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20 protocols using xlplan n

1

Stimulated Raman Scattering Microscopy Setup

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We used an inverted laser-scanning microscope (FV1200 MPE, Olympus) optimized for near-infrared (near-IR) throughput and a 25× water objective (XLPlan N, 1.05 N.A., MP, Olympus) with high near-IR transmission for SRS microscopic imaging. A picoEMERALD system (Applied Physics & Electronics) supplied synchronized pulse pump beam (with tunable 720–990 nm wavelength, 5–6 ps pulse width, and 80-MHz repetition rate) and Stokes (with fixed wavelength at 1064 nm, 6 ps pulse width, and 80 MHz repetition rate). Stokes was modulated at 8 MHz by an electronic optic modulator. Transmission of the forward-going pump and Stokes beams after passing through the samples was collected by a high N.A. oil condenser (N.A. = 1.4). A high O.D. bandpass filter (890/220, Chroma) was used to block the Stokes beam completely and to transmit the pump beam only onto a large area Si photodiode for the detection of the stimulated Raman loss signal. The output current from the photodiode was terminated, filtered, and demodulated by a lock-in amplifier at 8 MHz to ensure shot-noise-limited detection sensitivity. The demodulated signal was fed into analog channel of the FV1200 software FluoView 4.1a (Olympus) to form image during laser scanning.
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2

Visualizing Cell-Seeded Scaffolds with Multiphoton Microscopy and SEM

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Cell seeded scaffolds were visualized using a custom-built multiphoton microscope previously reported [39 (link)]. Coherent anti-stokes Raman scattering (CARS) imaging at 2911 cm-1 was used to image the PCL scaffold fibres, whilst simultaneously exciting two photon fluorescence (TPEF) from Phalloidin and DAPI stained cells. All images were acquired using a 25x/1.05 N. A water immersion lens (XLPlanN, Olympus), providing a maximum field of view of 509 μm on the sample. To measure infiltration of cells into the scaffold Z-stacks were acquired with 1 μm steps.
Cell seeded scaffolds were also visualized using SEM using a previously described osmium based method [40 (link)]. These osmium stained scaffolds were visualized using a Hitachi TM4000 tabletop SEM (Hitachi) with a 15 kV accelerating voltage and a 10mm working distance. These scaffolds were sputter coated with an Elmscope FLM-007 using gold.
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3

Intravital Imaging of Murine Liver

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Mice were anaesthetized via i.p. injection of Avertin (240 mg/kg). The antibodies and fluorescent dyes were injected via tail vein. Surgical preparation for liver intravital imaging was performed as previously described32 (link).The liver was observed by two-photon microscopy (FVMPE-RS, OLYMPUS) equipped with two infrared lasers (MAITAI HPDS-OL: 690 nm–1040 nm; INSIGHT X3-OL: 690 nm−1300 nm). The MAITAI laser was tuned to 940 nm for excitation of FITC or Dendra2. INSIGHT laser excitation was tuned to 1200 nm for simultaneous excitation of PE, eF 660 or DiD. Emitted light was detected using a 25 × 1.05 NA water lens (XLPlan N, OLYMPUS) coupled to a 4-color detector array. The operating room temperature was normally kept between 20 °C and 24 °C.
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4

Multiphoton Imaging of Biological Samples

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Imaging was performed with an Ultima system (Prairie Technologies). Excitation at 950 nm from a mode-locked laser was raster scanned at 5–12 Hz with emission collected in red (607/45 nm) and green (525/70 nm) channels. 40× 0.8 NA objective (Olympus) used. As noted, 25× objective (Olympus XLPlan N) was used in some instances to afford a larger field of view.
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5

Fluorescence Lifetime Imaging and Confocal Microscopy

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FLIM was done as described previously (McCullock et al., 2020 (link)). Cells were transfected in either 35 or 60 mm culture dishes and imaged using a water immersion 25× objective (XL Plan N, 1.05 NA) mounted on an Olympus IX61WI upright microscope. A Mai Tai Ti:Sapphire multi-photon laser (Spectra Physics) was used for excitation with an 860 nm wavelength, a repetition rate of 80 MHz and pulse width of approximately 100 fs. Donor emission was filtered by a 480–20 filter and measured by a H72422P Hamamatsu hybrid avalanche photodiode. Time-correlated single photon counting was done using a Becker and Hickl card with a resolution of 25 ps. Using VistaVision software (ISS), donor fluorescence from the plasma membrane from individual cells was binned and fit with a single exponential function, consistent with the lifetime of CFP variant mTurquoise2 (Goedhart et al., 2012 (link)).
For confocal imaging, cells were transfected with Lck-CFP or CFP-tagged cASIC1 in 35 mm dishes. After 2 days, cells were stained with 2 mL of 7.5 µM FM1–43 (Invitrogen) immediately prior to imaging with an Olympus FV1000MP microscope using a 60× water immersion objective (U Plan SApo, 1.20 NA). CFP and FM1–43 were simultaneously excited with a 440 nm laser and emissions between 465 and 495 nm collected as CFP and 575 and 675 nm collected as FM1–43.
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6

