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1 - 50 of 3,426 search results for KA :ZA31 where 0 match all words and 3,426 match some words.

  1. Results that match 1 of 2 words

  2. Electronic and Photonic Nanodevices Group

    www3.eng.cam.ac.uk/~hjj28/publications.html
    P Parkinson, C Dodson, HJ Joyce, KA Bertness, NA Sanford, LM Herz, MB Johnston.

  3. Theta oscillation-coupled dendritic spiking integrates inputs on a…

    www3.eng.cam.ac.uk/~go223/Publications/huhn05.pdf
    8 Jun 2010: Neuron 40:177–188. Bernander O, Douglas RJ, Martin KA, Koch C. 1991.

  4. DEVELOPMENT AND APPLICATIONOF A PROGRAM FOR THE COMPUTER AIDED ...

    www3.eng.cam.ac.uk/outreach/Project-resources/Senior-glider/Aery-technical-paper.pdf
    12 Oct 2011: a. c c Ka cK. K c a Kc. =. =. =.
  5. Thumbnail for www.youtube.com/watch?v=cjbhQUML-KA&feature=youtube_gdata_player
    00:02:17

    Valencia Yacht Club Design

    Duration: 00:02:17
    Published Date: 2011/10/25
    First prize in the Carl Zeiss video competition at the University of Cambridge, Department of Engineering : 'Valencia Yacht Club Design Video' Undergraduate students had to come up with an interesting design for a tension structure and do all the complicated nonlinear structural calculations to show that the structure would stand up. Even if we ignore the video, the design is brilliant on so many

  6. PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...

    www.tcm.phy.cam.ac.uk/~tmw38/Whitehead16a.pdf
    5 Apr 2016: 2), which gives. ψ cont0 (r) J0(kr) π. 2[γ ln(ka/2)] Y0(kr), (7). ... 9) of (kR)2/2π , and so describe the scattering correctto O((ka)4).

  7. Theoretical Physics II

    www.tcm.phy.cam.ac.uk/~rjs269/TP2/TP2y2024.pdf
    22 Jan 2024: Department of PhysicsUniversity of Cambridge. Part II Physics. T H E O R E T I C A L P H Y S I C S I I. T O P I C S I N Q U A N T U M T H E O R Y. R.-J. Slager and G. ChaudharyLent 2024. Contents. 1 Quantum Dynamics 7. 2 Introduction to path

  8. NATURAL SCIENCES TRIPOS Part II Wednesday 13 January 2016 ...

    www.tcm.phy.cam.ac.uk/~nrc25/TP1/ExamFiles/exam16sol.pdf
    7 Jan 2019: 2mṙθ̇ mrθ̈ = ka sin(θ θB). d. dt. L. ṙ=L. ... r= mr̈ = mrθ̇2 kr ka cos(θ θB). d. dt. L.

  9. Publications 1980 - 1989

    www.tcm.phy.cam.ac.uk/~mw141/1980.html
    13 Dec 2009: Phys. A18 3007-3026 (1985) (23) Frequency Dependence of NMR Spin-Lattice Relaxation in Bilayer Membranes JA Marqusee, M Warner and KA Dill, J.

  10. LagrangianDynamics Engineering Part IBPaper 1 Lectures 9-16 J. S. ...

    www.tcm.phy.cam.ac.uk/~jsb56/resources/1B_Mechanics_handout.pdf
    24 Oct 2022: LagrangianDynamics. Engineering Part IBPaper 1. Lectures 9-16. J. S. Biggins. Engineering Department. University of Cambridge. Lent 2022. CONTENTS CONTENTS. Contents. 1 Course Details vi. 1.1 Synopsis. vi. 1.2 Practicalities. vii. 2 Generalized

  11. PHYSICAL REVIEW A 82, 063625 (2010) Condensed ground states ...

    www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevA.82.063625.pdf
    30 Dec 2010: By. are shown in Fig. 3. They are related by kAy kBy = 2π α.1Hence, cos(kA(B)y ) = cos(kB(A)y 2π α), so the Hamiltonian (8)is the ... 1Note that the positions kA(B) of these minima are gauge dependent.

  12. PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/Whitehead16.pdf
    24 Aug 2020: 2), which gives. ψ cont0 (r) J0(kr) π. 2[γ ln(ka/2)] Y0(kr), (7). ... 9) of (kR)2/2π , and so describe the scattering correctto O((ka)4).

