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30 Jul 2019: in the extrapolation of the training data.24,25 This isconceptually similar to the approach taken to uncertaintyestimation in ensemble models, although here the underlyingmodel is a deep neural network and ... 1. Introduction to Methodology and Encoding

30 Jul 2019: Cavendish Laboratory - J.J. Thomson Avenue, Cambridge, CB3 0HE, UK. received 24 October 2018; accepted in final form 18 June 2019published online 22 July 2019. ... and Zwierlein M. W., arXiv:0801.2500. (2008).[23] Chevy F., Phys. Rev. A, 74 (2006) 063628.

7 Jan 2019: 22). For P2 we have. P2x. = α/2 (23). P2y. = 0 (24).

7 Jan 2019: g. aB , ω2B = 12ga. l2(AB). so. ω2B = 12gal2B 24. ... 11. g2. l2ω2B ,. ω4 12gal2ω2 24. 11. g2. l2= 0 ,. and therefore. ω2 = 6ga. l2. 1. 1 2. 33. l2.

7 Jan 2019: z =1 p. 3i. 2+. q. 2. (1 p. 3i)2 4 q = 1 (24).

7 Jan 2019: 0. ux1du. 1 u= 2πi (24). Identifying the sin πx and dividing through, the required result is obtained.

7 Jan 2019: 2γ(tt′) sin (t t′). (24). We use the Green function to solve for the response to source f(t) by calculating.

7 Jan 2019: f̃(ω) =. dt f(t)eiωt ; f(t) =1. 2π. dω f̃(ω)eiωt (24). ... G(x,t) = dωdk. (2π2). ei(kxωt). ρω2 iγω Tk2(29). A. (24 January 2002) (TURN OVER.

7 Jan 2019: " $#&%'() ,--. /10 243 24567 849 : 9/24: ;<9 0 :=84/ >9?@9 9 2A BCD4E 9 7 9 E FG0 9 7 FHD@9 I@J J J KLE 9 /: 90 ... kx m n l. q3 J 91JLz|{124IHP B0 I49 0 9 }u4/17 3 B124: v B10<7 849A BHB10 I43 24/17 9 : m n J 849bH3 249 7

7 Jan 2019: " $#&%'() ,---./10 243 24567 849 : 9/24: ;<9 0 :=84/ >9?@9 9 2A BCD4E 9 7 9 E FG0 9 7 FHD@9 I@J J J KLE 9 /: 90

13 Feb 2019: 16. Introduction. radius [24]. There are two reasons why strong-coupling behaviour can be re-alised using localised excitations for which there is no microscopic mo-mentum conservation, despite the condition ... Bose condensation is the result of the

5 Feb 2019: 22. 3.1.3 Exchange and correlation. 23. 3.1.4 The Kohn-Sham equations. 24. ... g) = E (fr. g) : (2.24). This adiabatic principle is crucial because it allows us to separate the nuclear and.

6 Feb 2019: 23. 3.1.3.1 Tomfohr-Sankey method. 24. 3.2 Nuclear Dynamics. 24. 3.2.1 Forces on the nuclei. ... 24. 3.2.2 Atomic positions and velocities. 25. 3.2.2.1 Velocity Verlet algorithm.

5 Feb 2019: 12. 2.3 Bandstructure from the total energy method. 21. 3 Brillouin Zone integrations 24.

5 Feb 2019: 21. 2.4.1 Trial Wavefunctions. 24. v. vi CONTENTS. 2.4.2 Evaluating the Local Energy. ... the variational principle (see section 2.1),. E[(r)] E. 0. : (1.24).

4 Sep 2019: Part IIC (January 2019 version) Lent term 2019. QUANTUM INFORMATION. AND COMPUTATION. Lecture notesRichard Jozsa, DAMTP Cambridge. rj310@cam.ac.uk. CONTENTS1 Introduction: why quantum computation and information? 32 Principles of quantum mechanics

20 Nov 2019: 2M(d2ψ. dr2+. 2. r. dψ. dr) e. 2. 4π0rψ(r) = Eψ(r) , (7.24). ... polynomials.24. The corresponding wavefunctions are ψ(r) = CL1N1(2br) exp(br), where theconstant C is determined by normalisation.

1 Dec 2019: ψ, ABψ)|2 = 14(|(ψ, {A, B}ψ)|2 |(ψ, [A, B]ψ)|2). (6.26). Combining (6.24) and (6.26), we have that. ( ... Hence. (x̂ x̂ψ)ψ = ia(p̂ p̂ψ)ψ ,. which means we have equality in the Schwarz’s inequality (6.24) used to derive(6.28).

12 Nov 2019: FI =km. (5.24). FR =km. |R|2 = km. (k lk l.

6 Nov 2019: 4.24). 36. Hence. either A = 0 , sin(ka) = 0 ,. ψ(x) = B sin(kx) , k =nπ. 2afor n 2 even.

30 Oct 2019: those satisfying Eqn. (3.11). 24. 3.3 The 1D Schrödinger equation for a particle in a potential.

7 Oct 2019: 1923-24: de Broglie proposes wave-particle duality for matter, as for radiation. •

22 Jul 2019: https://www.ebi.ac.uk/gwas/downloads/summary-statistics. GABRIEL. Asthma. 26475. 10365. 16110. 24. 567589. log(OR). 20860503. 2010. ... Nature 2012;491:119-24. Please cite the paper if results from this study are used.

