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. Author manuscript; available in PMC: 2022 Aug 17.
Published in final edited form as: Nat Protoc. 2020 Dec 14;16(1):532–560. doi: 10.1038/s41596-020-00440-x

Fig. 1 |. A schematic of excitation optical paths for both vertical and inclined illumination.

Fig. 1 |

a, Schematic of the microscope setup for both the inclined and the vertical illumination in SPEED microscopy. A 488-nm (blue) and a 568-nm (green) laser are directed into the objective in vertical illumination or offset so that the lasers pass through the focal plane at an angle of θ3. The inset depicts a diagram of the edge excitation optics. The refractive angle (θi) at the interface of two different mediums with different refractive indexes (ni). The θ3 depends on the focal length of the objective (a), the refractive indexes of the different mediums in the optical path and the distance (d) between the center and edge excitation beams. The relationship between θ3 and d follows the equation: d=a*tan[sin1(ncellnoilsinθ3)], where a = 300 μm, ncell = 1.33 and noil = 1.516. For example, to obtain θ3 = 45°, d needs to be 237 μm. b, An illustration of a molecule traveling in three dimensions as it passes through an NPC. A 2D projection of the same pathway is depicted in the lower panel. c, An illustration of the effect of the optical chopper on laser intensity. The chopper is calibrated to be open for 1/10 of frames captured.