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16 Dec 2013: Bayesian Approaches to Multi-Sensor Data Fusion. A dissertation submitted to the University of Cambridge. for the degree of Master of Philosophy. Olena Punska, St. John’s College August 31, 1999. Signal Processing and Communications Laboratory.

5 Aug 2013: 700. 600. 500. 400. 300. 200. 100. 200 400 600 800 1000 1200. ... 400. 300. 200. 100. 200 400 600 800 1000 1200. (a) Video Frame 235.

17 Dec 2013: 0 200 400 600 800 1000 1200 1400 1600 1800 20000. ... p = 1/2ε = 0.1. 100 200 300 400 500 600 700 800 900 1000 11001016.

26 Jul 2013: Both the Ni and Au. segments have a diameter of 200 nm.

28 Nov 2013: 200–. 400. 400–. 600. 60. 0. Test. num. ber. Confinement pressure: kPa(a). ... 200. Fig. 9. Normalised shear modulus degradation curves of Toyourasand shifting with mean effective stress.

3 Oct 2013: c h r i s t ’s c o l l e g e. christ’ s co. llege m. aga. zin. e2. 013. m a g a z i n eno.238. no. 238. 2 0 1 3. Blo. ssom. in T. hird. Cou. rt. Phot. ogra. ph b. y C. hlöe. App. lin 2. 013. C o n t e n t s. C o l l e g e n e w s 3. S p e c i a

5 Aug 2013: Maximum correlation score at λ -0.8 and ω 200. Cor. rela. ... We observe that there is a corresponding peak at approximatelyR = 200 and s = 0.8.

26 Jul 2013: J. Fluid Mech. (2013), vol. 715, pp. 1–31. c Cambridge University Press 2013 1doi:10.1017/jfm.2012.484. Unsteady feeding and optimal strokes ofmodel ciliates. Sébastien Michelin1,† and Eric Lauga2. 1LadHyX – Département de Mécanique,

30 Jul 2013: Nicotinic acetylcholinereceptorandthestructuralbasisofneuromuscular transmission:insightsfromTorpedopostsynapticmembranes. Nigel UnwinMRC Laboratory of Molecular Biology, Francis Crick Avenue, Cambridge CB2 0QH, UK. Abstract. The nicotinic

27 Oct 2013: Computational Design of Advanced Steels. H. K. D. H. Bhadeshia a,b. aGraduate Institute of Ferrous Technology, Pohang University of Science andTechnology, Pohang 790-784, Republic of Korea. bMaterials Science and Metallurgy, University of Cambridge,

19 Aug 2013: sample number. ampl. itude. 0 100 200 300 400 500 600 700 800 900 1000800. ... 0 100 200 300 400 500 6001. 0. 1. 0 100 200 300 400 500 6001.

5 Aug 2013: kth finest scale levelE. k. subband 123456. (b) Wavelet energy. 50 100 150 200 250. ... Rippled data. 100. 101. 102. 103. 0. 100. 200. 300. False positives.

18 Jul 2013: 100,000. 200,000. 300,000. 400,000. 500,000. 600,000. 700,000. 800,00019. 71. 1974. 1977.

19 Oct 2013: Geophys. Astrophys.Fluid Dyn., 9, 185–200. Taylor, G. I. 1915 Eddy motion in the atmosphere.

28 Nov 2013: pressure of 200 kPa, directly to the centrifuge slip rings. Maximum pressures of 1?3 MPa were experienced at the package,. ... 00–600 –400 –200. Calculated pressure at slip rings, Ps: kPa400200 600.

5 Aug 2013: Fig. 1.1: Four utterances of the vowel sound ‘Aah’. 0 50 100 150 200 250 300 350 4006. ... valu. e of. thro. w. 100 200 300 400 500 600 700.

21 Apr 2013: 283. =. c2(n)qn2 = q. 12 20. 3q. 22. 200. 9q.

14 Mar 2013: We used 200 repli-cates. We again see that the risk curve is sharpest near criticality when the size of the anomalouscluster is sufficiently large, here for 50.

5 Aug 2013: 100. 200. 300. 400. 500. 600. Time Sample 235. 450 500 550 600. ... 0 100 200 300 4000. 10. 20. 30. Erro. r. Maximum LikelihoodParticle Filter.

4 Nov 2013: as a buoyant plume through the approximately 200 metre thick formation beforeit is ultimately stopped by the Nordland shale, a relatively impermeable cap rock atthe top of the formation. ... 2007)clearly show that the dynamics of the plume propagation

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:

31 Oct 2013: HOW ARE WE DOING?As a department, we do pretty well atpostgraduate and postdoc level, with agood number of women – for example,around a third of our 200-odd postdocsare female.

17 Jul 2013: with shearrate _. The chamber, typically 2 mm wide and 200 m deep,is made from polydimethylsiloxane by soft lithography andsealed with a glasscoverslipthat had been treated to promotevesicle adhesion.

7 Jan 2013: Recognition is needed that not all universities are able to. i Brown and Hesketh (200). ... Where possible, data have been included up to the end of June 200.

