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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

12 Jul 2016: V. CONCLUSIONS. We demonstrate the density dependence of the spinstate of a polariton condensate under non-resonant op-tical excitation. ... The latter weattribute to the inherent spin imbalance induced by op-tical excitation in combination with the

26 Feb 2008: Let θ be theangle between OQ and OP. Show that the equilibrium positions are at θ = π.

11 Nov 2006: IfOP represents z, then. OP ′. represents z, where P ′ is the point (x,y); i.e.P ′ is P reflected in the x-axis. ... vector, r, from some chosen origin O, with r =OP. and r = OP = |r|.Remarks. •

26 Feb 2008: If P is projected with speed V from thepoint r = r0, θ = 0 in the direction perpendicular to OP , find the equation of the orbitunder the assumptions.

20 Nov 2023: The ΣA1 result may be a surprise:One can algorithmically obtain just as much spectral information of such Schrödinger op-erators (by point sampling the potential) as that of diagonal ... As done in the case of bounded Hilbert space op-erators

26 Jun 2024: for example,. p̂x (x) = i@. @x. • Other operators now follow from our specification of position and momentum.The angular momentum operator is shorthand for a collection of three such op-.

25 Jan 2007: q2 is positive (same sign charges) then F12 is an repulsive force; if negative (op-posite sign charges), then it is attractive.The factor 140 is a dimensional quantity due to ... Take the z-axis along the wire, take O in the xy-plane throught the point P,

26 Jul 2023: Error control 2 limits 3 limits1 limit 3 limits. Approx. sparse normal op.

26 Jul 2013: The optimal elastic flagellumSaverio E. Spagnoliea and Eric Laugab. Department of Mechanical and Aerospace Engineering, University of California, San Diego,9500 Gilman Drive, La Jolla, California 92093-0411, USA. Received 25 September 2009; accepted

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.

2 Sep 2012: 118101-2. OP 3G G Q Q G; (3). where G F=Q 1=3l Tr F=Q is the nematicmolecular field. ... total deviatoricstress in the active case can be written as a v OP, plus a noise source unconstrained by a fluc-tuation-dissipation theorem since this is a

19 Oct 2013: already alluded to. In any case, the work of Lindzen and Tsay (op.

13 Dec 2018: op- erator A - l.

22 Nov 2010: Solar Flare Parcle Acceleraon ‐ a spectroscopic viewpoint. Lyndsay Fletcher. University of Glasgow. Helen‐Fest, Sept 14th, Cambridge. A broad view of flare spectroscopy. microwave loops EUV/SXR loops. Gamma-ray footpoints. X-ray, UV, optical

3 Oct 2017: 20 A. Iserles, K. Kropielnicka & P. Singh. Height reduction. A very interesting feature of the symmetrised differential op-erators (2.4) is the property of height reduction.

5 Oct 2013: exponential convergence whenevern = O (. m). We note that the use of polynomial least squares for overcoming the Gibbs phenomenon, as op-posed to the Runge phenomenon, is far less well known.

13 Dec 2018: but (10) will be more convenient for us because explicitly it involves only second as op-posed to fourth order derivatives inx.) The above will be applied below to the recovery

25 Jun 2024: These topics in turn can be di-vided into concrete applications, such as op-tion pricing or chemical kinetics, advancednumerical methods (higher order methods,multilevel Monte Carlo), and generaliza-tions, such

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.