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2: Recorded spectra for temperatures T1 and T2. 300 310 320 330 340 350 360 370 −10 −9 −8 −7 −6 −5 −4 −3 −2 −1 0 Temperature (K) W av el en gt h S hi ft (n m ) λ
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2: Recorded spectra for temperatures T1 and T2. 300 310 320 330 340 350 360 370 −10 −9 −8 −7 −6 −5 −4 −3 −2 −1 0 Temperature (K) W av el en gt h S hi ft (n m ) λ
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x t f x g x u= + (16) ( ) siny h x x h= = + θ (17) where the expressions for ( )f x and ( )g x are given in [Bobasu et al. 2005]. The
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je závislé především na teplotní roztažnosti masívu a západkovém mechanismu. 1 INTRODUCTION Our work extends the works of M. Hvozdara et al. [3] and J. Berger [7],
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