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21 - 30 of 1,743 search results for KA :PC53 24 where 0 match all words and 1,743 match some words.
  1. Results that match 2 of 3 words

  2. arX iv:q uant -ph/ 0409 078 v1 14 S ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI04027
    p(m)qkd (kA,kB) = Pr(KA = kA,KB = kB|M = m). (1). ... KA, kA, KB, kB: output keys for Alice and Bob.
  3. UMMAP7.dvi

    https://api.newton.ac.uk/website/v0/events/preprints/NI05032
    1. 5 Towards an infinite-dimensional Implicit Function Theorem 23. 6 Polynomials in additive operators 24. ... KA], [KU4]). These polynomials are defined suchthat the following Taylor expansion holds in arbitrary characteristic:.
  4. Definable sets in algebraically closed valuedfields: elimination of…

    https://api.newton.ac.uk/website/v0/events/preprints/NI05050
    Definable sets in algebraically closed valuedfields: elimination of imaginaries. Deirdre Haskell Ehud Hrushovski † Dugald Macpherson ‡. July 19, 2005. 2000 Mathematics Subject Classification: 03C60. Abstract.It is shown that if K is an
  5. On a class of 2-surface observables in general relativity ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI06005
    Then the time–space projection of the Killing operator acting on Ka is [3,4]. ... aAa, andthe third term is also zero because Ka is a Killing vector.
  6. DEFINABLE RELATIONS IN THE REAL FIELDWITH A DISTINGUISHED SUBGROUP ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI06008
    Then a kA and so theset {b : kb = a} is not empty. ... Mathematical Institute, University of Oxford, 24–29 St Giles, Oxford, OX1 3LB,United Kingdom.
  7. cimenotes.dvi

    https://api.newton.ac.uk/website/v0/events/preprints/NI06034
    1. k,g. γ2. )u = 0. This means that the link between the physical parameters (g,k,γ) and themathematical parameters is :. δ =g. γ2, h =. 1. k. (2.24). The ... 24. we can construct a solution uh = a(x,h) exp ϕ(x)h in the neighborhood ofx0.Let us
  8. DW_review.dvi

    https://api.newton.ac.uk/website/v0/events/preprints/NI06048
    eA0′fA = 0, (24). eA1′fA = 0. (25). 13. Define the almost complex structure J by. ... In spinors, if Ka = ιAoA. ′. then an α-plane distribution is defined by oA′. ,
  9. Bar categories and star operations E.J. Beggs & S. ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI07014
    Isaac Newton Institute, Cambridge CB3 0EH. December 24, 2006. Abstract. We introduce the notion of ‘bar category’ by which we mean a monoidal categoryequipped with additional structure induced by complex conjugation. ... l1m=0. q2 m2. ) l1n,a=0. (q q1
  10. SET THEORETIC SOLUTIONS OF THE YANG-BAXTEREQUATION, GRAPHS AND…

    https://api.newton.ac.uk/website/v0/events/preprints/NI07033
    4 TATIANA GATEVA-IVANOVA AND SHAHN MAJID. Proposition 1.12. [GIM, Proposition 2.24] Let (X,r) be a quadratic set. ... 24. Example 2.5. Let (X,r) be the nondegenerate involutive square-free solution with.
  11. EQUALITY OF LIFSHITZ AND VAN HOVE EXPONENTS ONAMENABLE CAYLEY ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI07039
    This has beenshown for periodic operators in [14, 24] and for site percolation Hamiltonians in [31]. ... s1λN1. kA(s), where N1. kA is the IDS of the. rescaled adjacency operator 1kA.

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