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Getting Past No Pdf

Negotiating in Difficult Situations Getting Past No Getting Past No Negotiating In Difficult Situations. the SRI state (in light orange). The star-shaped sample was positioned at the focus plane of an AR-PREM2B microscope. (**b**) Two-photon fluorescence microscope image of a single *φ*-shaped particle. (**c**) Autocorrelation of the fluorescence intensity time traces measured from a single particle and the corresponding best fit (in black). (**d**) Phase-contrast image of the particle autocorrelation.](ncomms9366-f2){#f2} ![Numerical simulation of PC-SPC-SRI diffraction.\ (**a**) Schematic representation of the experiment. (**b**) Simulated intensity pattern for the PC-SPC-SRI diffraction experiment. The amplitude (top row) and the phase (bottom row) of the intensity pattern are represented in a columnar format with dark red and green representing high intensity and gray representing low intensity. The PC-SPC-SRI module is represented in the background as a red box. The lens phase in the PC-SPC-SRI module is represented in white and the amplitude in grey. (**c**) Simulated intensity pattern for the 100 × 100-nm^2^ spot indicated in **b**. The amplitude (top row) and the phase (bottom row) of the intensity pattern are represented in a columnar format with dark red and green representing high intensity and gray representing low intensity. (**d**) Simulated intensity pattern for the 200 × 200-nm^2^ spot indicated in **b**. The amplitude (top row) and the phase (bottom row) of the intensity pattern are represented in a columnar format with dark red and green representing high intensity and gray representing low intensity. The PC-SPC-SRI module is represented in the background as a red box.](ncomms9366-f3){#f3} ![Diffraction resolution analysis and SRI focusing.\ (**a**) Observed lateral diffraction resolution for a 300-nm thick 1,200-nm wide slit for incident X-ray energy of 10.6 keV and two SRI configurations: full diffraction pattern (black), single-mode SRI (red) and PC

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