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31 May 2023: Preprint typeset in JHEP style - HYPER VERSION Lent Term, 2017. Applications of Quantum MechanicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical

23 Sep 2015: along the anterior (kA = 1000 μm, hA0 = 0:8) and strongly along the posterior-lateral cortex (kP = 150 μm, hP0 = 0, see ‘Materials and methods’ MT nucleation. ... the inset of panel C (yellow circles). In all panels, parameter values for anterior

19 Oct 2013: Another importantwave activity measure is given by the pseudomomentum vector,. p = kA =h′ u′. ... Because of the ray-invariance of absolute frequency we have that |kA| = |kB | asympto-tically.

19 Jun 2024: Electron excitation of Be-like Fe XXIII for the n=2,3,4 configurations. MC Chidichimo, G Del Zanna, HE Mason, NR Badnell, JA Tully, KA Berrington. –

19 Jun 2024: R Hložek, AI Malz, KA Ponder, M Dai, G Narayan, EEO Ishida, TA AllamJr, A Bahmanyar, X Bi, R Biswas, K Boone, S Chen, N Du, A Erdem, L Galbany, A

7 Apr 2021: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... v(k) =Ca. sin(ka) = Ca. sineEa. t. The Bloch frequency is! =

1 Sep 2011: On Lp-boundedness of the L2-projectoronto nite element spacesA. Yu. Shadrin1. IntroductionIn [Sh] we proved that, for p suciently close to 2, the Lp-norm of the L2-projector P onto the space S of polynomial splines of order k on a knot-sequence is

1 Sep 2011: TO KA-SAETSQ PORQDKA POLIGARMONINOSTI (g) = @(f)=@xj, TO, POSKOLXKU OPERACIQ DIFFERENCIRO-WANIQ SOHRANQET TOT PORQDOK, IMEEMr2(g) = 0; = m1 1 2m1 = m:pREDLOVENIE 1a0, A S NIM I SLUAJ 1a)

19 Jun 2024: XC Vidal, M D'Onofrio, PJ Fox, R Torre, KA Ulmer, A Aboubrahim, A Albert, J Alimena, BC Allanach, C Alpigiani, M Altakach, S Amoroso, JK Anders, JY Araz, A Arbey,

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