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16 protocols using xlumplfln20xw

1

In Vivo Nanoimaging of Cardiomyocytes

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The details of the microscopic system for in vivo nanoimaging have been described in our previous studies [5 (link), 6 (link)]. In brief, an upright microscope (BX-51WI, Olympus Co., Tokyo, Japan) combined with a Nipkow confocal scanner (CSU21, Yokogawa Electric Co., Tokyo, Japan) and an electron multiplying CCD (EMCCD) camera (iXonEM+, Andor Technology Ltd, Belfast, Northern Ireland) were used at a 512 × 512 (or 512 × 170) pixel resolution at an exposure time of 28 (or 9.8) ms. A water immersion lens, either 60× (LUMPLFLN 60XW, N/A 1.00, Olympus Co.), 40× (LUMPLFLN 40XW, N/A 0.80, Olympus Co.), or 20× (XLUMPLFLN 20XW, N/A 1.00, Olympus Co.), and also a 2× lens (XLFluor 2X/340, N/A 0.14, Olympus Co.) were used to visualize the LV surface.
AcGFP-expressing myocytes were excited by a 488 nm laser light (HPU50211-PFS, Furukawa Electric Co., Tokyo, Japan), and the resultant fluorescence signals (emission filter: BA510–550, Olympus Co., Tokyo, Japan) were detected. In the experiments with CellMask, the heart was excited at 532 nm (MiniGreen FCIM-100; Snake Creek Lasers, Friendsville, PA, USA), and the resultant fluorescence signals (emission filter: BA575IF, Olympus Co.) were detected. When excited at 532 nm, the wavelength range for the detection of the fluorescence of CellMask was >575 nm.
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2

Multimodal Optical Imaging of Organ Tissues

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One mTmG mouse was used in Fig. 2a, b. About 200-μm tissue slices of the liver and 300-μm tissue slices of the kidney were optically cleared by CUBIC50 (link). The liver slices were imaged using a custom-built time-delay integration-based line-scanning microscope6 (link) that has the characteristics of wide-field imaging and enhanced signal-to-noise ratio (Fig. 2a). A 20× /1.0-NA water-immersion objective (XLUMPLFLN 20XW, Olympus) was used for acquisition and the voxel size was 0.32 × 0.32 × 1 μm3. The kidney slices were imaged using a Nikon Ni-E A1 multiphoton laser-scanning microscope with a 60× /1.2-NA water-immersion objective (Nikon) using 920-nm two-photon excitation and a voxel size of 0.21 × 0.21 × 1 μm3 (Fig. 2b). The whole-brain vasculature datasets used in Fig. 2c were provided by Todorov et al.28 (link), where the 3DISCO51 (link) cleared brains were acquired with LaVision light-sheet microscopes at a 1.63 × 1.63 × 3 μm3 voxel resolution. One Thy1-GFP M-line mouse was used in Fig. 2d. The mouse brain was sectioned into 300 μm tissue slices. The sections were optically cleared by CUBIC and then imaged using the Nikon Ni-E A1 microscope working in the confocal mode. The imaging setup was the same as the two-photon imaging of the kidney.
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3

Two-Photon Imaging of Live Embryos

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Two-photon imaging of live embryos and larvae was performed at RT on a custom-built microscope controlled by ScanImage (Pologruto et al., 2003 (link)). Excitation was provided by a Chameleon-XR Ti:Sapphire laser (Coherent) tuned to 890 nm. Fluorescence was detected using a Multiphoton Detection Unit mounted on a SliceScope (Scientifica). We used water immersion objectives from Olympus, either 60×/NA1.0 (LUMPLFLN60X/W) or 20×/NA1.0 (XLUMPLFLN20XW). For imaging, larvae were embedded in 1% low melting point agarose, covered with embryo medium (5 mM NaCl, 0.17 mM KCl, 0.33 mM CaCl2, and 0.33 mM MgCl2), and imaged at RT.
For the imaging of transgenic/mutant larvae, TgBAC/pcdh19+/− fish were crossed and embryos were kept in individual wells of a 24-well plate. After imaging, fish were genotyped by HRMA to identify homozygous mutants. As homozygous mutants are viable and fertile, some of the experiments were performed on incrossed TgBAC/pcdh19−/− adults.
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4

