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101 - 150 of 556 search results for TALK:PC53 20 |u:www.tcm.phy.cam.ac.uk where 0 match all words and 556 match some words.

  1. Results that match 1 of 2 words

  2. Bibliography

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper13/node11.html
    28 Oct 2002: Rev. B 51 9668. 20.

  3. AWGIF 2015

    www.tcm.phy.cam.ac.uk/AWG/2015awgif/programme.html
    31 Aug 2015: Confirmation of selected participants. July 20-22, 2015. AWGIF.

  4. Density-functional calculations

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper8/node3.html
    31 Oct 2002: Next: Results of the calculations Up: First-principles density-functional calculations using Previous: Origin of the basis.. Density-functional calculations. The Kohn-Sham (KS) equation for an. -electron system is[. (6). where. are the KS

  5. Corrected penalty-functional method for linear-scaling calculations…

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper2/
    25 Oct 2002: Experimental values and results of the. CASTEP. plane-wave code [19], using the same pseudopotential [20] and equivalent Brillouin zone sampling are also shown.

  6. About this document ...

    www.tcm.phy.cam.ac.uk/~bdj10/psi/delanoy/node9.html
    3 Sep 1996: HTML. translator Version 95.1 (Fri Jan 20 1995) Copyright 1993, 1994, Nikos Drakos, Computer Based Learning Unit, University of Leeds. ... dir www/psi delanoy.tex. The translation was initiated by Brian Josephson on Tue Sep 3 20:37:32 BST 1996.

  7. cultural biases against psi

    www.tcm.phy.cam.ac.uk/~bdj10/psi/bias1.html
    20 Dec 2000: 20. David Fisher (July 2000, p. 22) rejects parapsychology on the basis of difficulty in replicating positive results in the field.

  8. Publications: Gunnar Möller

    www.tcm.phy.cam.ac.uk/~gm360/papers/index.html
    2 Jul 2024: Gunnar Möller and Nigel R. Cooper. New Journal of Physics 20, 073025 (2018). ... 20, 3533 (2006). Composite Fermions in Negative Effective Field: A Monte-Carlo Study.

  9. Bibliography

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper14/node11.html
    10 Feb 2004: Phys. Rev. B 55 (20), 13485 (1997). 18. ... total-energy pseudopotential calculations. Comput. Phys. Commun. 102 (1-3), 17 (1997). 20.

  10.  Oscillating Systems Oscillating Systems Natural SciencesPhysics…

    www.tcm.phy.cam.ac.uk/~jsb56/resources/osc_slides/lecture_9/index.html
    30 Nov 2015: top:0px;width:45.81px;height:43.31px" > </div> <div class="sg" id="s30" data-sgid="Straight Arrow Connector 69" ... png" style="z-index:1;left:0px;top:0px;width:391.47px;height:31.64px" > </div> <div class="sg" id="s81" data-sgid="Picture 2"

  11. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/AustriaTalk2024.pdf
    7 May 2024: Slide 15. Slide 16. Slide 17. Slide 18. Slide 19. Slide 20.

  12. AWGIF 2015

    www.tcm.phy.cam.ac.uk/AWG/2015awgif/participants.html
    31 Aug 2015: Application deadline. May 3, 2015. Confirmation of selected participants. July 20-22, 2015.

  13. Publications: Biology

    www.tcm.phy.cam.ac.uk/~bds10/dir/publications_bio.html
    15 Jun 2024: Nature Cell Biology 20, 677-687 (2018) | doi:10.1038/s41556-018-0108-1 | PMCID: PMC6984964. ... Nature Cell Biology 20, 127-134 (2018) | doi:10.1038/s41556-017-0013-z | PMCID: PMC5787369.

  14. TCM at Sixty: Timetable

    www.tcm.phy.cam.ac.uk/events/sixtieth/timetable.html
    10 Jul 2015: 16:20: Dr Alix Pryde (Vodafone) Physics to the Rescue! - How I've used my physics background to solve business problems.

