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Unit 1: Vector Space over Fields




          This theorem can be generalised as:                                                   Notes
          if a, b, c, … k, l, m   G, then
                                                     –1
                                                         –1
                                                             –1
                                             –1
                    (a o b o c o … k o l o m) –1  = m  o l  o k  o. .c  o b  o a .
                                                 –1
                                          –1
          Theorem 5: Cancellation laws hold good in a group, i.e., if a, b, c, are any elements of G, then
                                   a o b = a o c   b = c             (left cancellation law)
          and                      b o a = c o a   b = c            (right cancellation law)
          Proof: Let a   G. Then
                         –1
                 a  G   a   G such that a  o a = e
                                       –1
                 = a o a , where e is the identity element
                      –1
          Now, let us assume that
                 a o b = a o c
          then   a o b = a o c   a  o (a o b) = a  o aoc
                                       –1
                             –1
                     –1
                    (a  oa) ob = (a  oa) oc (by associative law)
                              –1
                                        –1
                    eob = eoc   (because a  oa = e)
                    b = c.
          Similarly, b o a = c o a

                    (boa) o a  = (coa) o a –1
                          –1
                                  –1
                    bo (ao a ) = co (ao a )
                         –1
                    boe = coe
                    b = c.

          Theorem 6: If G is a group with binary operation o and if a and b are any elements of G, then the
          linear equations
                                         aox = b and yoa = b

          have unique solutions in G.
                                 –1
          Proof: Now     a   G   a    G,
                         –1
                                       –1
          and            a    G, b   G   a  ob   G.
          Substituting a  ob for x in the equation aox = b, we obtain
                     –1
                             a o (a  o b) = b
                              –1
                           (a o a ) o b = b
                               –1
                           e o b = b
                           b = b       [because e is identity]

                  –1
          Thus x = a  ob is a solution of the equation aox = b.
          To show that the solution is unique let us suppose that the equation aox = b has two solutions
          given  by

                                          x = x  and x = x
                                              1       2




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