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1990"N'ã ‰ù‚©‚µ‚¢ ‚¨‚à‚¿‚á-Ht= u(ct)µ1t(yt−ct−(nδ)kt)µ2tνsλAt NtλA φ t, where yt= Aσ tk α t(1−sAt)1−α • First order necessary conditions ∂Ht/∂ct= 0, ∂Ht/∂sAt= 0 ρ¯= ∂Ht/∂kt µ1t µ˙1t µ1t, ρ¯= ∂Ht/∂At µ2t µ˙2t µ2t lim t→∞ µ1te −ρt¯ k t= 0, lim t→∞ µ2te −ρt¯ A t= 0 Romer (1990) and Jones (05) – p 28HansJoachim Wunderlich IEEE transactions on computeraided design of integrated circuits and Proceedings of IEEE International Conference on Computer Aided Design (ICCAD Proceedings 19th IEEE VLSI Test Symposium VTS 01, Y Tang, HJ Wunderlich, P Engelke, I Polian, B Becker, J Schlöffel,

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Universities in Japan since 1990, using administrative documents and articles of internship In conclusion, there are two characteristics of internships in Japanese universitiesLet C n(q,t)=h∇e n,s 1ni,whereh,i is the usual Hall scalar product defined by hs β,s µi =1ifβ = µ and 0 otherwise A few years ago Garsia and Haglund GH01, GH02 proved that C n(q,t)= X π qarea(π)tbounce(π), (8) where the sum is over all Catalan lattice paths β from (0,0) to (n,n), which are paths consisting of N (0,1) and E (1,0) steps which never go below the diagonal y = xHereH hâz lØ\o5a lpdjh msjlpdjh msjlpdjh msj_ÊdÚ(Ï °7ð

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