorem Slides created by M. Macauley, Clemson (Modified by E. Gunawan, UConn) http://egunawan.github.io/algebra Abstract Algebra I Sec 5.2 The orbit-stabilizer theorem Abstract Algebra I 1 / 9

  2. Orbits, stabilizers, and fixed points Suppose G acts on a set S . Pick a configuration s ∈ S . We can ask two questions about it: (i) What other states (in S ) are reachable from s ? (We call this the orbit of s .) (ii) What group elements (in G ) fix s ? (We call this the stabilizer of s .) Definition 2 Suppose that G acts on a set S (on the right) via φ : G → Perm( S ). (i) The orbit of s ∈ S is the set Orb( s ) = { s .φ ( g ) | g ∈ G } . (ii) The stabilizer of s in G is Stab( s ) = { g ∈ G | s .φ ( g ) = s } . (iii) An element s ∈ S is called a fixed point of the action if Orb( s ) is of size one. That is, the set of fixed points of the action is Fix( φ ) = { s ∈ S | s .φ ( g ) = s for all g ∈ G } . Note that the orbits of φ are the connected components in the action diagram. Sec 5.2 The orbit-stabilizer theorem Abstract Algebra I 2 / 9

  3. Orbits, stabilizers, and fixed points Let’s revisit Example 2: 0 1 0 0 1 0 1 0 1 1 1 0 0 0 1 0 0 1 1 1 0 0 0 1 0 1 0 0 The orbits are the 3 connected components. There is only one fixed point of φ . The stabilizers are: � � � � � � 0 0 0 1 = { e , r 2 , rf , r 3 f } , 0 0 Stab = D 4 , Stab Stab = { e , f } , 0 0 1 0 1 1 � � � � 1 0 = { e , r 2 , rf , r 3 f } , 1 0 = { e , r 2 f } , Stab Stab 0 1 1 0 � � 1 1 Stab = { e , f } , 0 0 � � Observations? 0 1 = { e , r 2 f } . Stab 0 1 Example 4: G = C 2 = { e , g } and S = Z . Let G acts on S by x .φ ( g ) = − x . Orb(0) = { 0 } , and the orbit of any other element x in S is the set {− x , x } . Stab(0) = C 2 , but the stabilizer of any other element of S is { e } . Fix( φ ) = { 0 } . Sec 5.2 The orbit-stabilizer theorem Abstract Algebra I 3 / 9

  4. Orbits and stabilizers Proposition 1 For any s ∈ S , the set Stab( s ) is a subgroup of G . Proof (outline) - see actual proof in video To show Stab( s ) is a group, we need to show three things: (i) Contains the identity . That is, s .φ ( e ) = s . (ii) Inverses exist . That is, if s .φ ( g ) = s , then s .φ ( g − 1 ) = s . (iii) Closure . That is, if s .φ ( g ) = s and s .φ ( h ) = s , then s .φ ( gh ) = s . You’ll do this on the homework. Remark The kernel of the action φ is the set of all group elements that fix everything in S : Ker φ = { g ∈ G | φ ( g ) = e } = { g ∈ G | s .φ ( g ) = s for all s ∈ S } . Notice that � Ker φ = Stab( s ) . s ∈ S Sec 5.2 The orbit-stabilizer theorem Abstract Algebra I 4 / 9

  5. Lemma 1: Bijection between orbits and right cosets of the stabilizer Lemma 1 For any group action φ : G → Perm( S ), and any x ∈ S , There is a bijection f : Orb( x ) → G / Stab ( x ). Let’s look at our previous example to get some intuition for why this should be true. 0 0 1 0 0 0 G = D 4 and H = � f � Let x = 1 1 1 0 1 1 Then Stab( x ) = � f � . e r r 2 r 3 Partition of D 4 by the right cosets of H : fr 2 fr 3 f fr 0 1 1 1 0 1 0 0 Hr 2 Hr 3 H Hr Here, x .φ ( g ) = x .φ ( k ) iff g and k are in the same right coset of H in G . Sec 5.2 The orbit-stabilizer theorem Abstract Algebra I 5 / 9

