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1 Sep 2011: 0; h! 0;W TO WREMQ KAK DLQ p > 2 kD1hkLp(V ) = Op(1)h12=pj lnhj! ... 13:9)I WYPOLNENY OCENKI kf1kWmp (I4h) = Op(1); p 2 [1; 2);k(f1)kL1(Vh) = OH(j lnhj)!

1 Sep 2011: 0; h! 0;whereas for p > 2, we havekD1hkLp(V ) = Op(1)h12=pj lnhj! ... r2); (13:9)and the estimates kf1kWmp (I4h) = Op(1); p 2 [1;2);k(f1)kL1(Vh) = OH(j lnhj)!

10 Apr 2011: The theory of OP thus suggests a microscopic theoretical explanation for the observed trends in A 1 and Zc rather than just a parametri-zation of the data.

10 Apr 2011: Op. Cell Biol. 7, 673–680. van de Meent, J. W., Tuval, I. & ... Curr. Op. Cell Biol. 16, 68–72. Taiz, L. 1992 The plant vacuole.

10 Apr 2011: "!$#%'&( ) ,--/. 01203547689:8; <>=?=@BA=5CEDFFGH>IKJI5L MN/OPIQRTSU7VXW YZ Y[]. P_$_ a b c'dfehgikjhllmonqpsrtEu'vPwyx{zP|}/s/BEBoBsyk"/ ¡¢£E¤¥Eo«ª"BB µ${P"º»sq¿BÀÀÂÁTÃÄÅÆBÇBÈÉPÊËÍÌPÎ"ÊÏÐsÑÍÒoÓqÔÕkÖ"ÖØhÙ]Ú5Û

10 Apr 2011: Phototactic orientation in natural environments can be op-posed by ambient vorticity (30), which may be created by themotion of other nearby organisms, convection, or wind-drivensurface waves.

10 Apr 2011: r. op-al. e,thechenpa-. erhal-. m,. rspi. POWERS, HUBER, AND GOLDSTEIN PHYSICAL REVIEW E65 041901.

10 Apr 2011: unfavorable to the op&m of th6, tsanmision of the particles of the pollen to the o d m , than to that which considers the direct action d these prn&h

6 Oct 2011: 1). / z. " OP=R P. Fig. 1. w 2. I n t e g r a t i o n s.

1 Sep 2011: 3. Acknowledgements. I am grateful to Prof. W. Dahmen for giving me the op-portunity to work at the RWTH Aachen, and for his constant inspiring encouragementof my studies.