Question about Lagranges theorem in Group Theory

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SUMMARY

The discussion focuses on adapting the proof of Lagrange's theorem in group theory to demonstrate that \( g^{m!} \) is an element of subgroup \( H \) for any element \( g \) in finite group \( G \), where the order of \( G \) is \( m \) times the order of \( H \). The approach involves partitioning \( G \) into \( m \) left cosets of \( H \): \( H, gH, g^2H, \ldots, g^{m-1}H \). The bijective nature of the translation by \( g \) leads to the conclusion that \( g^mH \) must equal \( H \), inferring that \( g^m \) belongs to \( H \), and consequently, \( g^{m!} \) also belongs to \( H \).

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  • Familiarity with subgroup and coset definitions.
  • Knowledge of finite groups and their properties.
  • Basic algebraic manipulation involving exponents in group elements.
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  • Explore the properties of left cosets and their implications in group theory.
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Students of abstract algebra, particularly those studying group theory, as well as educators seeking to clarify Lagrange's theorem and its applications in finite groups.

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Homework Statement


If H is a subgroup of a finite group G, and if the order of G is m times the order of H, |G|=m|H|, adapt the proof of Lagrange's theorem to show that gm! is an element of H for all g in G.

The Attempt at a Solution


My thoughts so far were to think that we can divide G into m pieces: H, g1H, g2H, ..., gm-1H. If we now take an arbitrary gk, it is certainly in gkH, since H contains the identity. The question now is: what happens if we look at gk2, (gk2)3... where do they end up? I need a hint...
 
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If g is in H, there's nothing to prove; if not, consider the m (left) cosets:

[tex] H,gH,g^{2}H,...,g^{m-1}H[/tex]

Now, if you apply the translation by g again, you get:

[tex] gH,g^{2}H,...,g^{m}H[/tex]

But this translation is bijective, and that implies that [tex]g^{m}H[/tex] must be equal to what? And from this, what may be inferred about [tex]g^{m}[/tex] (and also [tex]g^{m!}[/tex])?
 

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