Does associativity imply bijectivity in group operations?

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SUMMARY

The discussion centers on the relationship between group operations and bijectivity within group theory. Participants explore whether associativity of a group operator implies that the operator is bijective. They reference specific groups such as S3 and S2, discussing subgroup properties and the implications of group order. The consensus is that while a group operation can be bijective, it is not inherently so by definition, particularly in the context of finite versus infinite groups.

PREREQUISITES
  • Understanding of group theory concepts, including group operations and bijections.
  • Familiarity with specific groups such as S3 (symmetric group) and S2 (symmetric group on two elements).
  • Knowledge of group homomorphisms and their role in group actions.
  • Basic comprehension of finite and infinite groups and their properties.
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  • Study the properties of group homomorphisms and their implications for group actions.
  • Explore the concept of group actions in detail, particularly in relation to symmetric groups.
  • Investigate the differences between finite and infinite groups, focusing on bijectivity of operations.
  • Examine the implications of group order and subgroup relationships in various group structures.
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Mathematicians, students of abstract algebra, and anyone interested in deepening their understanding of group theory and its applications in various mathematical contexts.

  • #31
Stephen Tashi said:
Are you/we distinguishing between a "group operator" and a "group action"?
If I understand right, a group action is like a group operating on a set, but I'm still learning (think groups 101). Anyhow, my initial question seems silly in hindsight, or maybe I'm missing something. I just assumed that the operator was inherently bijective, but I never read anywhere that it was, and I'm not sure how to drive the truth of that question base on the definition of a group.
 
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  • #32
valenumr said:
If I understand right, a group action is like a group operating on a set, but I'm still learning (think groups 101). Anyhow, my initial question seems silly in hindsight, or maybe I'm missing something. I just assumed that the operator was inherently bijective, but I never read anywhere that it was, and I'm not sure how to drive the truth of that question base on the definition of a group.
And to clarify a little, it seems obvious for finite groups, but may be a little more messy for infinite groups. I expect aG (or Ga) to recover all elements of the group for all a in G. I haven't had time to revisit the concept with infinite groups just yet.
 
  • #33
valenumr said:
If I understand right, a group action is like a group operating on a set, but I'm still learning (think groups 101). Anyhow, my initial question seems silly in hindsight, or maybe I'm missing something. I just assumed that the operator was inherently bijective, but I never read anywhere that it was, and I'm not sure how to drive the truth of that question base on the definition of a group.
Consider a group homomorphism ##\varphi \, : \, G \longrightarrow \operatorname{Sym}(X)## which means ##\varphi(g\cdot h)(x)=\varphi (g)(\varphi (h)(x)).## ##G## is the group here, and ##X## a set, ##\operatorname{Sym}(X)## the symmetry group of ##X,## i.e. the group that shuffles the elements of ##X##.

Now you can say ##G## acts on ##X##, ##G## acts on ##X## via ##\varphi ##, ##G## operates on ##X##, ##G## operates on ##X## via ##\varphi ##, or ##(G,\varphi )## is a representation of ##G## on ##X##. These are all the same, and people often write ##g.x## instead of ##\varphi (g)(x).## The homomorphism property is then written as an operation property ##(g\cdot h).x=g.(h.x).##

The term representation is often reserved for linear representations. This is when ##X=V## is a vector space and ##G## operates via regular linear functions, i.e. ##\varphi \, : \,G\longrightarrow \operatorname{GL}(V).## Then we call ##V## the representation space. ##G## still acts or operates on ##V,## only by certain functions (isomorphisms of ##V##) and not all bijections of ##X=V.##
 
  • #34
fresh_42 said:
Consider a group homomorphism ##\varphi \, : \, G \longrightarrow \operatorname{Sym}(X)## which means ##\varphi(g\cdot h)(x)=\varphi (g)(\varphi (h)(x)).## ##G## is the group here, and ##X## a set, ##\operatorname{Sym}(X)## the symmetry group of ##X,## i.e. the group that shuffles the elements of ##X##.

