Inverse map is involutive: Difference between revisions

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===Proof of reversal law===
===Proof of reversal law===


This follows from associativity. Consider:
In order to show that the element <math>a_n^{-1}a_{n-1}^{-1}\ldots a_1^{-1}</math> is a two-sided inverse of <math>a_1a_2 \ldots a_n</math>, it suffices to show that their product both ways is the identity element. Consider first the product:


<math>a_1a_2 \ldots a_na_n^{-1}a_{n-1}^{-1}\ldots a_1^{-1}</math>
<math>(a_1a_2 \ldots a_{n-1}a_n)(a_n^{-1}a_{n-1}^{-1}\dots a_2^{-1}a_1^{-1})</math>


We first cancel <math>a_n</math> and <math>a_n^{-1}</math>, and keep proceeding in this way, till the whole word reduces to the identity element.
Due to associativity, we can drop the parentheses and we get:


A similar argument follows for the product:
<math>a_1a_2 \ldots a_{n-1}a_na_n^{-1}a_{n-1}^{-1}\dots a_2^{-1}a_1^{-1}</math>


<math>a_n^{-1}a_{n-1}^{-1}\ldots a_1^{-1}a_1a_2 \ldots a_n</math>
Now, consider the middle product <math>a_na_n^{-1}</math>. This is the identity element, and since the identity element has no effect on the remaining product, it can be removed, giving the product:
 
<math>a_1a_2 \ldots a_{n-1}a_{n-1}^{-1}\dots a_2^{-1}a_1^{-1}</math>
 
We now repeat the argument with the middle product <math>a_{n-1}a_{n-1}^{-1}</math> and ''cancel'' them. Proceeding this way, we are able to cancel all terms and eventually get the identity element.
 
A similar argument follows for the product the other way around:
 
<math>(a_n^{-1}a_{n-1}^{-1}\ldots a_1^{-1})(a_1a_2 \ldots a_n)</math>


Thus, the elements are two-sided inverses of each other.
Thus, the elements are two-sided inverses of each other.
'''Note''': In fact, it suffices to check only one of the two inverse conditions, i.e., check only that the first product is the identity element. This is because, in a group, every element has a two-sided inverse. Further, [[equality of left and right inverses in monoid]] forces any ''one-sided'' (left ''or'' right) inverse to be equal to the two-sided inverse.


===Proof for applying it twice===
===Proof for applying it twice===

Latest revision as of 19:39, 31 March 2022

This article gives the statement, and possibly proof, of a basic fact in group theory.
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Statement

The inverse map in a group, i.e. the map sending any element of the group, to its inverse element, is an involutive map, in the sense that it has the following two properties:

  • It satisfies the reversal law:

(a1a2an)1=an1an11a11

  • Applying it twice sends an element to itself:

(a1)1=a

It fact, both these are true in the greater generality of a monoid, under the condition that all the ais have two-sided inverse ai1 (note: we still need a monoid to guarantee that two-sided inverses, when they exist, are unique).

Proof

Proof of reversal law

In order to show that the element an1an11a11 is a two-sided inverse of a1a2an, it suffices to show that their product both ways is the identity element. Consider first the product:

(a1a2an1an)(an1an11a21a11)

Due to associativity, we can drop the parentheses and we get:

a1a2an1anan1an11a21a11

Now, consider the middle product anan1. This is the identity element, and since the identity element has no effect on the remaining product, it can be removed, giving the product:

a1a2an1an11a21a11

We now repeat the argument with the middle product an1an11 and cancel them. Proceeding this way, we are able to cancel all terms and eventually get the identity element.

A similar argument follows for the product the other way around:

(an1an11a11)(a1a2an)

Thus, the elements are two-sided inverses of each other.

Note: In fact, it suffices to check only one of the two inverse conditions, i.e., check only that the first product is the identity element. This is because, in a group, every element has a two-sided inverse. Further, equality of left and right inverses in monoid forces any one-sided (left or right) inverse to be equal to the two-sided inverse.

Proof for applying it twice

This is direct from the definition. let b=a1. Then, by the inherent symmetry in the definition of inverse element, we see that a=b1.

More explicitly, if b=a1, that means that ab=ba=e. But this is precisely the condition for stating that a=b1.

References

Textbook references

  • Abstract Algebra by David S. Dummit and Richard M. Foote, 10-digit ISBN 0471433349, 13-digit ISBN 978-0471433347, More info, Page 18, Proposition 1