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1 - 20 of 3,427 search results for KA :ZA31 where 0 match all words and 3,427 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. 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. =. =. =.
  4. 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

  5. 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).

  6. 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

  7. 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.

  8. 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.

  9. 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

  10. 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.

  11. 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).

  12. 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).

  13. 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,

  14. 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,

  15. 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.

  16. 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.

  17. 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.

  18. 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.

  19. qcmft

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

  20. 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:(.

  21. 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).

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