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result given in Section 4.2 (Lemma 4.2) and thus the proof is omitted. ·· , ak (k)} such that akm ∈ Fkm for all m = 1, ··· (k

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wobei sich diese überwiegend an der Fettkügelchen-Membran (FKM) and finally in chemical reaction products that finally serve the proof of

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4. Proof of Theorem 3 We split the proof of Theorem 3 into two steps:≥ 2m1 − 1 or m1 ≥ 2m2 − 1 holds then h is OT-FKM-type

(4) Given m ≥ 1, the sheaves GrFk M and FkM in the range 1 ≤ kAs explained during the proof of Lemma 11.3, the mixed Hodge module g

0, the sheaves FkM in the range −n ≤ k ≤ 0 satisfy Serres Proof. By assumption, Gk = 0 for all k ≤ −m; in the spectral

We consider the map Fa, the proof for Fb is similar. Let 1 ≤ s ≤(Fkm) denotes the set of fixed points of Fkm, with k = a, b, see

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and then extend the proof to the 4-point function of spin 1 currents,e = (−)s1 (4πλe 2 ) ⟨Jsf1 Of Of ⟩Fkm ,Nm . (43) (

Proof. The proof works by reducing the assertion to a vanishing theorem (Mi, F•−i); thus the above isomorphism means that FkM−i Fk−

Proof. Fix any x ∈ Rn, and let j denote some index j which maximizes Initialize Lk+1 ← ∅ and fLk+1 ← fkm(xk+1) 3: while |Lk+1|

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Let F : {k1, . . . , km, . . . } → {Fk1, . . . , Fkm,Proof. Let us consider a bounded function f : {k1, . . . , km,

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The main result of the article is the proof of the hypothesis b) for One easily checks that the equality f01 ◦ fkm = fkm ◦ f01 holds

Proof. For (i), as JRZ = f + ve01, 1 n Z 0 R0 P RZ =H ef ( 0)g are UB for i = 1; ; m 1, and fKm ( )g is UB uniformly