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18 protocols using lucplanfln

1

Raman Spectroscopy of Nerve Fibers

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For Raman spectroscopy study of nerve fibers, we used the confocal Raman spectrometer NTEGRA Spectra (NT-MDT, Russia) with a 532-nm laser excitation. Raman spectra were recorded by focusing the laser beam on the nerve fiber myelin surface through the ×40 objective with NA 0.6 (LUCPlanFL N, Olympus, Japan). Laser power was set to 0.8 mW and integration time for each spectrum was 50–60 s. Spectrometer has a grating with 600 lines/mm and entrance slit set to 100 μm. Raman scattered light was collected in a backscattering mode and detected with a CCD camera (1024 × 256 pixels, -50°C). Subsequent Raman spectra baseline subtraction and calculation of Raman peak intensities were made using OriginPro 2015 software (OriginLab Corporation, USA) [9 ,16 (link)].
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2

Fluorescence Microscopy Imaging Protocol

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For fluorescence microscopy imaging, an inverted microscope (IX 71, Olympus, USA), with a 100x objective (LUCPlan FL N, Olympus, USA), a mercury burner (U-RFL-T, Olympus, USA) and fluorescent filter set (exciter ET470/40x, dichroic T495LP, emitter ET525/50m, Olympus, USA) was used. Images were acquired at 150 ms/frame using a CCD camera (Quantum 512 SC, Photometrics, USA) and Micro-Manager software (University of California, USA) and analyzed with Image J software (version 1.43).
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3

Fluorescence Microscopy of Electrode Chips

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Fluorescence images of electrode chips during and after field application were acquired with an upright fluorescence microscope (Olympus BX51) equipped with a cooled CCD camera (Olympus F-View). 60× (Olympus LUC Plan FL N, N.A. = 0.70) or 100× (N.A. = 0.90) objectives were used. Fluorescence filters were adapted to the respective dye’s spectroscopic characteristics: excitation 520–570 nm, beamsplitter 565 nm, emission 635–675 nm for rhodamine 6G; excitation 460–496 nm, beamsplitter 505 nm, emission > 510 nm for TMPPPdCl4; excitation 545–580 nm, beamsplitter 600 nm, emission > 610 nm for TSPPPdNa4. An LED lamp (CoolLED pE-4000) and a mercury arc lamp (Osram HBO 103 W/2) served as illumination sources. Illumination times and image acquisition were controlled by the software Olympus CellM.
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4

Fluorescence Imaging of Organic Photovoltaics

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The fluorescence from the Structure I was collected by an objective lens (60×, N.A.:0.7, LUCPlanFLN, Olympus) and passed through a confocal pinhole (100 μm) and suitable filters. To detect the fluorescence of the BP, a 405 nm laser was used as an excitation source, and a long-pass filter (LP02-442RU, Semrock) and a short-pass filter (FF01-650/SP, Semrock) were used to cut the excitation laser beam and fluorescence from PC61BM, respectively. The detected fluorescence was split into two paths by a 50/50 beam splitter, and the two paths were detected using a spectrometer (SpectraPro2358, Acton Research Corporation) with a cooled CCD camera (PIXIS400B, Princeton Instruments) and an avalanche single-photon counting module (APD: SPCM-AQR-14, PerkinElmer). The signal from the APD was connected to a time-correlated single-photon counting board (SPC-630, Becker & Hickl) for the fluorescence images.
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5

