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83 sonuçtan 1-3 arası sonuçlar
Sayfa 105
M-^M-H^KU- Combining these two expressions inside the trace trQl,.,.,Qfc, we
obtain (4.17) for j = 2 and fc < — 3. The calculation of the residues at the rest of
the poles can be done by using symmetries. We set (4.18) ta(X2) = ra5(X23 - 1) ...
M-^M-H^KU- Combining these two expressions inside the trace trQl,.,.,Qfc, we
obtain (4.17) for j = 2 and fc < — 3. The calculation of the residues at the rest of
the poles can be done by using symmetries. We set (4.18) ta(X2) = ra5(X23 - 1) ...
Sayfa 108
After that, the argument is similar, and we obtain an expression similar to (4.43).
Adding these two expressions, we obtain the left-hand side of (4.37). □ Using (
4.19), we obtain *-*^&(-*-5) {□SU)(*w,(*.-4i)) <4-44> *r„2(-fc) • □ □ ra>!(-3)r„5(-i
+ ...
After that, the argument is similar, and we obtain an expression similar to (4.43).
Adding these two expressions, we obtain the left-hand side of (4.37). □ Using (
4.19), we obtain *-*^&(-*-5) {□SU)(*w,(*.-4i)) <4-44> *r„2(-fc) • □ □ ra>!(-3)r„5(-i
+ ...
Sayfa 508
Thus if we assume that the subspaces 6^^(C) span i2 for almost all ( s T, we
obtain <I> — F = and so the zero function is the only superoptimal approximant of
§7. Badly approximable operator functions In [PT3] we obtained a description of
the ...
Thus if we assume that the subspaces 6^^(C) span i2 for almost all ( s T, we
obtain <I> — F = and so the zero function is the only superoptimal approximant of
§7. Badly approximable operator functions In [PT3] we obtained a description of
the ...
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İçindekiler
A FeHepanoe A M KorieHHan nopoacfleHHOCTb aire6p | 1 |
BblUKO A r O Uqsl2 HHBapHaHTHbIX lMaTpHljaX flJIfl CTapilJMX | 24 |
Mamuioe JI M 06 OTcyrcTBHH coScTBeHHbix 3HaMeHHH b cneKTpe | 47 |
Telif Hakkı | |
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absolutely continuous algebraic solutions amoebas analytic arbitrary assume asymptotic badly approximable Belyi function Bose gas bounded coefficients coincides compact condition conjugacy classes consider constant convergence convex Corollary correlation functions corresponding curves defined definition deformation denote dessins diagram differential dimension Dirac operator discrete edges eigenvalues element English transl equivalent estimate exists finite matrix functions formula G-cycle geodesic given Goursat problem graph hyperbolic identity implies inequality integral intersection invariant lattice Lemma linear Lipschitz Lipschitz map locally Math Mathematics Subject Classification metric space Newton polygon notation obtain Painleve parameter Phys polygon polynomial problem proof of Theorem Proposition prove quantum R-matrix rational functions relation respectively result right-hand side satisfies selfadjoint sequence sixth Painleve equation spectrum strongly regular graph Subsection subspace Suppose symmetric Theorem 2.1 theory transformation unique variables vector vertex vertices YB equation zero