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  1. Results that match 1 of 2 words

  2. 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.
  3. 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
  4. 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).
  5. 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,
  6. 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,
  7. 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
  8. qcmft

    www.tcm.phy.cam.ac.uk/~bds10/tp3/ps2.pdf
    10 Oct 2012: cos ka. ——————————————–. Quantum Condensed Matter Field Theory.
  9. 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.
  10. 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).
  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.

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