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  2. 2 Oct 2021: deep learning approaches,24 methods that mitigate against training time, as well. ... Ba, Adam: A method for stochastic optimization, arXiv e-prints,. art. arXiv:1412.6980 (2014).24.
  3. Template for Electronic Submission to ACS Journals

    www.tcm.phy.cam.ac.uk/~tmw38/IrwinLevellWhiteheadSegallConduit20.pdf
    2 Oct 2021: QSAR methods 20 including decision trees and random forests 21–23, radial basis functions 24,. ... B. 24. Figure 9. Comparison of the results on the independent test set for best of four QSAR methods.
  4. Deep imputation on large‐scale drug discovery data

    www.tcm.phy.cam.ac.uk/~tmw38/Irwin21.pdf
    2 Oct 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
  5. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/TCMCurrentResearch_2Talk2021.pdf
    14 Jun 2021: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26.
  6. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/SurrogateModelsTalk2017.pdf
    3 Sep 2021: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27.
  7. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ODSCTalk2018.pdf
    7 Sep 2021: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28.
  8. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/NUSTalk2017.pdf
    5 Sep 2021: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.
  9. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ManchesterTalk2017.pdf
    5 Sep 2021: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.
  10. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/LouvainTalk2018.pdf
    7 Sep 2021: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25.
  11. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/LorentzTalk2016.pdf
    3 Sep 2021: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.
  12. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/EPFLTalk2018.pdf
    7 Sep 2021: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25.
  13. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/EngineeringTalk2020.pdf
    11 Sep 2021: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26.
  14. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/DuxfordTalk2018.pdf
    7 Sep 2021: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.
  15. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/DassaultTalk2017.pdf
    5 Sep 2021: Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.
  16. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CamnetTalk2019.pdf
    11 Sep 2021: Slide 22. Slide 23. Slide 24.
  17. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/BPTalk2020.pdf
    11 Sep 2021: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25.
  18. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ASTARTalk2017.pdf
    5 Sep 2021: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27.
  19. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/A_STAR_Talkii2019.pdf
    10 Sep 2021: Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. Slide 26.
  20. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/A_STAR_Talki2019.pdf
    10 Sep 2021: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29.
  21. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/A_STAR_Talk_2020.pdf
    11 Sep 2021: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25.
  22. Machine learning predictions of superalloymicrostructure Patrick L.…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/TaylorConduit21.pdf
    28 Sep 2021: Email: pt409@cam.ac.uk. Preprint submitted to Computational Materials Science September 24, 2021. ... 8 305.2 856.9 31.0 941.4 24.8Frequency 92 38 7.
  23. NICKEL ALLOY COMPOSITION - European Patent Office - EP 2944704 B1

    www.tcm.phy.cam.ac.uk/~gjc29/papers/StoneConduitConduit14.pdf
    30 Aug 2021: a low pressure turbine 24 and an exhaust nozzle 26.
  24. The Journalof Chemical Physics ARTICLE scitation.org/journal/jcp…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/SantakConduit20.pdf
    23 Aug 2021: when modeling viscosity of decane;24 Cho, Jeong,and Buig modeled the viscosity of polymer melts;21 Yang, Pakkanen,and Rowley determined the viscosity index of various lubricant sizemolecules,25 as ... NC Nmol E[δρ](gl ). 6 10 0.697 16 0.518 26 0.579 24
  25. OPTIMADE, an API for exchanging materials data

    www.tcm.phy.cam.ac.uk/~gjc29/papers/OPTIMADE21.pdf
    12 Aug 2021: 24. Ong, S. P. et al. Python Materials Genomics (pymatgen): A robust, open-source python library for materials analysis. ... 24, LT-03225, Vilnius, Lithuania. 12Fritz-Haber-Institut der Max-Planck-Gesellschaft, Faradayweg 4-6, 14195, Berlin, Germany.
  26. Imputation of Sensory Properties Using Deep Learning Samar Mahmoud†,…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/MahmoudIrwinChekmarevVyasKattasWhiteheadMansleyBikkerConduitSegall21.pdf
    15 Oct 2021: latent variables; Radial basis functions (RBF) [24]; Random forests (RF) [22]; and Gaussian process (GP) with. ... kernel-based learning methods, Cambridge, U.K.: Cambridge University Press, 2000. [24] P.
  27. The Journal ofChemical Physics ARTICLE scitation.org/journal/jcp…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/LiuAndrewsConduit19.pdf
    22 Aug 2021: 24 containing no exact. ... Hartree, Math. Proc. Cambridge Philos. Soc. 24, 111–132 (1928).13J. C. Slater, Phys.
  28. Deep Imputation on Large-Scale Drug Discovery Data

