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16 Jun 2015: ApJ, 270, 342 (1983). 24. Mackay, C.D. and Astill, D.M., CCD Development at Cambridge, England'. ... 31. Mackay, C.D., CCDs in Astronomy'. Ann. Rev. Ast. And Astrophys., 24, 255, 1986.

21 Apr 2015: Next fEC/IAP seminars are 12 February & 24 March 2015, 9.30-11am in 16 Mill Lane.

5 Feb 2015: B Q) Q = 2(QB B) (4.24). 11. for any bivector B. ... eiSn eiRn , (5.24)eiSn Rnei , (5.25). 18. and the latter combines with Eq.

28 Oct 2015: University Offices (Legal Services). Ms Julia Stacey Durham, M.A., TH, C.P.E., London, LL.M., Nottingham, appointed from 24 September 2015 until the retiring age and subject to a

22 Oct 2015: 131. University Finance (a) Planning and Resources. The minutes of the meeting of the Planning and Resources Committee held on 24 June 2015 were received.

8 Nov 2015: RTkz RTz‖2 ‖R(Tkz) R(Tz)‖2 p(Tk z,T z)2. 8δ̂(Tk z,T z)2. 24(1 |z|2)2δ̂(Tk,T)2. ... ζ(z)2 ζ̃2k(z)| C. 24(1 |z|2)δ̂(Tk,T). (5.4). If z σ(T) then at least one of ‖R(Tz)‖ and ‖R(Tz)‖ is equal

16 Jun 2015: 0.0206, 0.15. available. NIRSPEC. 10m Keck II. 0.95-5.5. 2500 25000. 12 24. ... grisms or FP. R50 J 25.8 H 25.1 K 24.6. R500 J 24 H 23.5 K 22.6.

3 Apr 2015: Numerical stability in the presence of variable. coefficients. Ernst Hairer. Section de mathématiquesUniversité de Genève. Email: Ernst.Hairer@unige.ch. Arieh Iserles. Department of Applied Mathematics and Theoretical PhysicsCentre for

19 Feb 2015: performs time-ensemble computation, in much the sameway NMR quantum computation performs molecular-ensemble computations.24,25,26 Time-ensemble computa-tion alleviates the demand for single-shot spin measure-ments ... ψ(y,t) = exp[. f1(t) y2 f2(t) y f3(t

19 Feb 2015: 22 E =. d. 2ισ12 ισ. 22 E. (24). It follows that the propagator in the transformed basis can be constructed as. ... 24). Clearlythe observable which measures the amount of a state in any one eigenspinoris a constant of the motion, and more generally,