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17 protocols using chameleon ultra 2

1

Collagen Quantification in 3D Multiphoton Imaging

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As previously described [26] , 3D stacks of 425x425x60 μm were acquired using a 7MP multiphoton laser scanning microscope (Carl Zeiss, Jena, Germany), equipped with a 20x objective and coupled to a Tisapphire femtosecond laser, Chameleon Ultra 2 (Coherent Inc) tuned to 800 nm. Organized fibrillar collagens were detected by second harmonic generation at a wavelength of 400 nm.
The acquired 3D images and collagens quantification were analyzed off-line with Imaris software (Bitplane AG). Briefly the volume occupied by the collagen was calculated by measuring the volume occupied by the isosurface of the SHG in a cube of defined volume (80,1 x 80,1 x 80 µm). Three independent samples were used for each condition.
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2

Biphoton Microscopy of 3D Spheroids

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Cleared spheroids were maintained in a 1 mm-thick imaging chamber (CoverWell, ThermoFischer Scientific, Waltham, MA, USA) filled with ethylcinnamate between the slide and the cover-slide. The observation was made under a 7MP biphoton microscope (Laser Scanning Microscopy, Zeiss, Oberkochen, Germany) equipped with a ×20 immersion objective (NA 0.95) and coupled to a Ti-Sapphire femtosecond laser, Chameleon Ultra 2 (Coherent Inc., Santa Clara, CA, USA), tuned to 800 nm and 920 nm for the PI and GFP/Tomato signals, respectively. The GFP signal was detected through a 500–550 nm band pass filter, and the PI and Tomato signals through a 565–610 nm band pass filter with non-descanned detectors. The 3D stacks of spheroids (607 × 607 µm, variable z) were acquired at a resolution of 0.59 µm and with a z-sacking of 4 µm. The resulting 3D images were stored and analyzed off-line using Imaris software 9.3 (Bitplane AG, Schlieren, Switzerland) to show both transversal and side views of the spheroids.
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3

Multiphoton Microscopy of Fibrillar Collagen

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Stacks of 425x425x60 μm were acquired using a 7MP multiphoton microscope (Carl Zeiss, Jena, Germany) coupled to a Ti-Sapphire laser, Chameleon Ultra 2 (Coherent Inc) settled to 800 nm. Organized fibrillar collagens were detected by second harmonic generation at a wavelength of 400 nm. Imaris software (Bitplane AG) was used to analyzed the acquired 3D images.
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4

Visual Stimuli Calcium Imaging in Larval Zebrafish

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5 to 6 dpf ITNGal4, UAS:GCaMP3 larvae were individually mounted in 2% low-melting-point agarose in a 35 mm petri dish and the eyes and tail subsequently freed from the agarose with a scalpel. Visual stimuli consisted of small moving spots (subtending 5° visual angle) back-projected onto a curved screen in front of the animal, appeared at 76° to the left or right of the midline and then moving 152° right or left across the frontal region of visual field (at an average angular velocity with respect to the fish of 30°/s). At each imaging plane, 12–18 repetitions of each of the visual stimuli (L > R, R > L) were presented in pseudo-random order.
2-photon calcium imaging was simultaneously performed using a custom-built microscope equipped with a 20 × /1.00 NA Olympus objective and a Ti:Sapphire ultra-fast laser (Chameleon Ultra II, Coherent Inc) tuned to 920 nm. Average laser power at the sample was 5–10 mW. Images were acquired by frame scanning at 3.6 Hz with 1 µs dwell time per pixel. For each larva, 1–3 focal planes through the ITN nuclei of the larva were imaged. Image acquisition and visual stimulus presentation were controlled using software written in LabView and MATLAB.
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5

Redox-Sensitive Fluorescent Probe Imaging

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Mitochondrial and cytosolic oxidant stress was measured using the redox sensitive roGFP probe targeted to the cytosol or mitochondrial matrix (Graves et al., 2020 (link); Guzman et al., 2010 (link)). Slices were transferred to a recording chamber with normal aCSF at 32–34 °C continuously perfused. Measurement and analyses are consistent with prior studies (Graves et al., 2020 (link)). In brief, fluorescence was measured using an Ultima Laser Scanning Microscope system (Bruker) with an Olympus 60/0.9NA lens and PrairieView software. An excitation wavelength of 920 nm was applied using a two-photon laser (Chameleon Ultra II, Coherent Inc.) to excite roGFP. A t-series of roGFP fluorescence was obtained with 60 frames acquired over ~20 s with 0.195 μm × 0.195 μm pixels and 10–12 μsec dwell time. The probe was calibrated by obtaining the dynamic range; this was accomplished by acquiring additional t-series with bath perfusion of 2 mM dithiothreitol, a reducing agent, and 200 μM aldrithiol, an oxidizing agent, to determine the maximal and minimal fluorescence intensity as previously described (Graves et al., 2020 (link)). Test measurements were calculated as relative oxidation, data normalized to controls, and presented as % control.
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6

