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41 - 50 of 2,148 search results for tj KaKaotalk:PC53 where 0 match all words and 2,148 match some words.

  1. Results that match 1 of 2 words

  2. EIGENVECTOR LOCALIZATION FOR RANDOM BAND MATRICES WITH POWER LAW ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI09019
    Tj Pj1Y1+ Pj1T. †j , T. †j1Pj1YPj1Tj1 AW. By Prop. 5 Pj Y1Pj AW. ... Lemma 3.2 (Lemma W for XW ;nW ). Let Vj, Tj, j = 1,. ,

  3. SPADES AND MIXTURE MODELS FLORENTINA BUNEA ALEXANDRE B. TSYBAKOV ...

    https://api.newton.ac.uk/website/v0/events/preprints/NI09022
    δ/2 M. j=1. P{ω̄j > ωj}. Define. tj = 2Ef4j (X1)Ef2j (X1). ... log(2M/δ)n. and note that. 2n. ni=1. f2j (Xi) tj T 2j.

  4. hard_hard_test_d_zoom_convergence.eps

    https://api.newton.ac.uk/website/v0/events/preprints/NI09023
    To compute the reconstruction polynomial wi(x,t. n)valid for element Ti we require integral conservation for all elements Tj insidethe stencil Ssi , i.e. ... 1. x. Tj. wsi (x,tn)dx =. 1. x. Tj. Ψl(x)dx ŵ(i,s)l (tn) = Qnj , Tj Ssi.

  5. On a nonlinear integrable differenceequation on the square…

    https://api.newton.ac.uk/website/v0/events/preprints/NI09025
    Tj 1)µui,j µ1ui1,j. 1ui,jui1,j= 0, where Tj is the shift operator for the j index.

  6. The Generalized Symmetry Method forDiscrete Equations D.…

    https://api.newton.ac.uk/website/v0/events/preprints/NI09026
    The Generalized Symmetry Method forDiscrete Equations. D. LeviDipartimento di Ingegneria Elettronica,. Università degli Studi Roma Tre and Sezione INFN, Roma Tre,Via della Vasca Navale 84, 00146 Roma, Italy. E-mail: levi@roma3.infn.it. R.I.

  7. P. Grinevich, S.Novikov Singular Finite-Gap Operators and Indefinite…

    https://api.newton.ac.uk/website/v0/events/preprints/NI09030
    tj kj (w). (O. (1. k(w). ))dk(w), w P. (9). Here we assume that only finite number of variables tn are different from 0. ... exp[i. j. tj. zw. j. ](11). Here j are meromorphic differentials with an unique pole at the point P ,. j = d(kj) regular tems.

  8. Lagrangian multiforms and multidimensional consistency Sarah Lobb and …

    https://api.newton.ac.uk/website/v0/events/preprints/NI09032
    Utjtj. (n2j. (ti tj)2U2tiU2tjU2titjU2tj 1tj ti. UtitjUtj. ). n2i2(ti tj)3. UtjUti. ... 2(ti tj)(tj tk)U2tj+. n2k2(tj tk)(tk ti)U2tk. (4.10a). or(ti tj)UtkUtitj (tj tk)UtiUtjtk (tk ti)UtjUtkti = 0.

  9. Darboux-review-v7.dvi

    https://api.newton.ac.uk/website/v0/events/preprints/NI09047
    4.19) jθi Qij(j)θj = θTj(ij)(ψTi(j)Qψj ψ. Tj(i)Qψi. ),. which vanishes due to (4.17).

  10. P.Grinevich 1, S.Novikov2 Singular Finite-Gap Operators and…

    https://api.newton.ac.uk/website/v0/events/preprints/NI09048
    tj kj (w). (O. (1. k(w). ))dk(w), w P. (9). Here we assume that only finite number of variables tn are different from 0. ... exp[i. j. tj. zw. j. ](11). Here j are meromorphic differentials with an unique pole at the point P ,. j = d(kj) regular tems.

  11. A constructive approach to the soliton solutionsof integrable…

    https://api.newton.ac.uk/website/v0/events/preprints/NI09072
    T11 T12 ηj,. η123j =Tj [T13 (T. 11 T. 12 η3)T3][T. ... N}, (4.7). in terms of whichη1.ij =. Tj Ai 1T1j Ai 1.

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