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

20 Apr 2023: Forsdyke; Email: jf580@cam.ac.uk. Received: 15 August 2022; Revised: 01 March 2023; Accepted: 24 March 2023. ... with a trowel to achieve a flat exposed face. The concrete cubes were removed from the molds followingan initial setting period of 24 hr,

8 Oct 2009: 3.2. SYMMETRY IN QUANTUM MECHANICS 24. 3.2 Symmetry in quantum mechanics.

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.

6 Feb 2006: We can summarize this procedure as:. |Φ+〉12|Φ+〉34 =1. 2(|Ψ+〉13|Ψ+〉24+|Ψ〉13|Ψ〉24+|Φ+〉13|Φ+〉24+|Φ〉13|Φ〉24). and the Bell

24 Aug 2020: Received 5 June 2014; published 24 September 2014). The contact interaction is often used in modeling ultracold atomic gases, although it leads to pathologicalbehavior arising from the divergence of the ... 2005).[24] D. L. Maslov and A. V. Chubukov, Phys

15 May 2018: 1976) proposed parameterizations of wind variability. over a range of time periods up to 24 h,.

24 Aug 2020: R3Deff < 0 for narrow Feshbachresonances and R3Deff 0 for broad Feshbach resonances so thatin typical experiments exploiting the full gamut of availableresonances, 100 k2FR2eff 0 [6,12,24]. ... 24). where the ui are the Nu = 3 optimizable coefficients.

22 Aug 2021: random forests (RFs),2123 radial basis functions (RBFs),24. support vector machines,25,26 and Gaussian processes(GPs).2729 Intermediate neural network methods have along history, including artificial neural networks11,30 ... CYP2D6 % inhibition 0.26 0.37

8 Jan 2016: Appendix A: The Survey. 24. Appendix B: Summary of survey responses.

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).

24 Aug 2020: of systems consisting of many thousands of atoms [24,25],giving rise to new opportunities for applications in differentfields, as discussed, for example, in recent reviews on thesubject [26,27].

24 Sep 2017: More saliently, genons at ν 1 in our modelhave d 2 thus allowing for universal quantum compu-tation, while the quasiparticles of the MR state itself cannot[12,24]. ... E. Tai, M.Rispoli, R. Islam, and M. Greiner, Ultra-precise holographicbeam shaping

10 Nov 2013: Lecture Notes October 2006. Lecture VI 24. Lecture Notes October 2006.

4 Apr 2010: 24. (a) Applying the Hubbard-Stratonovich transformation, the classical partition func-tion is given by.

2 Nov 2009: Z Element Configuration 2S1LJ Ioniz. Pot. (eV). 1 H (1s) 2S1/2 13.62 He (1s)2 1S0 24.63 Li He (2s) 2S1/2 5.44 Be He (2s)2

8 Jan 2016: eg. t2g. t2g. eg. U3J+ CF. 2J. 2J. – Typeset by FoilTEX – 24.

12 Aug 2010: n 0 1 2 3 4 12cjg<0 0.726(4) 0.86(1) 0.91(1) 0.93(1) 0.95(1) 12cjg>0 1.556(4) 1.24(1) ... This (incompressible) filled LL will appear as astep in the transverse density profile, as measured in situ orin an expansion measurement [24].

9 Nov 2009: 1 H (1s) 13.62 He (1s)2 24.63 Li He (2s) 5.44 Be He (2s)2 9.35 B He (2s)2(2p) 8.36 C He

28 Nov 2023: ever-increasing complexity of toxicological testing. 23. 24. AUTHOR INFORMATION. Corresponding Author. ... https://doi.org/10.1016/j.yrtph.2018.10.013. 27. QSAR Toolbox. (n.d.). Retrieved March 24, 2022, from https://qsartoolbox.org/.

12 Aug 2010: 24 OCTOBER 2008. 0031-9007=08=101(17)=176803(4) 176803-1 2008 The American Physical Society. ... 24 OCTOBER 2008. 176803-2. CF-Fermi sea state is uniquely defined as filling two CFshells in each layer (at this flux, the pth CF shell has 2porbitals) [3,12]

24 Sep 2017: 0 3 6 9 12 15 18 21 24 27 30 33 36 39 42n. ... 0 2 4 6 8 10 12 14 16 18 20 22 24 26n.

30 Aug 2021: 30) Priority: 24.05.2013 GB 20130940422.10.2013 GB 201318622. (43) Date of publication of application: 26.11.2014 Bulletin 2014/48. ... 0.24. 50. 135. 0.03. 55. wt. %N. iC. rC. oF. eM.

9 Nov 2009: eV)1 H (1s) 2S1/2 13.62 He (1s)2 1S0 24.63 Li He (2s) 2S1/2 5.44 Be He (2s)2 1S0 9.35 B He

12 Aug 2010: function of a polarized filled LL times an additionalfactor describing the spin texture [24]. ... Finite Skyrmions of size K N=2 on thesphere have L S N=2 K [24].

8 Jan 2016: Since then, HPC has enabled automakers around the world to reduce the time for developing new vehicle platforms from an average 60 months to 24 months. ... Professional bodies such as the Institute of Physics [24] and the Royal Society of Chemistry [7]

24 Oct 2022: 23. 6.5 Second integral of the equation of motion. 24. 6.5.1 Second integral for the simple pendulum (non-examinable).

23 Sep 2021: L E T T E R. Deep imputation on large-scale drug discovery data. Benedict W. J. Irwin1,2 | Thomas M. Whitehead3 | Scott Rowland4 |. Samar Y. Mahmoud1 | Gareth J. Conduit2,3 | Matthew D. Segall1. 1Optibrium Limited, CambridgeInnovation Park, Cambridge

20 Jul 2022: Rep., vol. 8, no. 1, pp. 1–12, 2018. 24. A. Dave et al., “Autonomous discovery of battery electrolytes with robotic experimentation and machine learning,” Cell Reports Phys.

