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First Permian occurrence of the shark egg capsule morphotype Palaeoxyris Brongniart, 1828
Hamad A., Fischer J., Voigt S., Kerp H., Schneider J., Scholze F.
. Fischer, S. Voigt, H. Kerp, J. W. Schneider, and F. Scholze. 2016. First Permian occurrence of the shark
First Permian occurrence of the shark egg capsule morphotype Palaeoxyris Brongniart, 1828
Hamad A., Fischer J., Voigt S., Kerp H., Schneider J., Scholze F.
. Fischer, S. Voigt, H. Kerp, J. W. Schneider, and F. Scholze. 2016. First Permian occurrence of the shark
A globally convergent lp-Newton method
Fischer A., Herrich M., Izmailov A.F., Solodov M.V.
A globally convergent LP-Newton method for piecewise smooth constrained equations: escaping nonstationary accumulation points
Fischer A., Herrich M., Izmailov A.F., Scheck W., Solodov M.V.
Spin diffusion in melts of entangled polymers
Fischer E., Kimmich R., Fatkullin N.
Based on theoretical considerations [N. F. Fatkullin, Sov. Phys. JETP 72, 563 (1991)], immaterial
Effect of substituting Fe by Mn in GdFeO3 perovskite catalyst for CO hydrogenation
Sharaeva A.A., Sheshko T.F., Kryuchkova T.A., Yafarova L.V., Zvereva I.А.
Fischer-Tropsch synthesis
The confined-to-bulk dynamics transition of polymer melts in nanoscopic pores of solid matrices with varying pore diameter
Fatkullin N., Kimmich R., Fischer E., Mattea C., Beginn U., Kroutieva M.
only if the pore diameter complies with the limit dpore ≫ (b3/k BTκT )1/3RF ≈ 10R F , where b
Local Attractors of Newton-Type Methods for Constrained Equations and Complementarity Problems with Nonisolated Solutions
Fischer A., Izmailov A.F., Solodov M.V.
Spin diffusion in melts of entangled polymers
Fischer E., Kimmich R., Fatkullin N.
Based on theoretical considerations [N. F. Fatkullin, Sov. Phys. JETP 72, 563 (1991)], immaterial
The confined-to-bulk dynamics transition of polymer melts in nanoscopic pores of solid matrices with varying pore diameter
Fatkullin N., Kimmich R., Fischer E., Mattea C., Beginn U., Kroutieva M.
only if the pore diameter complies with the limit dpore ≫ (b3/k BTκT )1/3RF ≈ 10R F , where b

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