    www.tcm.phy.cam.ac.uk/~gjc29/papers/IrwinWhiteheadRowlandMahmoudConduitSegall21.pdf
    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
  29. Practical Applications of Deep Learning To Impute Heterogeneous Drug…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/IrwinLevellWhiteheadSegallConduit20.pdf
    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
  30. A nickel alloy - European Patent Office - EP 2805784 B1

    www.tcm.phy.cam.ac.uk/~gjc29/papers/HardyStoneMignanelliConduitConduit14.pdf
    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.
  31. Temporal fluctuation-induced order in conventional superconductors

    www.tcm.phy.cam.ac.uk/~gjc29/papers/FooConduit21.pdf
    28 Apr 2021: J. Phys. 54, 362 (1986).[24] B. J. Verhaar, J. P. H.
  32. MINET Conference: Measurement, Sensation and Cognition

    www.tcm.phy.cam.ac.uk/~gjc29/papers/DalkeConduitConduitCorso09.pdf
    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.
  33. Alloy composition - European Patent Office - EP 2796580 B1

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitConduitStoneHardy14.pdf
    30 Aug 2021: 21) Application number: 14161255.6. (22) Date of filing: 24.03.2014. (51) Int Cl.:C22C 27/04 (2006.01).
  34. 1498390593355545040-09347118

    www.tcm.phy.cam.ac.uk/~gjc29/papers/ConduitConduitStoneHardy13.pdf
    30 Aug 2021: 45) Date of Patent: May 24, 2016. (54) ALLOY COMPOSITION (56) References Cited. ... U.S. Patent May 24, 2016 US 9,347,118 B2. 16OOP. 1400 - OptimalOW COstalloy'MoB.
  35. PROBABILITY AND MEASURE J. R. NORRIS Contents 1. Measures ...

    www.statslab.cam.ac.uk/~james/Lectures/pm.pdf
    6 Oct 2021: 24. (iii) for some integrable function g, for all x E and all t U,ft (t,x) g(x).
  36. ADVANCED PROBABILITY JAMES NORRIS Contents 0. Review of measure ...

    www.statslab.cam.ac.uk/~james/Lectures/ap.pdf
    3 Oct 2021: 24. (a) X is a martingale,(b) for all bounded stopping times T and all stopping times S, XT is integrable and.
  37. PUBLICATIONS OF HARRY KESTEN 1950 1960 1970 1980 1990 ...

    www.statslab.cam.ac.uk/~grg/papers/kesten-bib.pdf
    18 Oct 2021: Kesten. Continuity of local times forMarkov processes. Compositio Math., 24:277–303, 1972. ... Sidoravicius. A problem in last-passage per-colation. Braz. J. Probab. Stat., 24(2):300–320, 2010.
  38. Part IIC Lent term 2021 QUANTUM INFORMATION AND COMPUTATION ...

    www.qi.damtp.cam.ac.uk/files/PartIIIQC/Part%20IIC%20QIC/PartIIC%20QIClectures%20Full.pdf
    27 Sep 2021: Part IIC Lent term 2021. 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 and the Dirac bra-ket
  39. RECOGNITION-INDUCED UPDATING OF FACE MEMORIES 1 Active Recognition…

    www.memlab.psychol.cam.ac.uk/pubs/Plummer2021%20PsyArXiv.pdf
    25 Oct 2021: RECOGNITION-INDUCED UPDATING OF FACE MEMORIES. 24. choose aspects of their learning experience even when those choices are irrelevant for later.
  40. jcn01770 2328..2341