24 Jul 2019: 0 10 18 21 24 40Reduction of area (%) 63.4 9.0 64 5 61 64 68 74UTS / MPa 903.6 191.0 837 473 790 897 988 1756Loading frequency / Hz ... 200. 300. 400. 500. 600. 0 100 200 300 400. Figure 24: Distribution of Charpy impact toughness in the input data

30 Dec 2019: 0. 0. 0. 0. 0. 0. 0. 0. 800. 24.3. Steel005_6. ... 24.3. Steel031_6. 0.12. 0. 0. 1. 0. 9. 0. 0. 0.

20 Mar 2019: 由于贝氏体片太细小，不能用传统的光学干涉显微镜来观察，而需要用原子力显微镜。.

24 Dec 2019: 19. 20. 21. Terashima & Bhadeshia, 2006. 22. 23. 24. 25.

24 Dec 2019: 24. Daido Steel. TiAl . 25.

24 Dec 2019: Yates, Jerath. 22. Yates, Jerath. 23. 24. UPPER BAINITE. (High Temperature).

24 Dec 2019: 17. Diffusion Coefficient. 18. 19. 20. Mechanism. 21. 22. 23. 24.

20 Jul 2019: 80C 73C, 240 h [24]ε Fe-0.81C 125C, 1 h [25]θ Fe-0.02C 250C, 15–250 min [26]θ Fe-0.014C 150C, 170 h; 260C, ... ProcASTM. 1952;52:592–596. [24] Okamoto H, Oka M. Isothermal martensite transfor-mation in a 1.80 wt% C steel.

30 Jun 2019: accidentally placed with the emulsion side down, during exposure? 24. Is the camera constant for a TEM unique? ... accidentally placed with t;he emulsion side down, during exposure? 24. Is the camera constant for a TEM unique?

12 Jun 2019: Full Terms & Conditions of access and use can be found athttps://www.tandfonline.com/action/journalInformation?journalCode=ymst20. Materials Science and Technology. ISSN: 0267-0836 (Print) 1743-2847 (Online) Journal homepage:

23 Nov 2019: The change in volume required toinduce the magnetic transition is about 5% [24,25]. ... 24 h with thecomposite periodically rotated in the field to magneti-cally align the particles as the resin solidifies.

23 Jun 2019: J Mater Sci. 1997;32(20):5439–5444. [24] Honeycombe RWK. Structure and strength of alloysteels. ... Metall Trans A.1993;24:1251–1256. [28] Cui H, Sun F, Chen K, et al.

4 Jan 2019: be found in [15,24]. Defining the thermal model. Each weld bead (pass) is considered to be deposited as a block (sometimes called. ... 491.294. [24] A.F. Mark, R. Moat, A. Forsey, H. Abdolvand, P.J.

29 May 2019: phase ( 2(1) 8.24, p 0.008), but not at test (. 2(1) 0.12,. p 1), and a linear trend was observed during both study ( 2(1) 12.58, ... StudyR Precuneus 6, 68, 46 1242 6.19R Angular gyrus 44, 54, 54 515 5.01R Middle temporal gyrus 66, 24, 8 80 5.02R Middle

20 Mar 2019: 53]FEP-HARMS-LT-NH. 1613. 25.1 (4.6)24.6 (2.2). 12/48/5. BRPS (variable) Auditory. Neves et al., 2016 [63] BD-HBD-NH. ... the bilateral STG, bilateralHG, and bilateral insula [23,24,26] (Supplementary S3–4) and quali-tative reviews on structural

19 Feb 2019: The other participants made up the consolidation group, and only learned this inconsistent information on day 2, after 24 hours time for consolidation.

19 Jun 2019: of other people.24 While descriptions of hallucinatory. ... 1991;26:287–292. 24. Johns LC, Cannon M, Singleton N, et  al. Prevalence and correlates of self-reported psychotic symptoms in the British population.

20 Mar 2019: THEORETICAL REVIEW. Exploring the neurocognitive basis of episodic recollection in autism. Rose A. Cooper1 & Jon S. Simons2. Published online: 9 July 2018# The Author(s) 2018. AbstractIncreasing evidence indicates that the subjective experience of

17 Jan 2019: With these scalings, equations(22) and (24) can be written in dimensionless form as. ... 24] A.W. Rempel, M.G. Worster, The interaction between a particle and anadvancing solidification front, J.

28 Aug 2019: with it. In fact there are two dierent 1’s lurking in the expression (2.24). ... 25 –. We can deal with the infinity in (2.24) in a more practical way.

28 Aug 2019: 3.24). since t, being the upper limit of the integral, is the latest time so HI(t) can be pulled. ... For n = 4,. the equation reads. T(1234) = : 1234 : z}|{12 : 34 :. z}|{13 : 24 : four similar terms. z}|{12. z}|{34. z}|{13. z}|{24.

28 Aug 2019: where µsatisfies. µ. = µ (1.24). For example, a rotation by about the x3-axis, and a boost by v < 1 along the x1-axis. ... transformations. µ= µ! µ. (1.49). where! µis infinitesimal. The condition (1.24) for to be a Lorentz transformation.

28 Aug 2019: 4.23). S[] = exp12 S. (4.24). Although the basis of generators M and S are dierent, we use the same sixnumbers in both and S[]: this ensures that we’re

28 Aug 2019: in spacetime such that they satisfy the operator equation. @. @t= i[H, ] (5.24). ... Figure 23: An incoming anti-fermion Figure 24: An outgoing anti-fermion. • Each vertex gets a factor of i. •

19 Jul 2019: ai bj = 2 ij (2.24)? is sometimes referred to as the dual lattice. ... 53 –. The condition (2.24) can also be stated as the requirement that.

19 Jul 2019: magnetic field,. An =2eB. (n ) (3.24). This quantisation of area is actually a variant of the Landau level quantisation that we. ... N = 0. which should clearly be an integer. The quantisation (3.24) due to a background magnetic field.

19 Jul 2019: r(10.24). The 1/r fall-o follows from solving the free Schrödinger equation; we’ll see this ex-.