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8 Mar 2021: 24] B. Adcock and A. C. Hansen, “Generalized sampling and infinite-dimensional compressed sensing,” Foundations of Computational Math-ematics, vol.

16 Feb 2021: fundamental problems of S.Smale on existence of algorithms [24, 25, 100–102] and work by C.

18 May 2021: 24 CHAPTER 2. GENERALISED SOLUTIONS. The representation (2.8) makes it clear again that the Moore-Penrose inverse is un-bounded if R(A) is infinite dimensional.

8 Oct 2021: and absolutely impossible for me to do so in a course of 24 lectures).

8 Oct 2021: hx| i =Z. R (x0) hx|x0i dx0 = (x). (2.24). In other words, the position space wavefunctions we’re familiar with are nothing but the.

15 Apr 2021: Notice that by the Friedmann equation. 3M2PlH2 = Λ (24). A metric with this property is called conformally flat.

15 Apr 2021: M2Plä. a= 1. 6(ρ 3p). (1.24). Second, by taking the time derivative of the Friedmann equation and using the continuityequation to get rid of ρ̇, we can find the ... ̇K = ä2K. ȧ3ä (ρ 3p) (1 3w) , (1.27). where in the second step I used the

16 Apr 2021: D : (3 ττ ) kiki , (4.24)b K : (3 ττ ) 2biki b kkiki 2kikibjkj. ... R|comoving R =A. 2. (5.24). The metric then takes the form.

20 Apr 2021: The quantities we are interested in are vortices. 24. 2 Vortices III Classical and Quantum Solitons.

6 Oct 2021: 1923-24: de Broglie proposes wave-particle duality for matter, as for radiation. •