Now you can say ##G## acts on ##X##, ##G## acts on ##X## via ##\varphi ##, ##G## operates on ##X##, ##G## operates on ##X## via ##\varphi ##, or ##(G,\varphi )## is a representation of ##G## on ##X##. These are all the same, and people often write ##g.x## instead of ##\varphi (g)(x).## The homomorphism property is then written as an operation property ##(g\cdot h).x=g.(h.x).##

The term representation is often reserved for linear representations. This is when ##X=V## is a vector space and ##G## operates via regular linear functions, i.e. ##\varphi \, : \,G\longrightarrow \operatorname{GL}(V).## Then we call ##V## the representation space. ##G## still acts or operates on ##V,## only by certain functions (isomorphisms of ##V##) and not all bijections of ##X=V.##
Honestly, you are a bit ahead of me. I'm not quite clear on the difference between homomorphism and isomorphism, though they look very similar to me at the moment.
 
  • #35
fresh_42 said:
Consider a group homomorphism ##\varphi \, : \, G \longrightarrow \operatorname{Sym}(X)## which means ##\varphi(g\cdot h)(x)=\varphi (g)(\varphi (h)(x)).## ##G## is the group here, and ##X## a set, ##\operatorname{Sym}(X)## the symmetry group of ##X,## i.e. the group that shuffles the elements of ##X##.

Now you can say ##G## acts on ##X##, ##G## acts on ##X## via ##\varphi ##, ##G## operates on ##X##, ##G## operates on ##X## via ##\varphi ##, or ##(G,\varphi )## is a representation of ##G## on ##X##. These are all the same, and people often write ##g.x## instead of ##\varphi (g)(x).## The homomorphism property is then written as an operation property ##(g\cdot h).x=g.(h.x).##

The term representation is often reserved for linear representations. This is when ##X=V## is a vector space and ##G## operates via regular linear functions, i.e. ##\varphi \, : \,G\longrightarrow \operatorname{GL}(V).## Then we call ##V## the representation space. ##G## still acts or operates on ##V,## only by certain functions (isomorphisms of ##V##) and not all bijections of ##X=V.##
By the way, when you say symmetry group, do you me the maximal (I think) order group for X?
 
  • #36
valenumr said:
By the way, when you say symmetry group, do you me the maximal (I think) order group for X?
I mean the group of all bijective functions ##X \longrightarrow X##.
 
  • #37
fresh_42 said:
I mean the group of all bijective functions ##X \longrightarrow X##.
Ok, I think that's in line with what I thought, basically Sn from my material.
 
  • #38
valenumr said:
Ok, I think that's in line with what I thought, basically Sn from my material.
Eh, let me walk that back a little. I mean, I'm still working on things where group operators are essentially scalar operations. I'm not sure what to expect yet when it goes beyond that.
 
  • #39
Stephen Tashi said:
Are you/we distinguishing between a "group operator" and a "group action"?
I thought about this for a while, because, as I've mentioned, pretty much all of the material examples I've encountered so far have been based on integers, with a sprinkling of reals, and mostly finite groups. Think like an advanced ninth grader or typical eleventh grader could probably easily handle the material.

In any case, my consideration would be a nice Persian rug I happen to own. It does have multiple symmetries, say left / right reflection, front back reflection, and top / bottom reflection.

So when I say "group operator", I'm thinking of the concept of one element of the group composed with another (single) element of the group. When you say "group action", which I expect is more appropriate, it's like rotating the carpet some multiple of pi / 2 on the floor, or maybe flipping it over. It affects the whole rug, but it is just applying the operator to every element.

I'm still trying to think about non-unitary stuff as well that might shrink my rug, for example. But I don't what to get ahead of the material.

In any case, my other comment about working with scalars is mostly a reflection. I suspect that whole "abstract" part of abstract algebra doesn't really care about the group elements or group operator, so long as the rules apply.
 

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