  15. Bibliography

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper11/node10.html
    31 Oct 2002: 72, 1240 (1994). 20.

  16. 4. Overlap matrix elements

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper1/node4.html
    22 Sep 1999: 19). (20). where. (21). For the case when. , we note that since the integrand in equation (17) must still only have a simple pole at.

  17. Total energy optimisation

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper11/node3.html
    31 Oct 2002: 20). We choose to carry out the total energy minimisation in two nested loops, in a fashion similar to the ensemble DFT method of Marzari et al. ... but we also impose the electron number and idempotency constraints (19) and (20).

  18. FT-E.dvi

    www.tcm.phy.cam.ac.uk/impact/FT-E22.pdf
    25 Apr 2022: 6 May. ON DUALITY. • 13 May. QUANTUM BOX. • 20 May.

  19. Dr McGinley

    www.tcm.phy.cam.ac.uk/profiles/mm2025/
    14 Apr 2024: About. Research. People. Events. Join us. Impact. Max McGinley. Dr Max McGinley. Fellow of Trinity College. Office: 505 Mott Bld. Phone: 44(0)1223 3 37380. Email: mm2025 @ cam.ac.uk. SPT Lectures feedback form:. TCM Group, Cavendish Laboratory.

  20. www.tcm.phy.cam.ac.uk/~as3546/publication/index.xml

    www.tcm.phy.cam.ac.uk/~as3546/publication/index.xml
    12 Feb 2024: waves with vertical odd viscosity https://www.tcm.phy.cam.ac.uk/as3546/publication/2204.09375/ Wed, 20 Apr 2022 00:00:00 0000

  21.  Oscillating Systems Oscillating Systems Natural SciencesPhysics…

    www.tcm.phy.cam.ac.uk/~jsb56/resources/osc_slides/lecture_6/index.html
    19 Nov 2014: 25" style="z-index:2;left:10.79px;top:101.21px;width:416.69px;height:20.87px"> <img class="sg" src="FA548664.png" id="s14_i" title="" alt="TP_tmp.png" ... style="z-index:1;left:0px;top:0px;width:184.70px;height:20.87px" > </div>.

  22. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/SharpeningEdgeTalk2024.pdf
    13 May 2024: Slide 20. Slide 21.

  23. programmeAWGSRG

    www.tcm.phy.cam.ac.uk/AWG/2023awgsrg/programmeAWGSRG.pdf
    6 Sep 2023: 16:00-16:20 E.Lhotel (Institut Neel CNRS): Fluctuation-dissipation relation in spin ices Dy2Ti2O7 and Ho2Ti2O7: preliminary results16:20-16:40 S.Davis (Oxford/Cork): Quantum spin noise ... 17:00-17:20 S.Bhattacharjee (ICTS): Spin-3/2 ice17:20-17:40

  24. lectures

    www.tcm.phy.cam.ac.uk/~bds10/aqp/lec20-21.pdf
    27 Nov 2009: K 2 = k2 U0. With kR ' 1, K % U1/20 (1 O(k2/U0)), find scattering length,. ... σtot %4π. k2sin2 δ0(k) % 4πR2. (tan(KR). KR 1. )2, K % U1/20.

  25. KINETICS.dvi

    www.tcm.phy.cam.ac.uk/impact/KINETICS-2022.pdf
    19 Oct 2022: ficients of atomic gases. • 20 October. LECTURE 4. Self-consistent field and collision-less dynamics for plasma.

  26. Phase Transitions and Collective Phenomena Anson…

    www.tcm.phy.cam.ac.uk/~achc2/phase/lec1_slides.pdf
    27 Jan 2024: e.g. Vortices in atomic superfluid. 20. e.g. disclinations in a liquid crystal.

  27. Page 1/28 Modelling nicotine pharmacokinetic pro�le for e-cigarette…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/PrasadEdward24.pdf
    3 Jul 2024: 23 40 58.6 168 20.8 29.0 29.2 F 4 1317. 24 34 85.4 162 32.5 48.3 22.5 F 8 1536. ... Regul Toxicol Pharmacol. 2018 Mar;93:84-91. Page 20/28. 15. Goldenson NI, Buchhalter AR, Augustson EM, Rubinstein ML, Van Hoof D, Henningeld JE.