Widefield and Two-photon Calcium Imaging

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Widefield imaging was performed using a GFP filter cube (460/50 excitation, 540/50 emission) and a white light source (X-cite 120Q or LED Engin LZ1-10CW00). GCaMP3 fluorescence was collected through a 10× 0.25 NA objective (Olympus) by a Photometrics CoolSnap HQ camera, furnishing a 2×2 mm2 field of view with a pixel size of 15×15 µm2. Illumination power density was 0.25 mW/mm2. For GCaMP6s, a Photometrics Evolve 512 camera was used instead.
Two-photon Ca2+ imaging was performed using an Ultima system (Prairie Technologies) with a mode-locked laser (Coherent Chameleon XR Ti:Sapphire) tuned to 950 nm and raster scanned at 5–12 Hz via a pair of galvanometer mirrors. Laser power at the sample was between 20–80 mW. Typically a 40× 0.8 NA objective (Olympus) was used, although in some instances a 25× 1.05 NA objective (Olympus XLPlan N) was used. Resolution along the y-axis was reduced by a factor of 4× for faster imaging, yielding a final pixel size of 0.45×1.8 µm (or 0.7×2.9 µm with the 25× objective). Dwell time was either 2 or 4 µs. Green emission channel (525/70 nm) was used for GCaMP3 or Fluo-2 fluorescence. Cells were imaged at depths of 150 to 430 µm, with the majority (73%) between 200 and 300 µm.
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7

Intraventricular Calcium Imaging of Embryos

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Prior to imaging, embryos were injected intraventricularly with Fluo-4AM calcium dye (17 μg of calcium dye Fluo-4AM, Molecular Probes) dissolved in 3 μl of 20% F-127 pluronic® acid (Sigma) in dimethyl sulfoxide (DMSO, Sigma) that was then diluted in artificial cerebrospinal fluid (ACSF, in mM: 125 NaCl, 1.25 NaH2PO4, 2 CaCl2, 1 MgCl2, 5 KCl, 20 D-glucose, 10 HEPES) to reach a final concentration 0.4 mM of Fluo with 13 mM FastGreen dye (Sigma) added for injection guidance.
Two-photon imaging was performed with Olympus Fluo View 1000MP system at the rate 1.2 fps at a resolution 512 × 512 via 25X objective (XLPlan N, Olympus). Excitation light was produced by Mai-Tai DeepSee laser (Spectra Physics).
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8

Coherent Anti-Stokes Raman Scattering Microscopy

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Synchronized pump (tunable from 720–990 nm) and Stokes (fixed at 1064.2 nm) beams with both 6-ps pulse width and 80-MHz repetition rate are provided by a picoEmerald system from APE (Applied Physics & Electronic, Inc.). The intensity of the 1,064 nm Stokes beam was modulated sinusoidally by a built-in electro-optic modulator (EOM) at 8 MHz with a modulation depth of more than 95%. Spatially and temporally-overlapped pump and Stokes beams were coupled into an inverted laser-scanning microscope (FV1200MPE, Olympus). A 25× water objective (XLPlan N, 1.05 NA, MP, Olympus) was used. The forward-going pump and Stokes beams after passing through the samples were collected in transmission with a condenser (oil immersion, 1.4 NA, Olympus). A large-area (10 mm ×10 mm) Si photodiode (FDS1010, Thorlabs) was used for pump intensity detection after filtering the Stokes beam completely with two high-optical-density bandpass filter (890/220 CARS, Chroma Technology). The output current of the photodiode was then sent to a fast lock-in amplifier (HF2LI, Zurich Instruments) for signal demodulation.
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9

Photostimulation-Driven Circuit Mapping

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Photostimulation was accomplished as previously described (Wang et al., 2007 (link)). In brief, for wide-field excitation, slices were exposed to blue light (465-495 nm) from a mercury arc lamp. For high-speed circuit mapping, photostimulation was done with a laser-scanning microscope (FV1000MPE; Olympus, Tokyo, Japan) equipped with × 25 NA 1.05 (Olympus XLPlan N) water-immersion objectives lens. A 510 × 510 μm area of the slice was scanned with a 405-nm laser spot (4 ms duration) in a 32 × 32 array of pixels, yielding a scanning resolution of 16 μm. The laser spot was scanned in a pseudorandom sequence, to avoid photostimulation of adjacent pixels, while cellular responses were simultaneously measured in cell-attached or whole-cell patch clamp recordings. Mapping data were analyzed with custom software to produce the synaptic input maps and averaged probability maps. Data are expressed as mean ± SEM.
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10

Ultrafast Laser Ablation Microscopy

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A 2.5 W titanium-sapphire laser (Mai Tai HP, Newport) with a pulse duration of < 100 fs and repetition rate of 80 Mhz attached to a multiphoton microscope (FV1000, Olympus) and focused through a 25× 1.05 NA objective (XLPlan N, Olympus) was used for ablation experiments. Dwell time 2 μs per scan and λ = 800 nm were used for ablation, with pixel size set to 497 × 497 nm for most experiments. Maximum power exiting the objective was 244 mW at 800 nm.
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