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13 Dec 2009: Phys. A18 2325-41 (1985) (24) Rod to Coil Transitions in Nematic Polymers M Warner, JMF Gunn and A Baumgärtner, J. ... Phys. A18 3007-3026 (1985) (23) Frequency Dependence of NMR Spin-Lattice Relaxation in Bilayer Membranes JA Marqusee, M Warner and KA

24 Oct 2022: 23. 6.5 Second integral of the equation of motion. 24. 6.5.1 Second integral for the simple pendulum (non-examinable).

30 Dec 2010: 2This was also found in the studies of Ref. [24] (D.K.K. ... not gauge-invariant. Under the transformation (24) the single-particle density operator becomes.

24 Aug 2020: 9) of (kR)2/2π , and so describe the scattering correctto O((ka)4). ... Mueller, Phys. Rev. A 78,. 033607 (2008).[24] X. Li, J. Kolorenč, and L.

24 Aug 2020: cot[δ(k)] = 2π. ln(ka) k2R2eff. 4. (1). Here a is the scattering length and Reff the effective range. ... R3Deff < 0 for narrow Feshbachresonances and R3Deff 0 for broad Feshbach resonances so thatin typical experiments exploiting the full gamut of

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,

24 Aug 2020: dau damping propagates under renormalization to allterms in an expansion of the action[22, 24–27]. ... 4. 4.5. 5. 5.5. 6. |q(rlu)|. T(K. ). 0.2 0.21 0.22 0.23 0.24.

24 Aug 2020: δcont (k) ={. arctan(ka), = 0,0, > 0,. is the scattering phase shift in the angular momentum channel. ... 2005).[24] D. L. Maslov and A. V. Chubukov, Phys. Rev. B 81, 045110.

23 Dec 2020: Math. Mech. Solids 13, 199–220. (doi:10.1177/. 1081286507086898)3. Grimvall G, Magyari-Köpe B, Ozoliņš V, Persson KA.

10 Oct 2012: 24 CHAPTER 2. SECOND QUANTISATION. Our aim is to find an operator V̂ in second quantised form whose action on a many-bodystate gives. ... 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