Search

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

23 Feb 2024: Teslovich TM, Thorleifsson G, Van den Herik EG, Voight BF, Volcik KA, Waite LL, Wong A, Wu Y, Zhang W, Absher D, Asiki G, Barroso I, Been LF, Bolton JL, Bonnycastle

29 Dec 2023: Preprint typeset in JHEP style - HYPER VERSION. Statistical PhysicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,.

20 Mar 2024: Dunajski, M. and Ka'zmierczak, M. (2007) Moduli spaces with external fields', hep-th/0610220.

23 Oct 2023: Indeed, withk = t, we have:. Euler: un1 = (I kA)un, ez = 1 z O(z2);Implicit Euler: un1 = (I kA)1un, ez = (1 z)1 O(z2);.

15 Jan 2024: Show that the phase shifts δl obey. tanδl =jl(ka). nl(ka). 4. ... Show that the phase shifts obey. tanδl =q jl(ka)j. ′l(qa) k j.

4 Jan 2024: Ex = ωA sin(nπy. a. ). sin(kz ωt). and. By = kA sin(nπy.

1 Dec 2023: T R A N S P O R T P H E N O M E N A A N D F L U I D M E C H A N I C S. On two-phase modeling of dewatering pulp suspensions. Daniel T. Paterson1 | Tom S. Eaves2 | Duncan R. Hewitt3 | Neil J. Balmforth4 |. D. Mark Martinez1. 1Department of Chemical

1 Dec 2023: J. Fluid Mech. (2013), vol. 737, pp. 205–231. c Cambridge University Press 2013 205doi:10.1017/jfm.2013.559. Stability of columnar convection in a porousmedium. Duncan R. Hewitt1,†, Jerome A. Neufeld1,2,3 and John R. Lister1. 1Institute of

18 Mar 2024: Home page Indexes: The Girton Poetry Group. Not Averse. So much happens that we miss or forget,. waking from dreams of the house in my head,. that old haunt still knocking about breaking. things scratching walls hiding under bedsheets,. buoyed by