Visualizing Myenteric Ganglia Fluorescence

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Myenteric ganglia were visualized through a 20× wide-field water-immersion objective lens (Olympus XLUMPLFLN20xW, 1.0 numerical aperture) on an upright Olympus BX51WI fixed-stage microscope (Center Valley). Ganglia were identified based on their plexiform appearance and high expression of the fluorescent tdTomato reporter in resident glial cells. Illumination for fluorescence imaging was supplied by a DG4 Xenon light source (Sutter Instrument) (SI Appendix, Materials & Methods).
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5

In Vivo Calcium Imaging of Mouse Neuronal Activity

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After habituation and training, mice were used for Ca2+ imaging. Multiphoton fluorescence microscope (Femtonics, Budapest, Hungary) with a 16× NA 0.8 water-immersion objective (CFI75 LWD 16X W, Nikon, Tokyo, Japan) or with a 20× NA 0.8 water-immersion objective (XLUMPLFLN20XW, Olympus, Tokyo, Japan) was used for Ca2+ imaging in vivo. Ti:Sapphire laser (Chameleon Ultra, Coherent, USA) with an excitation wavelength of 920 nm was used to excite the fluorescence of GCaMP6f. Fluorescence signal from a brain area of 600 × 600 or 175 × 175 µm2 (512 × 512 pixels) was recorded in resonant scanning mode at 30 frames/s. The signal was filtered with a 520/60 nm bandpass filter (Semrock, Rochester, NY, USA) and then detected with a GaAsP photomultiplier (H11706P-40, Hamamatsu, Japan). Simultaneously, autofluorescence was filtered with a 650/100 nm bandpass filter and detected with a second identical photomultiplier. Several imaging sessions of 10 min were carried out for each mouse. In parallel with Ca2+ imaging, the animal movements on the platform were monitored with locomotion-tracking software (Neurotar, Helsinki, Finland). All sessions were video recorded in infrared light. The experimental session did not exceed 2 h per mouse.
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6

Two-Photon Calcium Imaging of rd1-Thy1-GCaMP6s Retina

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Two-photon calcium imaging of rd1-Thy1-GCaMP6s retina was carried out on a custom galvo-scanning microscope equipped with a 20×1.0 NA water immersion objective (XLUMPLFLN20XW, Olympus). Excitation at 920 nm was provided by a tunable Ti:Sapphire ultrafast laser (Chameleon Ultra, Coherent). Imaging parameters were controlled by ScanImage 3.8.1 software (http://scanimage.vidriotechnologies.com/): 256×256 pixels at 1.25 Hz (2ms per line). GCaMP6s emission was collected with a GaAsP PMT shielded by a longpass filter (ET500lp, Chroma).
Isolated retinas were cut into four-leaf clovers and transferred onto filter paper (0.45 mm nitrocellulose membranes, MF-Millipore) with the ganglion cell layer facing up. Oxygenated ACSF was then perfused over the retina at 34 °C for 30 minutes with a flowrate of 1 mL/min. An initial imaging session performed to account for potential two-photon sensitivity. Experimental imaging was performed with the laser power at the sample ≤5 mW. For pharmacological blockade of actional potentials, Lidocaine (2% in saline) was applied to the bath during corresponding recordings. Washout of Lidocaine was performed by continuously perfusing oxygenated ACSF at 34 °C over the course of two hours with a flowrate of 1 mL/min.
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7

Two-Photon Excited Fluorescence Imaging In Vivo

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High-resolution two-photon excited fluorescence (TPEF) in vivo imaging was performed on a Prairie Ultima Multiphoton microscope equipped with a mode-locked Ti:sapphire laser (Chameleon Ultra II, Coherent, Santa Clara, California). Laser excitation was set at 910 nm for EGFP detection and a maximum power of 35  mW was used for data acquisition. Images were acquired with a water immersion lens (XLUMPLFLN20XW, Olympus, Tokyo, Japan; 20× magnification, NA=1 ) at 1024×1024  pixel resolution and zoom = 1, leading to 600  μm field of view with linear resolution of 0.594  μm/pixel .
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8

