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21 Jan 2023: This wasthe most challenging aspect of the experimental procedure. Tosummarize, the total number of high-speed movies acquiredwas nmov[hs] = 24. ... b) and (d) showboxplots of peak values () and beat-average quantities (〈〉) computedfrom n = 48

14 Feb 2023: KaðzÞffiffiffiffiffip2z. rez 1þ4a. 2 18z. þð4a2 1Þð4a2 9Þ. 128z2. ; (24).

26 Jan 2023: x, y) = n,k(x mE/eB2, y) (1.24). and the energies are now given by. ... 24 –. which obey @z = @̄z̄ = 1 and @z̄ = @̄z = 0.

1 Dec 2023: Received 24 February 2017; revised 22 May 2017; accepted 10 July 2017;first published online 30 August 2017).

20 Nov 2023: Brown [27–29]) and Toeplitztheory (see A. Böttcher & B. Silberman [24–26]).

14 Jan 2023: 2e20. Zddx. (4.24). The factor of N in front of the first term is what gives us hope because, in the limit. ... Specifically, we send N! 1,. keeping e20N fixed. The path integral (4.24) is then dominated by the minimum.

1 Dec 2023: u = 0. (2.1). In place of the Navier–Stokes equations for an unconfined fluid, in a porous medium the Darcyvelocity u is governed by Darcy’s Law [23,24], which

16 Jun 2023: Therefore, its spectral information can be far more complicatedand more difficult to compute than that of a finite matrix [91, 20, 5, 24, 22].

29 Dec 2023: Z(1.24). If we make a measurement described by an operator Ô, then the probability that wefind ourselves in the eigenstate |ϕ⟩ is given by.

27 Dec 2023: Supersymmetric Field Theory. University of Cambridge Part III Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical Sciences,. Wilberforce Road,. Cambridge, CB3 OBA, UK.