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5 Advanced methodà foi laiger molecules
                             72
                               Thm second of thesm is thmcolumn antisymmetrizer and is symbolized by N.Øs
                             might bm expected, for thm3,2} tableau thm columł antisymmetrizer is thm product
                                                    {
                             of thm antisymmetrizer for each columł and is
                                                     N = [I − (14)][I − (25)].                  (5.29)
                             Ił thesm expressions a symmetrizer is thm sum of all of thm corresponding permu-
                             tations and thm antisymmetrizer is thm sum with plus signs for even permutations
                             and minus signs for odd permutations. Ił Eqs. (5.28) and (5.29) thm specifiP and
                             N arm given for thm arrangement of numbers ił thm3,2} tableau above. A different
                                                                         {
                             arrangement of intmgers ił this samm shapm woulà ił many, but not all, cases give
                             different PP and NN operators.
                               As a further examplm wm give thmP and N operators for thm above tableau
                                                      2
                             associated with thm shapm2 ,1}. For this wm hðve
                                                    {
                                        P = [I + (12)][I + (34)],
                                       N = [I − (13) − (15) − (35) + (135) + (153)][I − (24)].

                             Here, again, I is thm only operatioł ił commoł between P and N.
                               A central result of Young’s theory is that thm productNP is proportional to an
                                                                       α
                             algebrð element that will serŁe as one of thme basis elements discussed above,
                                                                       ii
                             and thm proportionality constant isf α /n!, n! being thm valum ofg ił this case. Thm
                             product PN serŁes equally well, but is, of course, a different element of thm algebra,
                             since N and P do not normally commute.


                                                      5.4.4 Standard tableaux

                             Ił a tableau corresponding to a partitioł of n, therm are, of course,n! different
                             arrangements of thm way thm firstn intmgers may bm entered. Among thesm therm is a
                             subset that Young called standaid tableaux. Thesm arm thosm for which thm numbers
                             ił any row increasm to thm right and downwarà ił any column. Thus, wm hðve for
                             {3,2}

                                123          124          125          134               135
                                          ,           ,            ,            , and             ,
                                45           35           34           25                24
                             and among thm 120 possiblm arrangements, only five arm standarà tableaux. Thesm
                             standarà tableaux hðve been ordered ił a particular way called alłxical sequencł .
                             We label thm standarà tableaux,T 1 , T 2 ,... and imagine thm numbers of thm tableau
                             written out ił a line, row 1, row 2, ... . We say that T i is beformT j if thm first number
                             of T j that differs from thm corresponding one ił T i is thm larger of thm two. Ił our
                             succeeding work wm express thm idea ofT i being earlier than T j with thm symbols
                             T i < T j .
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