  13. PHYSICAL REVIEW A 96, 023619 (2017) Effective-range dependence of ...

    www.tcm.phy.cam.ac.uk/~gjc29/papers/SchonenbergVerpoortConduit17.pdf
    24 Aug 2020: cot[δ(k)] = 2π. ln(ka) k2R2eff. 4. (1). Here a is the scattering length and Reff the effective range. ... f (k) = 4 2. πln(ka) k2R2eff4 i. (8). Matching both expressions, we can express ω0 and λ in termsof a and Reff ,. ω0 = 8π R2eff. ln(qa), (9a).

  14. Machine learning to predict mesenchymal stem cell efficacy for…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/LiuLuOhConduit20.pdf
    11 Nov 2020: RESEARCH ARTICLE. Machine learning to predict mesenchymal. stem cell efficacy for cartilage repair. Yu Yang Fredrik LiuID1, Yin Lu2, Steve Oh2, Gareth J. ConduitID1. 1 Theory of Condensed Matter Group, Cavendish Laboratory, University of Cambridge,

  15. Quantum Order-by-Disorder in Strongly Correlated Metals Andrew G.…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/GreenConduitKruger17.pdf
    24 Aug 2020: Quantum Order-by-Disorder in Strongly Correlated Metals. Andrew G. Green,1 Gareth Conduit,2 and Frank Krüger1, 31London Centre for Nanotechnology, University College London,. Gordon St., London, WC1H 0AH, United Kingdom2TCM, Cavendish Laboratory,

  16. PHYSICAL REVIEW A 90, 033626 (2014) High-fidelity pseudopotentials…

    www.tcm.phy.cam.ac.uk/~gjc29/papers/BugnionLopezRiosNeedsConduit14.pdf
    24 Aug 2020: δcont (k) ={. arctan(ka), = 0,0, > 0,. is the scattering phase shift in the angular momentum channel. ... RcontE,=0(r) =sin[kr δ0(k)]. kr,. where δ0(k) = arctan(ka) and k =. E. The continuityequations at the cutoff are. p(rc) = ln{. sin[krc δ0(k)]rc.

  17. Absence of diagonal force constants in cubic Coulomb crystals

    www.tcm.phy.cam.ac.uk/~gjc29/papers/AndrewsConduit20.pdf
    23 Dec 2020: Math. Mech. Solids 13, 199–220. (doi:10.1177/. 1081286507086898)3. Grimvall G, Magyari-Köpe B, Ozoliņš V, Persson KA.

  18. NATURAL SCIENCES TRIPOS Part II Wednesday 13 January 2016 ...

    www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam16sol.pdf
    20 Jan 2016: 2mṙθ̇ mrθ̈ = ka sin(θ θB). d. dt. L. ṙ=L. ... r= mr̈ = mrθ̇2 kr ka cos(θ θB). d. dt. L.

  19. qcmft

    www.tcm.phy.cam.ac.uk/~bds10/tp3/secqu.pdf
    10 Oct 2012: Ĥ = JN S2 B.Z.Xk! ka†kak O(S0) (2.16). where! k = 2JS(1 cos k) = 4JS sin2(k/2) represents the dispersion relation of the spinexcitations.

  20. qcmft

    www.tcm.phy.cam.ac.uk/~bds10/tp3/ps2.pdf
    10 Oct 2012: cos ka. ——————————————–. Quantum Condensed Matter Field Theory.

  21. Lecture I 1 Lecture I: Collective Excitations: From Particles ...

    www.tcm.phy.cam.ac.uk/~bds10/tp3/lectures.pdf
    10 Nov 2013: ka†k. )] O(N. 1/20 ). cf. quantum AF in spin-wave approximation. ... 2. (akak a. †ka†k. )]As with quantum AF, Ĥ diagonalised by Bogoluibov transformation:(.

  22. phmain

    www.tcm.phy.cam.ac.uk/~bds10/phase/topol.pdf
    4 Apr 2010: The first indication of unusual behaviour in the two-dimensional XY -model (n = 2)appeared in an analysis of the high temperature series expansion by Stanley and Ka-plan (1971).

  23. 16.4. PROBLEM SET IV 216 16.4 Problem Set IV ...

    www.tcm.phy.cam.ac.uk/~bds10/aqp/ps4.pdf
    22 Nov 2009: and verify that the scattering is isotropic when the energy of the incidentparticle or the size of the scatterer is sufficiently low, so that Ka 1.Obtain an expression for the

  24. lectures

    www.tcm.phy.cam.ac.uk/~bds10/aqp/lec2_compressed.pdf
    21 Oct 2009: κa =. {ka tan(ka) evenka cot(ka) odd. κa =. (2ma2V0! 2 (ka)2. ... leads to the condition,. k [An1 cos(ka) Bn1 sin(ka) An] =2maV0!