16 Jul 2013: 88692 HD 165439 1.2 200 A2 11 Myr? Age uncertain? (22)89046 HD 166191 45.9? ... Inany case, removal of the coolest few sources (those below 200 Ksay) would make little difference to our analysis.

12 May 2013: The integrated intensities. 2. of (200)α, (211)α, and (220)γ, (311)γ reflections were used to quantitativelydetermine the austenite content.

15 Aug 2013: One of the. 50. 100. 150. 200. 250. 300. 350. 400. ... 60. 50. 40. 30. 20. 10. 0. 400. 200. 0. 200.

31 Oct 2013: More than 200 people came to his. funeral: members of his family, ex-members of his group, friends, col-leagues and neighbours, all enriched forhaving known him.The flood of messages

4 Oct 2013: The device was mountedonto the single-molecule confocal setup, and sample waswithdrawn from the device at a rate of 200 μL/h.

14 Mar 2013: In the high-frequency region above 200 cm1, theE12g (384 cm1), A1g (409 cm1), 2LA(M) (453 cm1),. ... Although the in-plane modes in 5 and 6L-MoS2above 200 cm1 are almost identical, the C and LB modepositions below 100 cm1 are different.

10 Jan 2013: nanotube mode-locked 2 lm solid-state lasers (e.g., 200 fs(Refs. 8, 9, and 52)), but shorter than previous graphene.

18 Jul 2013: 0 200 400 600 800 1000 1200. Buckinghamshire Solent. Enterprise M3 Oxfordshire.

3 Feb 2013: We determined the temperature-dependent distributions of θfrom more than 200 scattering events by tracking the position of thecell body up to a distance of 70 μm from the corner (Fig.

17 Apr 2013: At this radius, the time-scale for planet stir-ring is only 0.65 Myr, orders of magnitude less than the star’s age(200 Myr; Barrado y Navascues et al.

16 Mar 2013: 15] L̄ = 200–400 nm 2L̄ 1 = 0.005–0.01 <960 MPaNanoparticle strengthened [16] NV = 1.1 1024 m3, r = 1.25 nm 4πr 2 NV = 0.011 800Accumulative roll ... bonding [17] L̄ = 420 nm 2L̄ 1 = 0.005 870Severe plastic deformation [18] L̄ = 100 nm 2L̄ 1 =

3 Feb 2013: 5R18: Environmental Fluid Mechanics Pollution dispersion in the environment. 1. 5R18:. ENVIRONMENTAL FLUID MECHANICS AND AIR POLLUTION. Dispersion of Pollution in the Atmospheric Environment. “Air and water, the two essential fluids on which all.

4 Nov 2013: At the working distances typically used this resolution implies a spatialresolution of 5-7 pixels per millimetre (150 200 µm per pixel).

5 Jun 2013: or 200 knot. The cores of these thin jets may meander, river-like, with.

4 Nov 2013: σi. (a). 5 10 15 20 25 30–400. –300. –200. –100. ... 5. 10. 15. 20. 25. Rmc. –200. –150. –100. –50. 0.

16 Dec 2013: 300 200 100 0 100 200 300. 0.8. 0.6. 0.4. 0.2.

5 Oct 2013: 18. 50 100 150 200 250 3000. 500. 1000. 1500. 50 100 150 200 250 3000. ... 19. 50 100 150 200 250 300 350. 0.9. 1.0. 1.1.

15 Aug 2013: 7. It is required to design an FIR bandpass filter of order 200. ... to design a causal FIR bandpass filter which approximates the idealbandpass filter, having an impulse response hn for 0 n 200.

19 Nov 2013: Continuing undergraduates 120 99 78 65 Continuing full-time postgraduates 141 145 138 135 sub-total (continuing full-time students) 261 244 216 200.

29 Nov 2013: 10. 15. 20. 25. 30. 35. 40. 0 100 200 300 400 500. ... 1. 5. 20. 40. 70. 85. 94. 96. 98. 99. 150 200 250 300 350 400 450 500.

3 Jan 2013: Sens. Actuators A133, 200–209. (doi:10.1016/j.sna.2006.03.010). 20. Jung K, Nam J, Choi H.

16 Jul 2013: 298.15. 350. 475. 0 25 50 125 150 200 3000. 500.

24 Jan 2013: 80. 100. 120. 140. 160. 180. 200. 220. 240. 1 5 15 30. ... 60. 80. 100. 120. 140. 160. 180. 200. 220. 10 30 50 70 90.

28 Nov 2013: 300. 200. 100. 00. (a). (b). (c). 10 000 20 000 30 000 40 000. ... props. The maximum bending moment induced by the. undrained excavation amounted to about 200 kNm/m.

5 Feb 2013: Indeed, recently,we demonstrated behaviorally that individuals with poor atten-tional control showed impaired target processing in an RSVP taskfollowing presentation of an irrelevant emotional distractor, ifthe target appeared within 200

11 Sep 2013: As a numerical example, let us consider a multiple accesschannel that consists of a single receiver, placed at the origin,and 200 transmitters, placed uniformly along thex-axis witha separation of25 ... 3, forthe caseρ = 1, and if all the nodes outside