  6. Theorem 1 (The Orbit-Stabilizer Theorem) The following is a central result of group theory. Orbit-Stabilizer theorem For any group action φ : G → Perm( S ), and any x ∈ S , | Orb( x ) | · | Stab( x ) | = | G | . if G is finite. Proof of Orbit-Stabilizer theorem Since Stab( s ) < G , Lagrange’s theorem tells us that [ G : Stab( x )] · | Stab( x ) | = | G | . � �� � � �� � number of cosets size of subgroup Thus, it suffices to show that | Orb( x ) | = [ G : Stab( x )]. By Lemma 1, there is a bijection between the elements of Orb( x ) and the right cosets of Stab( x ). Sec 5.2 The orbit-stabilizer theorem Abstract Algebra I 6 / 9

  7. Proof of Lemma 1 part (i) Lemma 1 For any group action φ : G → Perm( S ), and any x ∈ S , there is a bijection f : Orb( x ) → G / Stab( x ). Proof of Lemma, (i) defining f and showing that f is well-defined Throughout, let H = Stab( x ). We define f : Orb( x ) → G / H as follows. If s ∈ Orb( x ), then there is g ∈ G such that s = x .φ ( g ) by def of Orb( x ), and we define f ( s ) = Hg . (i) First, we show that f is well-defined, independent of the choice of g ∈ G such that x .φ ( g ) = s . We need to show: if two group elements both send x to s ∈ S, then the two group elements are in the same coset. Suppose g , k ∈ G both send x ∈ S to s ∈ S . This means: ( x .φ ( g )) .φ ( k ) − 1 = ( x .φ ( k )) .φ ( k ) − 1 x .φ ( g ) = x .φ ( k ) ⇒ ( x .φ ( g )) .φ ( k − 1 ) = ( x .φ ( k )) .φ ( k − 1 ) ⇒ x .φ ( gk − 1 ) = x .φ ( kk − 1 ) ⇒ since φ is a right group action x .φ ( gk − 1 ) = x .φ ( e ) ⇒ x .φ ( gk − 1 ) = x ⇒ (since φ sends e to the identity permutation) gk − 1 stabilizes x ⇒ gk − 1 ∈ H ⇒ (recall that H = Stab( x )) ⇒ g ∈ Hk ⇒ Hg = Hk Sec 5.2 The orbit-stabilizer theorem Abstract Algebra I 7 / 9

  8. Proof of Lemma 1 part (ii) injectivity Proof of Lemma (cont.), (ii) showing that f is injective Suppose (a.) x 1 , x 2 ∈ Orb( x ) such that (b.) f ( x 1 ) = f ( x 2 ). By (a), there exist g 1 , g 2 ∈ G such that x 1 = x .φ ( g 1 ) x 2 = x .φ ( g 2 ) , with Hg 1 = Hg 2 , due to (b). Then hg 1 = g 2 for some h ∈ H = Stab( x ). (1) So x 2 = x .φ ( g 2 ) = x .φ ( hg 1 ) by (1) = ( x .φ ( h )) .φ ( g 1 ) since φ is a right group action = x .φ ( g 1 ) since x .φ ( h ) = x due to h ∈ H = Stab( x ) = x 1 . Sec 5.2 The orbit-stabilizer theorem Abstract Algebra I 8 / 9

  9. Proof of Lemma 1 part (iii) surjectivity Proof of Lemma (cont.), (iii) showing that f is onto (iii) Finally, we show that f is onto. Let Hg 1 ∈ G / H . Then let x 1 := x .φ ( g 1 ), which means that x 1 ∈ Orb( x ). Then f ( x 1 ) = Hg 1 . Sec 5.2 The orbit-stabilizer theorem Abstract Algebra I 9 / 9

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