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Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

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29.5 THE ORTHOGONALITY THEOREM FOR IRREDUCIBLE REPRESENTATIONSMore mathematically, if we denote the entry in the ith row <strong>and</strong> jth column of amatrix D(X) by[D(X)] ij ,<strong>and</strong> ˆD (λ) <strong>and</strong> ˆD (µ) are two irreps of G having dimensionsn λ <strong>and</strong> n µ respectively, then∑ [ ]ˆD (λ) ∗ [(X) ˆD (X)](µ) = g δ ik δ jl δ λµ . (29.13)ijkl nXλThis rather <strong>for</strong>bidding-looking equation needs some further explanation.Firstly, the asterisk indicates that the complex conjugate should be taken ifnecessary, though all our representations so far have involved only real matrixelements. Each Kronecker delta function on the right-h<strong>and</strong> side has the value 1if its two subscripts are equal <strong>and</strong> has the value 0 otherwise. Thus the right-h<strong>and</strong>side is only non-zero if i = k, j = l <strong>and</strong> λ = µ, all at the same time.Secondly, the summation over the group elements X means that g contributionshave to be added together, each contribution being a product of entries drawnfrom the representative matrices in the two irreps ˆD (λ) = { ˆD (λ) (X)} <strong>and</strong> ˆD (µ) ={ ˆD (µ) (X)}. Theg contributions arise as X runs over the g elements of G.Thus, putting these remarks together, the summation will produce zero if either(i) the matrix elements are not taken from exactly the same position in everymatrix, including cases in which it is not possible to do so because theirreps ˆD (λ) <strong>and</strong> ˆD (µ) have different dimensions, or(ii) even if ˆD (λ) <strong>and</strong> ˆD (µ) do have the same dimensions <strong>and</strong> the matrix elementsare from the same positions in every matrix, they are different irreps, i.e.λ ≠ µ.Some numerical illustrations based on the irreps A 1 ,A 2 <strong>and</strong> E of the group 3m(or C 3v or S 3 ) will probably provide the clearest explanation (see (29.12)).(a) Take i = j = k = l = 1, with ˆD (λ) =A 1 <strong>and</strong> ˆD (µ) =A 2 . Equation (29.13)then reads1(1) + 1(1) + 1(1) + 1(−1) + 1(−1) + 1(−1) = 0,as expected, since λ ≠ µ.(b) Take (i, j) as(1, 2) <strong>and</strong> (k, l) as(2, 2), corresponding to different matrixpositions within the same irrep ˆD (λ) = ˆD (µ) = E. Substituting in (29.13)gives(0(1) +− √ 32) (−12)+( √32) (− ) (12 +0(1)+− √ 32) (−12)+( √32) (−12)=0.(c) Take (i, j) as(1, 2), <strong>and</strong> (k, l) as(1, 2), corresponding to the same matrixpositions within the same irrep ˆD (λ) = ˆD (µ) = E. Substituting in (29.13)gives(0(0)+− √ 32)(− √ 32)+( √32)( √32) (+0(0)+− √ 32)(− √ 32)+( √32)( √32)= 6 2 .1091

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