ar X iv : m at h . O C / 0 60 16 58 v 2 2 3 Ju n 20 06 FurtherResults onStrictLyapunovFunctions for RapidlyTime - VaryingNonlinear Systems ⋆

ar X iv : m at h / 06 01 65 8 v 2 [ m at h . O C ] 2 3 Ju n 20 06 FurtherResults onStrictLyapunovFunctions for RapidlyTime - VaryingNonlinear Systems ⋆

We explicitly construct global strict Lyapunov functions for rapidly time-varying nonlinear control systems. The Lyapunov functions we construct are expressed in terms of oftentimes more readily available Lyapunov functions for the limiting dynamics which we assume are uniformly globally asymptotically stable. This leads to new sufficient conditions for uniform global exponential, uniform globa...

2 6 Ja n 20 06 FurtherResults onStrictLyapunovFunctions for RapidlyTime - VaryingNonlinear Systems ⋆

We explicitly construct global strict Lyapunov functions for rapidly time-varying nonlinear control systems. The Lyapunov functions we construct are expressed in terms of oftentimes more readily available Lyapunov functions for the limiting dynamics which we assume are uniformly globally asymptotically stable. This leads to new sufficient conditions for uniform global exponential, uniform globa...

ar X iv : m at h / 06 06 67 1 v 1 [ m at h . A C ] 2 7 Ju n 20 06 PRÜFER ⋆ – MULTIPLICATION DOMAINS AND ⋆ – COHERENCE

ar X iv : 1 60 2 . 07 58 8 v 3 [ he p - ex ] 1 4 Ju n 20 16 FERMILAB - PUB

ar X iv : h ep - p h / 02 06 27 0 v 1 2 6 Ju n 20 02 1 The charge asymmetry from Pomeron - Odderon interference in hard