  28.  Oscillating Systems Oscillating Systems Natural SciencesPhysics…

    www.tcm.phy.cam.ac.uk/~jsb56/resources/osc_slides/lecture_4/index.html
    18 Nov 2014: width:621.04px;height:42.20px" > </div> <div class="sg" id="s23" data-sgid="Rectangle 20" ... div class="sg" id="s41" data-sgid="Picture 35" style="z-index:20;left:109.75px;top:49.27px;width:507.10px;height:27.61px"> <img class="sg" src="2B822998.png"

  29. Modus Operandi of New Energy Times

    www.tcm.phy.cam.ac.uk/~bdj10/articles/NET1.html
    8 Mar 2012: and want to market a 1kW heat source, you can simply install 20 of your 50 watt devices, and then, by simple arithmetic, you end up with a 1kW heat source.

  30. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/KymabTalk2020.pdf
    7 Nov 2021: Acc. urac. y. 0 10 20 30 40 50 60 70 80 90 100. ... Matrix factorize. 0 10 20 30 40 50 60 70 80 90 100.

  31. Ginzburg-Landau theory Define www.graidmagmtmhfutd mind i.e in the…

    www.tcm.phy.cam.ac.uk/~achc2/written/lec3.pdf
    1 Feb 2021: Tfcm. no. et n9. so. break ukofstuhh.ly. slowlyIml. t 20. h.

  32.  Oscillating Systems Oscillating Systems Natural SciencesPhysics…

    www.tcm.phy.cam.ac.uk/~jsb56/resources/osc_slides/lecture_3/index.html
    15 Nov 2014: data-sgid="Rectangle 20" style="z-index:6;left:61.53px;top:248.35px;width:597.54px;height:35.86px" data-fillcolor="16777215"> <img class="sg" src="2371A947.png" ... i" title="" alt="TP_tmp.png"

  33. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ASTARTalk2023.pdf
    15 Jan 2023: 40 cohort tracked patients (20 developed acute myeloid leukaemia cancer, 20 did not). ... Slide 15. Slide 16. Slide 17. Slide 18. Slide 19. Slide 20.

  34.  Oscillating Systems Oscillating Systems Natural SciencesPhysics…

    www.tcm.phy.cam.ac.uk/~jsb56/resources/osc_slides/lecture_12/index.html
    30 Nov 2015: 15" style="z-index:20;left:249.72px;top:158.64px;width:152.55px;height:50.73px"> <img class="sg" src="D6908071.png" id="s29_i" title="" alt="TP_tmp.png" ... 47.85px;height:59.37px" > </div> <div class="sg" id="s77" data-sgid="Picture 20" style="z-index:23

  35. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/UCLTalk2013.pdf
    24 Aug 2020: Elongation 15.2Weldability 8.0 %Oxidation 20. Electron micrograph. Yield stress. Yield stress. ... Elongation 15.2Weldability 8.0 %Oxidation 20. Partners. Heat treatments. Tβ. α βP.

  36.  Oscillating Systems Oscillating Systems Natural SciencesPhysics…

    www.tcm.phy.cam.ac.uk/~jsb56/resources/osc_slides/lecture_8/index.html
    24 Nov 2015: 20" style="z-index:9;left:362.58px;top:64.89px;width:73.29px;height:76.14px" data-pointer-events="none"> <img class="sg" src="4F47B1DB.png" id="s31_i" ... 25px" > </div> <div class="sg" id="s42" data-sgid="Straight Arrow Connector 42"

  37. FT-L.dvi

    www.tcm.phy.cam.ac.uk/impact/FT-L23.pdf
    1 Jan 2023: FAIRY TALES. Lent Term. • 20 January. RESTRICTED THREE BODY PROBLEM. •

  38. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2017.pdf
    24 Aug 2020: 2Fx=1. 2100.1=0.5 J. Modern materials: rubbers. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1. ... Potential energy in enormous band. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1.

