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15 Jul 2023: 24/37. 𝐴 𝑚𝑁 modality,𝑚 < 𝑁 , 𝑆 = 𝑦𝑘 𝑘=1𝑅 samples. ... 24] Colbrook, Matthew J. "Computing semigroups with error control." SIAM Journal on Numerical Analysis 60.1 (2022): 396-422.

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

15 Jul 2023: Slide 23: Lorenz system: projection-valued spec meas. Slide 24: Nonlinear pendulum.

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.

18 Dec 2023: 1. INTRODUCTION. In the wake of the many AI-based algorithms throughout the society and the sciences, potentially yielding hal-lucinations and instabilities [4, 23, 23, 24, 31, 34, 38, 40,

1 Dec 2023: 1/4ε. 0. dζ|X ′1|. log ε1]ε0. 1. (3.12). For the sinusoidal waveform, J 1.24, and the predictions from (3.11) are included infigure 3(d).

9 May 2023: V. d3x0J(x0). |x x0|. – 24 –. If we subsequently take the curl of this equation, then we get an expression for the.

31 May 2023: qg = 2πn with n Z (1.24). This is the famous Dirac quantisation condition. ... qg = 2πn with n Z. This, of course, is the Dirac quantisation condition (1.24).

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].

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.