    www.memlab.psychol.cam.ac.uk/pubs/Korkki2021%20JOCN.pdf
    8 Oct 2021: Mean memory precision (K) was significantlyhigher in the location (M = 34.65, SD = 27.24) in compar-ison to the color condition (M = 10.94, SD = 7.15), t(19) ... 016. Subsequent precision. No significant voxels. Conjoint activity. L middle occipital
  41. OP-BRCM210087 1..14

    www.memlab.psychol.cam.ac.uk/pubs/Gellersen2021%20BrainComms.pdf
    13 May 2021: ACE Memory 25.0 (1.50) 25.1 (1.00) 24.7 (1.53). ROCF immediate 33.3 (2.59) 31.8 (2.69) 32.0 (2.65).
  42. Cop yrig ht © 201 6 U nive rsity ...

    www.damtp.cam.ac.uk/user/tong/vc/benjonathan.pdf
    19 May 2021: mis. sion. 4 Surfaces and Surface Integrals 24. 4.1 Surfaces and Normals 24. ... 24 –. Cop. yrig. ht. 201. 6 U. nive. rsity.
  43. 5 Phase Transitions‣ Statistical Physics by David Tong

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S5.html
    18 Oct 2021: 5 Phase Transitions. 5 Phase Transitions. A phase transition is an abrupt, discontinuous change in the properties of a system. We’ve already seen one example of a phase transition in our discussion of Bose-Einstein condensation. In that case, we
  44. 4 Classical Thermodynamics‣ Statistical Physics by David Tong

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S4.html
    18 Oct 2021: Figure 24:. Expressing the work as. -. d. W. =. -. p. d. V. also allows us to underline the meaning of the new symbol. -.
  45. 3 Quantum Gases‣ Statistical Physics by David Tong

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S3.html
    18 Oct 2021: 3 Quantum Gases. 3 Quantum Gases. In this section we will discuss situations where quantum effects are important. We’ll still restrict attention to gases — meaning a bunch of particles moving around and barely interacting — but one of the
  46. 2 Classical Gases‣ Statistical Physics by David Tong

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S2.html
    18 Oct 2021: 2 Classical Gases. 2 Classical Gases. Our goal in this section is to use the techniques of statistical mechanics to describe the dynamics of the simplest system: a gas. This means a bunch of particles, flying around in a box. Although much of the
  47. 1 The Fundamentals of Statistical Mechanics‣ Statistical Physics by…

    www.damtp.cam.ac.uk/user/tong/statphys/statmechhtml/S1.html
    18 Oct 2021: ρ. =. e. -. β. H. Z. (1.24). If we make a measurement described by an operator. ... In the quantum context, it is sometimes written in terms of the density matrix (1.24) as.
  48. 3 The Renormalisation Group‣ Statistical Field Theory by David Tong

    www.damtp.cam.ac.uk/user/tong/sft/sfthtml/S3.html
    16 Oct 2021: ζ. Δ. ϕ. ϕ. (. 𝐱. ). Figure 24: RG flows when.
  49. 1 From Spins to Fields‣ Statistical Field Theory by David Tong

    www.damtp.cam.ac.uk/user/tong/sft/sfthtml/S1.html
    16 Oct 2021: 1.24). Here, the notation. {. s. i. }. |. m. (. 𝐱. ). means that we sum over all configurations of spins such that the coarse graining yields. ... We will invoke one last notational flourish. We’re left in (1.24) with a sum over all possible
  50. dynrel

    www.damtp.cam.ac.uk/user/tong/relativity/two.pdf
    12 Jun 2021: perpendicular to B. In the last line, we’ve used the equation (2.24). ... oscillating with frequency! = qB/m. However, because of the constraint (2.24), the.
  51. dynrel

    www.damtp.cam.ac.uk/user/tong/relativity/six.pdf
    12 Jun 2021: anti-clockwise in the Southern hemisphere. Notice that the period of rotation is not 24. ... hours unless the pendulum is suspended at the poles. Instead the period is 24/ sin.

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