  39.  Oscillating Systems Oscillating Systems Natural SciencesPhysics…

    www.tcm.phy.cam.ac.uk/~jsb56/resources/osc_slides/lecture_11/index.html
    30 Nov 2015: z-index:1;left:0px;top:0px;width:460.68px;height:31.18px" > </div> <div class="sg" id="s29" data-sgid="Picture 24" ... style="z-index:20;left:33.12px;top:152.89px;width:381.27px;height:73.05px" data-pointer-events="none"> <img class="sg" src="422C3A5A.png

  40. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2012.pdf
    24 Aug 2020: E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J. Alloys – where are they used? • ... Potential energy in enormous band:. E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J.

  41. 001.NewContents.dvi

    www.tcm.phy.cam.ac.uk/impact/Physical-2020.pdf
    6 Oct 2020: damping. 20. 1. Lecture 5. Diffusion approximation for the Boltzmann equa-.

  42.  Oscillating Systems Oscillating Systems Natural SciencesPhysics…

    www.tcm.phy.cam.ac.uk/~jsb56/resources/osc_slides/lecture_7/index.html
    21 Nov 2014: 84px" > </div> <div class="sg" id="s14" data-sgid="Picture 13" style="z-index:2;left:20.74px;top:95.08px;width:674.31px;height:23.28px"> <img class="sg" ... sgid="Picture 15" style="z-index:3;left:20.74px;top:130.46px;width:527.14px;height:27.59px"> <img

  43. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2016.pdf
    24 Aug 2020: 2Fx=1. 2100.1=0.5 J. Modern materials: rubbers. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1. ... Potential energy in enormous band. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1.

  44.  Oscillating Systems Oscillating Systems Natural SciencesPhysics…

    www.tcm.phy.cam.ac.uk/~jsb56/resources/osc_slides/lecture_10/index.html
    28 Nov 2014: style="z-index:1;left:0px;top:0px;width:42.21px;height:31.78px" > </div> <div class="sg" id="s29" data-sgid="Picture 44" ... sg" id="s92" data-sgid="Straight Connector 20" style="z-index:23;left:317.37px;top:126.04px;width:104.59px;height:11.39px"

  45. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2015.pdf
    24 Aug 2020: 2Fx=1. 2100.1=0.5 J. Modern materials: rubbers. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1. ... Potential energy in enormous band. E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1.

  46. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2014.pdf
    24 Aug 2020: 20.0053002=225 J. E=12kx2=1. 2Fx=1. 2100.1=0.5 J. Modern materials: rubbers. • Potential energy in elastic band:. • ... E=12mv2=1. 20.0053002=225 J. E=12kx2=1. 2Fx=1. 21005=250 J. E=12kx2=1. 2Fx=1. 2100.1=0.5 J.

  47. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/NUSTalk2017.pdf
    5 Sep 2021: Proposed alloy. Cr:15.8 Co: 20.0 Mo: 0.5 W: 0.5 Ta: 4.9 Nb: 1.1 Al: 2.4. ... Slide 19. Slide 20. Slide 21. Slide 22. Slide 23. Slide 24.

  48. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/EMMCTalk2023.pdf
    28 Apr 2023: cost < 0.028 £ kg-1. density < 2350 kg m-3. strength > 20 MPa. ... Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25.

  49. 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.

  50. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/ESDGTalk2012.pdf
    24 Aug 2020: Reduced three-body losses. m /m=1. m /m=20/3. Reduced two-body losses. m /m=1. ... m /m=20/3. Repulsive Non-interacting. Trapped behavior. • At high interaction strength light atoms forced to outside.

  51. Slide 1

    www.tcm.phy.cam.ac.uk/~gjc29/talks/CaiusTalk2013.pdf
    24 Aug 2020: Kinetic energy in handgun bullet:. E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J. ... Potential energy in enormous band:. E=12kx2=1. 2Fx=1. 2100.1=0.5J. E=12mv2=1. 20.0054002=400J.

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