All experiments, unless otherwise stated, were conducted in replicates of at least N = 2 6 (with specific N values are denoted for each experiment) and were repeated at a separate time, also in replicates of N = 2 6.
Let us firstly denote, for each n ∈ N, r n = d ( x n, B 0 ).
We also denote, for each i ∈ I, Meas ( Ω i, S i ) the set of measurable mappings from ( Ω i, Z i ) to S i.
The image resolution is denoted for each condition and corresponds to the lattice fringes with the highest spatial frequency (as indicted by a dashed circle).
The image resolution is denoted for each display and corresponds to the highest spatial frequency lattice fringes (indicated by a dashed circle).
If we let (widehat{h}^{nabla}_{n} (t,s)) denote for each fixed (sin mathbb {T}) the derivatives of (widehat {h}^{nabla}_{n} (t,s)) with respect to t, then widehat{h}^{nabla}_{n} (t, s)=widehat{h}_{n-1} (t, s) quadmbox{for } nin mathbb {N}, tin mathbb {T}_{kappa}.
The image resolution is denoted for each illumination condition and corresponds (as indicated by a dashed circle) to the lattice fringe with the highest spatial frequency, except at the highest total dose-rate at which the resolution represents an estimate from the onset of the sudden drop in intensity in the FFTs.
Suppose that (bar {h} x,y,z,k):mathbb{R}^{n}timesmathbb{R}^{n}timesmathbb{R}^{n}times mathbb{R}^{n}mapstomathbb{R}) is a (mathcal{C}^{1}) real function, and denote for each (lambdainmathbb{R}) h^{lambda} x,y,z,k)=h x,y,z,k)+lambdabar{h} x,y,z,k).
