By Gerhard Larcher, Friedrich Pillichshammer, Arne Winterhof, Chaoping Xing
Harald Niederreiter's pioneering study within the box of utilized algebra and quantity conception has resulted in vital and sizeable breakthroughs in lots of parts. This choice of survey articles has been authored via shut colleagues and major specialists to mark the get together of his seventieth birthday. The e-book presents a contemporary review of alternative learn parts, masking uniform distribution and quasi-Monte Carlo equipment in addition to finite fields and their functions, specifically, cryptography and pseudorandom quantity iteration. Many effects are released right here for the 1st time. The publication serves as an invaluable start line for graduate scholars new to those components or as a refresher for researchers desirous to persist with fresh tendencies.
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Extra info for Applied Algebra and Number Theory
In fact, for a = 0 ∈ Ftp and b ∈ P ⊥ D(0,b) f (x) = P(x) · (y + b) − P(x) · y = P(x) · b = 0. For details of the construction of plateaued Boolean functions without a linear structure we refer to [18, Section VIII]. 8), obtained by the Maiorana–McFarland construction are again quadratic. Partially bent functions which are not quadratic can easily be obtained from nonquadratic bent funcn tions. Let f be a bent function from Fn−s p to F p , and let f 1 : F p → F p be given as f 1 (x1 , . . , xn−s , .
45] H. Niederreiter and C. P. Xing, Explicit global function fields over the binary field with many rational places. Acta Arith. 75, 383–396, 1996.  H. Niederreiter and C. P. Xing, Cyclotomic function fields, Hilbert class fields and global function fields with many rational places. Acta Arith. 79, 59–76, 1997.  H. Niederreiter and C. P. Xing, Drinfeld modules of rank 1 and algebraic curves with many rational points II. Acta Arith. 81, 81–100, 1997.  H. Niederreiter and C. P. Xing, Global function fields with many rational places over the ternary field.
For instance, the isotropic discrepancy is defined with respect to the collection C of convex subsets of [0, 1]s . The local isotropic discrepancy is in this case defined by 1 PN ,s (C) = N N −1 1C (x n ) − λs (C), n=0 where C ∈ C is a convex set and λs is the s-dimensional Lebesgue measure. The isotropic discrepancy is then defined by DC∗ (PN,s ) = sup C∈C PN ,s (C) . The connection to numerical integration is not as clear in this case as for the case of anchored boxes. Again, a number of results are known about the isotropic discrepancy due to Beck , Hlawka , Laczkovich , Mück and Philipp , Niederreiter [42, 43], Niederreiter and Wills , Schmidt , Stute  and Zaremba .