Search

5 Oct 2013: Our approach is modeled on the abstractStetter-Lindberg-Skeel error analysis [15, 12, 14], which treats the initial value problem (IVP) as an op-erator equation approximated by a discrete operator

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

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

26 Jun 2024: Preprint typeset in JHEP style - HYPER VERSION 2018. Gauge Theory. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge, CB3 OBA, UK.

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

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.

17 Jun 2019: Are there Higher-Accuracy Analogues of. Semigeostrophic Theory? Michael E. McIntyre. Centre for Atmospheric Science. y. at the. Department of Applied Mathematics and Theoretical Physics,. Silver St, Cambridge CB3 9EW,. UK,.

19 Dec 2017: We seek the distribution function/(r,p,t) describing the time-dependent phase-space probability den-sity for electrons at position r with momentum p, and devel-op / perturbatively,.

26 Mar 2014: Given a sensing op-erator A Cmn or A B(L2(Rd),Cm) and noisy measurements y = Ax e with‖e‖2 η , the usual approach is to solve the

19 Oct 2013: 23 Nov 2004 1:27 AR AR235-FL37-11.tex AR235-FL37-11.sgm LaTeX2e(2002/01/18) P1: IBD10.1146/annurev.fluid.37.061903.175710. Annu. Rev. Fluid Mech. 2005. 37:263–93doi: 10.1146/annurev.fluid.37.061903.175710. Copyright c 2005 by Annual Reviews. All

19 Oct 2013: For the definition of PVwe may use for instance the shallow-water PV discovered by Rossby (1936), whoshowed it to be an exact material invariant for frictionless flow (op.

2 Sep 2012: 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.

21 Feb 2022: Day et al. eLife 2022;11:e72707. DOI: https:// doi. org/ 10. 7554/ eLife. 72707 1 of 28. Cellular organization in lab- evolved and extant multicellular species obeys a maximum entropy lawThomas C Day1, Stephanie S Höhn2, Seyed A Zamani- Dahaj1,3,4

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.

24 Aug 2023: Legendrean and G2 Contact Structures. Timothy Moy. April 1, 2021. Thesis submitted for the degree ofMaster of Philosophy. inPure Mathematics. at The University of AdelaideFaculty of Engineering, Computer and Mathematical Sciences. School of

13 Jan 2015: a) Infinite straight wire carrying current I. Take the z-axis along the wire, take O in the xy-plane throught the point P, and calculateB at P, r = OP using

26 Mar 2014: Given a sensing op-erator A Cmn or A B(L2(Rd),Cm) and noisy measurements y = Ax e with‖e‖2 η , the usual approach is to solve the

19 Oct 2013: It is numerically small, the more so the higherthe accuracy. However, for the plain PV inversion op-erators and PBMs under consideration, qAI 0 generi-cally if we exclude unphysical model

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

10 Apr 2019: On reconstructions from measurements. with binary functions. Robert Calderbank Anders Hansen Bogdan Roman. Laura Thesing. Abstract. We consider the problem of reconstructions from linear measurementswith binary functions. That is, the samples of the

27 Dec 2023: Supersymmetric Field Theory. University of Cambridge Part III Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge, CB3 OBA, UK.

4 Oct 2010: This was verifiedby finite-element calculations and experiments using the op-tical trap not shown.

28 Nov 2014: Part II Principles of Quantum MechanicsMichaelmas 2014. Prof. R.R. Horgan. November 28, 2014. Contents. 1 Introduction 1. 2 Dirac Formalism 2. 2.1 States and Operators. 2. 2.2 Observables and measurements. 4. 2.3 Time evolution and the Schrödinger

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.

17 Sep 2022: Matthew J. Colbrook†. Abstract. Sharpness conditions directly control the recovery performance of restart schemes for first-order op-timization methods without the need for restrictive assumptions such as strong convexity.

5 May 2015: 3/5)/2,k = 1, 0, 1.Since we deliberately postpone spatial discretisation, the splittings are in an op-.

3 Oct 2012: 3.2. Comparison CCD, CMOS, and QPD. After determining the optimal illumination level, we monitor the Brownian motion of op-tically trapped polystyrene colloids at a laser power adjusted to a

21 Mar 2013: On the Structure of Path Geometries and Null. Geodesics in General Relativity. Stephen Casey1. Department of Applied Mathematics and Theoretical Physics,. University of Cambridge,. Wilberforce Road, Cambridge CB3 0WA, UK. March 21, 2013. 1Email:

13 Nov 2010: e. j. -. 9.t,rA. liti- s s;-)r. b-;-:'-. nPH.: -. -. B. DNAL 0. bead. ::. FIGURE 1 (A) Simplified optical layout for the feedback-enhanced op-tical trapping interferometer (not to

10 Nov 2010: In the op-tical tweezers experiment, a particle having a larger refractiveindex than its surrounding medium is trapped by the radiationpressure of a focused laser beam. ... Note that the linear behavior is even found for large modulation.Small driving

30 Nov 2019: Numericalevidence concerning the conjecture will be discussed in Section 2.4.2. It will be helpful to introduce the notation Op(A,η) to mean terms of at least orderp in

10 Apr 2019: On reconstructions from measurements. with binary functions. Robert Calderbank Anders Hansen Bogdan Roman. Laura Thesing. Abstract. We consider the problem of reconstructions from linear measurementswith binary functions. That is, the samples of the

19 Oct 2013: The point,which now seems to be widely appreciated | and. indeed is coming close now to new forms of op-erational exploitation (A.

3 Oct 2008: ẑ). The position vector of a point P is. OP = r = exx eyy ezz =. 3. i=1. eixi. 1.2.2 Properties of the Cartesian unit vectors. The unit vectors form

8 Jul 2021: RESEARCH ARTICLE. The bank of swimming organisms at the. micron scale (BOSO-Micro). Marcos F. Velho Rodrigues1, Maciej LisickiID2, Eric Lauga1. 1 Department of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge, United.

6 Dec 2020: On the infinite-dimensional QR algorithm. Matthew J. Colbrook† and Anders C. Hansen†. †DAMTP, Centre for Mathematical Sciences, University of Cambridge, Wilberforce Rd,Cambridge CB3 0WA, United Kingdom. Abstract. Spectral computations of