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  2. On asymptotic structure in compressed sensingBogdan Roman ∗, Ben ...

    www.damtp.cam.ac.uk/research/afha/anders/Asymptotic_10a.pdf
    24 Jul 2018: a)(a) (b)(b). (c)(c) (d)(d). Fig. 1. (a) 12.5% uniform random subsampling scheme, (b) CS reconstructionfrom uniform subsampling, (c) 12.5% multilevel subsampling scheme, (d) CS ... b}. The kth relative sparsity is. Sk = Sk(N,M,s) = maxzΘ‖PNk1Nk Uz‖.
  3. Compact schemes for laser-matter interaction in Schrödinger equation …

    www.damtp.cam.ac.uk/user/na/NA_papers/NA2018_03.pdf
    21 Apr 2018: Remark 1 Note that another variant of the splitting can be obtained by swapping thechoices of A and B. ... Comput. Phys. 230(15), 5930–5956. Compact schemes for laser-matter interaction 13. Amstrup, B., Doll, J.
  4. On asymptotic structure in compressed sensingBogdan Roman ∗, Ben ...

    www.damtp.cam.ac.uk/research/afha/people/anders/Asymptotic_10a.pdf
    24 Jul 2018: a)(a) (b)(b). (c)(c) (d)(d). Fig. 1. (a) 12.5% uniform random subsampling scheme, (b) CS reconstructionfrom uniform subsampling, (c) 12.5% multilevel subsampling scheme, (d) CS ... b}. The kth relative sparsity is. Sk = Sk(N,M,s) = maxzΘ‖PNk1Nk Uz‖.
  5. Advanced Quantum Field Theory Lent Term 2013 Hugh Osborn ...

    www.damtp.cam.ac.uk/user/examples/3P5a.pdf
    23 Jan 2018: f. (. b. )ZA,b. b=0. (1.112). 12. We can simplify this straight away by substituting in our previous result (1.104). ... b̄,. b. )ZB,b. b=0. (1.122). One finds that⟨ziz̄j⟩ = B1ij , (1.123).

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