  25. lectures

    www.tcm.phy.cam.ac.uk/~bds10/aqp/lec2.pdf
    12 Oct 2009: κa =. {ka tan(ka) evenka cot(ka) odd. κa =. (2ma2V0! 2 (ka)2. ... leads to the condition,. k [An1 cos(ka) Bn1 sin(ka) An] =2maV0!

  26. lectures

    www.tcm.phy.cam.ac.uk/~bds10/aqp/lec16-17_compressed.pdf
    17 Nov 2009: eikna = ks (eika eika). 1N. eikna2ks cos(ka). We therefore find that. ... Classical chain: normal modes. ωk = 2. ksm| sin(ka/2)|. At low energies, k 0, (i.e.

  27. lectures

    www.tcm.phy.cam.ac.uk/~bds10/aqp/lec16-17.pdf
    17 Nov 2009: Substituted into the equations of motion, we obtain. (mω2 2ks ) = 2ks cos(ka). ... ksm| sin(ka/2)|. Classical chain: normal modes. ωk = 2. ksm| sin(ka/2)|.

  28. lectures

    www.tcm.phy.cam.ac.uk/~bds10/aqp/lec15_compressed.pdf
    9 Nov 2009: For N lattice sites and periodic boundary condition, αnN = αn,solution given by αn =. 1N. eikna,. E = Ek =ε 2t cos(ka)1 S cos(ka). i.e.

  29. lectures

    www.tcm.phy.cam.ac.uk/~bds10/aqp/lec15.pdf
    9 Nov 2009: For N lattice sites and periodic boundary condition, αnN = αn,solution given by αn =. 1N. eikna,. E = Ek =ε 2t cos(ka)1 S cos(ka). i.e.

  30. Chapter 10 From molecules to solids In the previous ...

    www.tcm.phy.cam.ac.uk/~bds10/aqp/handout_molecular.pdf
    9 Nov 2009: Substitution confirms that this is a solution with energies(exercise),. Ek =ε 2t cos(ka)1 S cos(ka).

  31. Chapter 2 Quantum mechanics in onedimension Following the rules ...

    www.tcm.phy.cam.ac.uk/~bds10/aqp/handout_1d.pdf
    8 Oct 2009: Thefigure (right) compares κa = ( 2mV0a. 2! 2 (ka)2)1/2 with ka tan(ka) for the even. ... Bn1 =2maV0! 2k Bn sin(ka) Bn cos(ka) An sin(ka). Advanced Quantum Physics.

  32. ans4

    www.tcm.phy.cam.ac.uk/~bds10/aqp/ans4.pdf
    20 Jan 2010: A sin(kR) = sin(KR δ0)kA cos(kR) k cos(kR δ0) = U0 sin(kR δ0).

  33. Phase Transitions and Collective Phenomena

    www.tcm.phy.cam.ac.uk/~achc2/phase/notes.pdf
    4 Jan 2023: Phase Transitions and CollectivePhenomena. Anson Cheungachc2@cam.ac.uk. January 2023. ii. Preface. The fundamental goal of statistical mechanics is to provide a framework in which themicroscopic probabilistic description of systems with large

  34. Chapter 5 Topological Phase Transitions Previously, we have seen ...

    www.tcm.phy.cam.ac.uk/~achc2/phase/chap5.pdf
    25 Jan 2021: The first indication of unusual behaviour in the two-dimensional XY -model (n = 2)appeared in an analysis of the high temperature series expansion by Stanley and Ka-plan (1971).

  35. Group Publicatons

    www.tcm.phy.cam.ac.uk/publications/Pubs2015.html
    KA Asghar, DA Rowlands, JM Elliott and AM Squires, ACS Nano 9 10970 - 10978 (2015).

  36. Group Publicatons

    www.tcm.phy.cam.ac.uk/publications/Pubs2014.html
    Hybrid MPI-OpenMP Parallelism in the ONETEP Linear-Scaling Electronic Structure Code: Application to the Delamination of Cellulose Nanofibrils KA Wilkinson, NDM Hine and C-K Skylaris, J. ... KA See et al., J.

  37. Daniel Rowlands

    www.tcm.phy.cam.ac.uk/profiles/dar55/
    27 Feb 2018: Predicting Sizes of Hexagonal and Gyroid Metal Nanostructures from Liquid Crystal Templating KA Asghar, DA Rowlands, JM Elliott, and AM Squires ACS Nano 9(11) 10970-10978 2015.

  38. Alumni of TCM Group

    www.tcm.phy.cam.ac.uk/about/alumni/
    1 Apr 2024: KA Kikoin (visitor 1994-95). RJ Kingdon (gs. 1986-87). DR Kingham (gs.