8 Aug 2011: Often for fractional quan-tum Hall systems, this is an ‘‘excitonic’’ state in which thehole binds a charge e to form a neutral exciton moving inthe background incompressible liquid [24]. ... 24] N. R. Cooper and D. B. Chklovskii, Phys. Rev. B 55,

12 Aug 2010: the relation between n andn remains linear [24,25], n n þ , with an offset. ... B. Laughlin, Phys. Rev. Lett. 59, 2095. (1987).[23] Time-reversal symm. is broken explicitly in the model.[24] F.

23 Aug 2021: 2School of Life Sciences, Heriot-Watt University, Scotland, U.K. 3:00 – 3:30 The Rasch model as a measurement model in affective 24. ... Journal of Experimental Psychology: Human Perception & Performance, 24, 830-846. 4.

12 Aug 2010: The data shown here arefor = 0.05 from Monte Carlo simulations on a lattice oflinear size L = 24, with the interaction summed over periodiccopies up to distance = 500 L.

15 Jun 2016: The nanomagnets have an elongated shape. with a length of 62 nm and a width of 24 nm, and are placedon the nodes of a two-dimensional kagome lattice with latticevectors ... 24] G. Möller and R. Moessner, Phys. Rev. Lett. 96, 237202 (2006).[25] U.

26 Jan 2012: A similar scan forNe 10 and 12, which was also performed in [24], reveals acharge gap for a 12=5 state with S 2. ... 24] A. Wójs, Phys. Rev. B 80, 041104(R) (2009).[25] Systems on the sphere can exhibit aliasing competition.

12 Aug 2010: 2Laboratoire de Physique Théorique et Mécanique Statistique, 91406 Orsay, FranceReceived 24 February 2005; published 19 July 2005. ... 498045 0.0531 0.065141 5 24 0.49761 0.0484 0.0584 7 18 0.497976 0.0502 0.0642 0.49682 0.0428 0.0608 0.49722 0.0413

24 Jun 2012: Cirac, C. W. Gardiner, and P. Zoller, Phys. Rev. Lett. 81, 3108 (1998).[24] G. ... I. Watson, J. Phys. A 24, 4999 (1991).[25] E. Tang, J.-W.

14 Jan 2013: Thomas Scaffidi. Ecole Normale Supérieure, 24 rue Lhomond, 75005 Paris, France and Rudolf Peierls Centre for Theoretical Physics,Oxford University, Oxford OX1 3NP, United Kingdom. ... 14 DECEMBER 2012. 0031-9007=12=109(24)=246805(5) 246805-1 2012

26 Jan 2012: peripheral sites [24]. In our real gauge, j are. identical up to translation in all unit cells. ... Chern number, in which states cannot be fully localized.[24] The projection to the upper band is similar, as single-.

27 Sep 2015: fermion theory (10) includes the Abelian states at fillingfactors ν 1=ðjkCj þ 1Þ that have recently been describedin studies of Chern bands with Chern number jCj > 1[22–24], for ... 11,14,20,24,25,41,42,43,44–52]. [41] T. S. Jackson, G. Möller,

5 Feb 2018: 3045. 00.410.811.2. xy. g(r. ). (b) (c). 0 12 24 36 012. ... 2436. 00.51. 11.5. 0 12 24 36 012. 2436. 00.51. 11.5.

2 Apr 2015: 5.3 DOS Parameters. 23. 5.4 JDOS Parameters. 24. 5.5 PDOS Parameters. ... 24 OptaDOS: User Guide. 5.3.7 real(kind=dp) :: dos spacing. Resolution at which to compute the DOS and related properties.

10 Dec 2014: 24) for allfive system sizes shown in Table II and also in Fig. ... Data derived from (24) are shown for systems of N particles at n unitsof flux above the ground state Nφ = N 2 n.

12 Aug 2010: 2Laboratoire de Physique Théorique et Modèles Statistiques, Université Paris-Sud, 91405 Orsay, France3Département de Physique, Laboratoire Pierre Aigrain, ENS, CNRS, 24 rue Lhomond, Paris F-75005, France. ... W. West,Phys. Rev. B 41, 7910 1990. 24 L.

30 Dec 2010: 2This was also found in the studies of Ref. [24] (D.K.K. ... not gauge-invariant. Under the transformation (24) the single-particle density operator becomes.

17 Oct 2023: This article is by contributors to the 4th Royal Society Yusef Hamied Workshop on Artificial Intelligence for India and the UK, held on 24-25 July 2023 in Delhi, India, where

24 Aug 2020: Notably, over the explored T range wesee no indication of a minimum in ρ(T), which is expectedat a certain temperature, depending on the concentrationof Kondo-type scatterers [24]. ... 35, 676(1975). [24] J. Kondo, Resistance minimum in dilute magnetic

24 Aug 2020: Received 24 November 2018; revised manuscript received 5 April 2019; published 10 July 2019). ... TIs are well-known spin-orbit materials, and the in-built potential of the p-n junction [24] provides a clear mech-anism for the breaking of inversion

14 Jan 2013: 2 0.015 4.2e-06 (3,2,3,2) 14.24 10 4 0,0,2 0.005 3.1e-04 (3,2,3,2) 15.34 4 6 ... 0,0,2 0.006 1.7e-05 (3,2,3,2) 14.24 8 8 0,0,2 0.0042 1.3e-07 (3,2,3,2) 15.26 6

12 Aug 2010: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom. 4Laboratoire Pierre Aigrain, Ecole Normale Supérieure, CNRS, 24 rue Lhomond, F-75005 Paris, FranceReceived 1 April 2009; published 23 June 2009.