Whole-Heart Imaging of Vascular and Myocardial Architecture

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To obtain vascular and myocardial information on the mouse heart, the sample was placed on the HD-dfMOST system for sectioning and imaging. The whole sample was immersed in a water sink containing PI solution for real-time staining of the myocardial architecture. Whole-heart imaging was performed in a water bath. In our experiment, the sample was imaged at a voxel resolution of 0.32 × 0.32 × 1.0 μm3. The heart sample colabeled with myocardial architecture and blood vessels was imaged through two channels (GFP and PI, respectively).
The following devices were used in the HD-dfMOST system (Figure 1B): lasers (488 and 561 nm, Cobolt, Sweden), lenses (L1, AC050-008-A-ML, f 7.5 mm; L2, AC254-250-A, f 250 mm; L3, TL, AC254-125-A-ML, f 125 mm, Thorlabs, USA), a cylindrical lens (ACY254-100-A, f 100 mm, Thorlabs, USA), an objective lens (XLUMPLFLN 20XW, 1.0 NA, Olympus, Japan), dichroic mirrors (ZT488/561rpc Chroma USA), excitation filters (ZET488/561 m, Chroma, USA), sCOMS cameras (ORCA-flash4.0 V3, Hamamatsu, Japan), and an XYZ linear stage (x-axis XML210, y-axis XMS100, z-axis GTS30V, Newport, USA).
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9

Two-Photon Microscopy for Volumetric Imaging

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We used a galvo-galvo-resonant two-photon microscope (Thorlabs Bergamo II, Vidrio RMR Scanner) with a fast piezoelectric objective scanner (Physik Instrumente P725) and a 20×/1.0 NA objective (XLUMPLFLN20XW, Olympus) for volumetric imaging. We used a Chameleon Vision-S Ti-Sapphire femtosecond laser tuned to 940 nm for two-photon GCaMP excitation. Emission was collected on GaAsP PMT detectors (Hamamatsu) through a 525-nm bandpass filter (Thorlabs). We used ScanImage 2018 software51 (Vidrio Technologies) to control the microscope, and imaging data were collected in ScanImage using National Instruments PXIe-6341 hardware.
The imaging region for all experiments was 256×128 pixels, with 12 slices in the z-axis for each volume (3–5 μm per slice) resulting in a ~10 Hz volumetric scanning rate. For EPG, PFNd, PFNv, SpsP, and IbSpsP imaging experiments, we imaged the PB. For LNO2 and LNO1 imaging experiments, we imaged the NO. For hΔB imaging experiments, we imaged the FB.
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10

Two-Photon Imaging of GCaMP6s Fluorescence

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Imaging was performed on a custom two-photon microscope controlled using ScanImage 3.8 (45 (link)). A Ti-Sapphire laser (Chameleon Ultra II, Coherent) tuned to 920 nm was used to excite GCaMP6s. The laser was focussed at the sample using a 20× 1.0–numerical aperture (NA) objective lens (XLUMPLFLN20XW, Olympus), downstream of 50- and 300-mm focal length scan and tube lenses (AC-300-050B and AC-508-300-B, Thorlabs). Scanning was achieved using 3-mm aperture scan mirrors (6215H, Cambridge Technology). Fluorescence emission from GCaMP was band-pass–filtered (FF01-520/70, Semrock) and detected with a GaAsP PMT (H7422PA-40, Hamamatsu). Output from the PMT was amplified using a preamplifier (SR570, Stanford Research Systems) and acquired using the same data acquisition card used to drive the scan mirrors (PCI-6110, National Instruments). Data acquisition from the microscope was triggered by a TTL pulse generated at the beginning of each trial by an Arduino connected to a separate computer running the behavior protocol. A continuous time series of two-photon images was acquired for every trial of the experimental protocol. Multitrial protocols had an ITI of 30 s. Imaging was discontinued for 24 s of the 30-s interval.
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