  39. 4 Solutions of the 1D Schrödinger equation We now ...

    www.qi.damtp.cam.ac.uk/files/Adrian/notespart2.completed.2019.pdf
    6 Nov 2019: or B = 0 , cos(ka) = 0 ,. ψ(x) = A cos(kx) , k =nπ. ... C cos(la) = A exp(ka) , (4.40)lC sin(la) = kA exp(ka).

  40. Part IB Quantum Mechanics, Michaelmas 2019 Tuesday and Thursday, ...

    www.qi.damtp.cam.ac.uk/files/Adrian/notes311219.pdf
    3 Jan 2020: Part IB Quantum Mechanics, Michaelmas 2019. Tuesday and Thursday, 11.05 a.m. to 11.55 a.m., Mill Lane lecture room 3. Prof. Adrian Kent (apak@damtp.cam.ac.uk). I am very grateful to previous lecturers of this course, and in particular toJonathan

  41. Part IB Quantum Mechanics, Michaelmas 2019 Tuesday and Thursday, ...

    www.qi.damtp.cam.ac.uk/files/Adrian/notes160520.pdf
    16 May 2020: Part IB Quantum Mechanics, Michaelmas 2019. Tuesday and Thursday, 11.05 a.m. to 11.55 a.m., Mill Lane lecture room 3. Prof. Adrian Kent (apak@damtp.cam.ac.uk). I am very grateful to previous lecturers of this course, and in particular toJonathan

  42. (Lecture3)

    www.phase-trans.msm.cam.ac.uk/mphil/MP7-3.pdf
    7 Jun 2010: b 0.15 15. c 0.4 80. ka. = 100. 0.1. (1 11 1. ). =.

  43. (Lecture 9, Overall Kinetics)

    www.phase-trans.msm.cam.ac.uk/mphil/MP6-9.pdf
    7 Jun 2010: where kA. and n characterise the reaction as a function of time, temperature and other. ... variables. The values of kA. and n can be obtained from experimental data by plotting.

  44. Part II Materials Science and Metallurgy Example of a ...

    www.phase-trans.msm.cam.ac.uk/litsur/litsur.pdf
    7 Jun 2010: ξ = 1 exp{kAtn} (2). where t is the time, kA and n rate constants and ξ is given by.

  45. FULL CRITICAL REVIEW CementiteH. K. D. H. Bhadeshia Materials ...

    www.phase-trans.msm.cam.ac.uk/2019/Cementite.pdf
    23 Nov 2019: 113] and Joubouri et al.[118] – the latter has been corrected to the Co Ka wavelengthto permit the comparison.

  46. Phase quantification in nanobainite via magnetic measurements and…

    www.phase-trans.msm.cam.ac.uk/2014/Magnetisation.pdf
    25 Nov 2014: Sample V ms / A m2 kg1 He / kA m1.

  47. Oxidation of silicon containing steel E. J. Song1, D. ...

    www.phase-trans.msm.cam.ac.uk/2012/red_Song_ISM_2012.pdf
    13 Oct 2012: X-ray diffractionexperiments were conducted using Cu Ka radiation withthe beam step scanned at 0?2u min21.

  48. Master thesis Spot Weldability of TRIP Steel with High ...

    www.phase-trans.msm.cam.ac.uk/2012/Jung_geunsu-_Master_thesis.pdf
    28 Jan 2012: uncoated steel [41]. Weld current = 7.4 kA. 20. Fig. 2.14 contact resistance comparison of AC and DC welding [42].

  49. Estimation of fracture toughness of temperednanostructured bainite A. …

    www.phase-trans.msm.cam.ac.uk/2012/fracture_Hamdany_MST_2012.pdf
    11 Jun 2012: X-ray diffraction was used to determine the phasefractions, using Cu Ka irradiation at 40 kV and 40 mA.The sample was scanned over the 2h range 30–150u andthe fractions

  50. Spot weldability of TRIP assisted steels withhigh carbon and ...

    www.phase-trans.msm.cam.ac.uk/2012/delta_Jung_STWJ_2012.pdf
    17 Jan 2012: The microstructures of the weld nuggets are given inFig. 7 for cases where the current was 0?5 kA less thanImax. ... Table 4 Joint properties for commercial and investigated alloys. Carbon/wt-%Thickness/mm. Minimum weldcurrent/kA.

  51. Spot weldability of d-TRIP steel containing0?4 wt-%C H. L. ...

    www.phase-trans.msm.cam.ac.uk/2010/stw1721.pdf
    11 Oct 2010: Alloy Current, kA Nugget, mm. Tensile shear strength Cross-tensile strength. Maximum load, kN Fracture Maximum load, kN Fracture.

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