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11 Oct 2020: XFlux @100 kHz. 3.0 kA/m. 248. mT. High Flux @100 kHz. ... Kool Mµ @100 kHz. 3.0 kA/m. 248. mT. Nanocrystalline @100 kHz.

21 Oct 2020: z O(z 2);. TR: yn =[(. I 12 kA)1 (. I 12 kA)]n. ... 24 / 28. Splitting of inhomogeneous systems. Recall our goal, namely fast methods for the two-dimensionaldiffusion equation.

16 May 2020: those satisfying Eqn. (3.11). 24. 3.3 The 1D Schrödinger equation for a particle in a potential.

3 Jan 2020: those satisfying Eqn. (3.11). 24. 3.3 The 1D Schrödinger equation for a particle in a potential.

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.

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

13 Jan 2020: Termination I - 14 ka. Termination IV - 337 ka. Termination V - 424 ka 11. ... 9e. 7e7a. 19. 15a. 103. 63. 9a. 5. 15e. 4. Termination VI - 533 ka.

10 Nov 2020: C A M B R I D G E U N I V E R S I T Y. REPORTERS p e c i a l N o 2 F r i d ay 6 N o v e m b e r 2 0 2 0 Vol c l i. P U B L I S H E D B Y A U T H O R I T Y. R O L L O F T H E R E G E N T H O U S E A N D L I S T O F M E M B E R S O F T H E FA C U LT I

1 Oct 2020: C A M B R I D G E U N I V E R S I T Y. REPORTERS p e c i a l N o 1 T h u r s d ay 1 O c t o b e r 2 0 2 0 Vol c l i. P U B L I S H E D B Y A U T H O R I T Y. N o t i c e s. Deputy Vice-Chancellors appointed 3Syndicates, Committees and other bodies: