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Electronic and Photonic Nanodevices Group
www3.eng.cam.ac.uk/~hjj28/publications.htmlP Parkinson, C Dodson, HJ Joyce, KA Bertness, NA Sanford, LM Herz, MB Johnston. -
Theta oscillation-coupled dendritic spiking integrates inputs on a…
www3.eng.cam.ac.uk/~go223/Publications/huhn05.pdf8 Jun 2010: Neuron 40:177–188. Bernander O, Douglas RJ, Martin KA, Koch C. 1991. -
DEVELOPMENT AND APPLICATIONOF A PROGRAM FOR THE COMPUTER AIDED ...
www3.eng.cam.ac.uk/outreach/Project-resources/Senior-glider/Aery-technical-paper.pdf12 Oct 2011: a. c c Ka cK. K c a Kc. =. =. =. ... A session plan similar to 1995 was used for this full capacity , 24 student, session. -
PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...
www.tcm.phy.cam.ac.uk/~tmw38/Whitehead16a.pdf5 Apr 2016: 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. -
Theoretical Physics II
www.tcm.phy.cam.ac.uk/~rjs269/TP2/TP2y2024.pdf22 Jan 2024: 1.23)The evolution operator is. U(t) =. U1(t) 0 t < t1U2(t t1)U1(t1) t1 t < t2 (1.24)where Ui(t) = eiHi t/h̄ and Hi =. p22m. ... This is Feynman’spath integral. 24. 2.2 The propagator. The path integral is a tool for calculating the propagator -
Publications 1980 - 1989
www.tcm.phy.cam.ac.uk/~mw141/1980.html13 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 -
LagrangianDynamics Engineering Part IBPaper 1 Lectures 9-16 J. S. ...
www.tcm.phy.cam.ac.uk/~jsb56/resources/1B_Mechanics_handout.pdf24 Oct 2022: 23. 6.5 Second integral of the equation of motion. 24. 6.5.1 Second integral for the simple pendulum (non-examinable). -
PHYSICAL REVIEW A 82, 063625 (2010) Condensed ground states ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevA.82.063625.pdf30 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. -
PHYSICAL REVIEW A 93, 042702 (2016) Pseudopotential for the ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/Whitehead16.pdf24 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. -
PHYSICAL REVIEW A 96, 023619 (2017) Effective-range dependence of ...
www.tcm.phy.cam.ac.uk/~gjc29/papers/SchonenbergVerpoortConduit17.pdf24 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
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