Fluorescence Lifetime of iLOV-mBeRFP Complex

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The fluorescence lifetime of iLOV in the absence and presence of mBeRFP moiety was measured using a home-built fluorescence lifetime setup (Harp300, Picoquant) coupled with the time-correlated single-photon counting (TCSPC) module (time resolution < 4 ps) and a broadband tunable pulse femtosecond Ti:Sappihire laser (Chameleon Ultra II, Coherent Inc.). The 457 nm femtosecond excitation source was obtained from the secondary harmonic generation with BBO nonlinear crystal to excite the iLOV protein, and the repetition rate was regulated down to 40 MHz with a pulse selection system (Conoptics, model 305). The emission passed through a band-pass filter (ET540/30m, Chroma) and was detected by a micro photodevice (Picoquant) with the time resolution of less than 40 ps. The emission lifetime was determined by fitting the emission trajectory with single exponential decay function.
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7

FLIM-FRET Microscopy for RhoA Activation

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FLIM-FRET data was acquired as described previously [26 (link),50 ] using an inverted Leica DMI 6000 SP8 confocal microscope (Leica Camera AG) with a 25 × 0.95 NA water immersion objective. A Titanium:Sapphire femtosecond laser (Chameleon Ultra II, Coherent Inc.), operating at 80 MHz, was used as an excitation source at 890 nm. The EGFP signal was recorded with RLD HyD detectors (Leica Camera AG) using a 525/50 nm emission filter (Chroma Technology Corp.). FLIM data was acquired using a Picoharp 300 TCSPC FLIM system (PicoQuant). For each sample, 5 representative regions of interest were imaged at a pixel depth of 512 × 512.
FLIM data was analyzed as described previously [53 (link),54 (link)], using FLIMfit (5.0.3), recording average single cell lifetimes of the EGFP donor. Cells were further grouped into RHOA “active” and “inactive” by the presence or absence of regions of high FRET within the cell membrane.
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8

Two-Photon Microscopy for Neuroimaging in Mice

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Mice were imaged using customized two-photon microscopy (2P PLUS, Bruker Corporation) coupled with a femtosecond mode-locked Ti: Sapphire laser (80 MHz, 140 fs, Chameleon Ultra II, Coherent Inc.) with 920 nm (for GCaMP6s only) or 965 nm (for GCaMP6s and jRGECO1a). A Pockels Cell (EO-PC, Thorlabs Corporation) was used to regulate laser power. For neuron imaging, power after the 4× objective (N4X-PF, 0.13 NA, Nikon) and 16× objective (N16XLWD-PF, 0.8 NA, Nikon) was limited to a maximum of 40 mW, dependent on depth. Emission light was filtered using a bandpass 525/70 filter for GCaMP6s and a bandpass 595/50 filter for jRGECO1a, detected by two GaAsP PMTs (model H10770, Hamamatsu Photonics). Images were collected at 30  Hz using a resonant-galvo scanner with 512×512  pixel resolution for functional imaging. Images were collected using a galvo-galvo scanner with 1024×1024  pixel resolution for structure imaging. For two-photon imaging in anesthetized experiments, isoflurane (0.6%, mixed with fresh air, 0.5  L/min ) was used to anesthetize mice during imaging. For two-photon imaging in awake experiments, 3 days of routine handling of the mice to acclimate them to the imaging system and immobilization device, which greatly helped to reduce animal motion.
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9

Fluorescence Lifetime Measurement Protocol

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The fluorescence lifetimes were recorded by time-correlated single-photon-counting (TCSPC) measurement using a home-built fluorescence lifetime setup (Harp300, Picoquant, Berlin, Germany). The excitation light source was a broadband tunable pulse femtosecond Ti:sapphire laser (Chameleon Ultra II, Coherent Inc., Santa Clara, CA, USA) equipped with a pulse-selection system (Model 305, Conoptics, Danbury, CT, USA) to modulate the repetition rate. A pulsed excitation laser of 450 nm was generated from the second harmonic generation with a BBO nonlinear crystal. Two long-pass filters (AT470lp, Chroma, Bellows Falls, VT, USA) were utilized to filter out the excitation light. Sample fluorescence was collected by a single-photon-counting avalanche photo diode detector (MPD, Picoquant, Berlin, Germany) and delivered into the TCSPC system for analysis. The typical full width at half-maximum (FWHM) of the system response was 0.15 ns. The recorded data were plotted as a fluorescence lifetime histogram, and the dynamic parameters were obtained from single or double exponential fitting.
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10

Two-Photon Microscopy of NADH in Cells

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After treatment, cells cultured in 35 mm dishes were observed using a two-photon microscope (LSM 710, Carl Zeiss, Jena, Germany) equipped with a Chameleon Ultra II pulsed infrared laser (Coherent Inc., Santa Clara CA, USA), and a W-Apochromat 63x/1.0 NA objective was used. NADH was excited at 730 nm and detected at 460 nm. The maximum projection of each image was obtained from a 5 μm-thick z-stack and analyzed with the CellProfiler program. Cells were delineated, and NADH fluorescent signal per cell was measured.
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