Time-Resolved Fluorescence Microscopy

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The laser module consists of an Nd:YVO4 laser source (Cougar, Time-Bandwidth Products, Switzerland). It produces 1064 nm at the source, and by frequency-doubling, we achieve the excitation wavelength of 532 nm. The laser is pulsed at a 20-MHz repetition rate, and the pulse width is 12 ps. The PicoHarp 300 (PicoQuant, Germany) device was used for TCSPC measurements. The excitation beam enters the microscope (Olympus IX71 inverted microscope, Germany) through a dichroic mirror (ZT532SPRDC, short pass 532 nm, AHF Analysentechnik, Germany) and illuminates the chip through the objective (60 × , UPLANSApo water immersion, numerical aperture (NA) = 1.2, WD = 280 μm, Olympus or 40 × LUCPlanFLN, NA = 0.6, WD = 3.00–4.20 mm, Olympus, Germany). The fluorescent emission passes the same lens and is filtered by a bandpass filter of 295–385 nm (DUG 11, Schott, Germany) right after the dichroic mirror. A photomultiplier tube (PMA 165 nm, PicoQuant, Germany) detects the emission. The droplet sorting event was captured by a customized upright microscope, as illustrated elsewhere [39 (link)].
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6

High-Speed Imaging of Ependymal Cilia Motility

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Ependymal cilia were prepared as previously described [56 (link)]. The motility of ependymal cilia was observed under a 60x objective (LUCPlan FL N, Olympus) on a differential interference contrast microscope (BX53, Olympus) and recorded at 200 fps through a HAS-220 high-speed camera (DITECT, Tokyo, Japan).
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7

Bacterial Microcolony Formation Assay

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To form microcolonies, 1 μL of bacterial culture was deposited onto soft TSA plates (0.7% agarose, wt/vol) and incubated at 37°C for 3 h. The thickness of soft TSA plates was controlled to be ~1 mm by adding 2 mL of growth media into a 60-mm petri dish. Bacterial microcolonies on agar plates were observed directly in phase contrast mode using an Olympus X71 inverted microscope with a 60×/0.7 Ph2 Air objective (Olympus LUCPlan FL N). The white light source was provided by an Olympus TH4-100 lamp. Digital images (672 by 512 pixels with a pixel size of 107.5 nm) were acquired by an ORCA-ER digital camera (Hamamatsu, Japan).
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8

Raman Mapping of PD-L1 on Single Cells

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Single cells were identified in the bright field for imaging of selected areas by confocal Raman microscopy (WITec alpha 300 R, grating monochromator with f = 30 cm focal length, EM‐CCD grating). A 40× air objective with cover glass correction and a NA of 0.6 (Olympus LUC Plan FLN) was used. The 632.8 nm radiation from a He‐Ne laser with a power of 1.2 mW at the sample was employed for exciting Raman scattering. The integration time per pixel was 100 ms. For the localization of PD‐L1 on single cells, the cells were at first identified in the bright‐field. Next an area was selected for the SERS mapping and investigated with an integration time of 100 ms and a laser power of 1.2 mW at the sample. After performing the mapping experiments the recorded SERS spectra were processed. Raw spectra were smoothed via the Savitzky‐Golay algorithm (7th order polynomial, 31 points). Then a baseline correction (Whittaker‐Henderson procedure 29) was performed. Mean spectra with error bars were calculated using a MATLAB algorithm (shadedErrorBars). For each pixel the maximum intensity of the Raman peak centered at ca. 1590 cm−1 was determined by using a Lorentzian line profile and a nonlinear least square algorithm in order to generate the corresponding SERS false‐color images.
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9

Microscopic Analysis of DNA Droplet Protein Uptake

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We used the DIC detection mode of inverted microscope (IX-73; Olympus, Tokyo, Japan) equipped with a microscopic objective (LUCPlanFL N, NA = 0.7, 60×) and a color-sensitive camera (DP74; Olympus) (46 (link)). Light sources (U-LH100L and U-HGLGPS; Olympus) were used for DIC and fluorescence detection, respectively. The excitation wavelength was 470–495 nm, and the fluorescence at 510–550 nm was detected. The sample solution was cast on a coverslip (Matsunami Glass) and covered with a glass slide (Matsunami Glass). The coverslip and slide glass were cleaned with ethanol and 5 M KOH and coated with 0.5% 2-methacryloyloxyethyl phosphorylcholine (MPC) polymer (Lipidureμ-CM5206; NOF Corp.) in ethanol before use (47 ). DIC and fluorescence images were obtained at 21–22°C. The uptake ratio of DNA-binding proteins inside to outside DNA droplets was calculated from the ratios of the fluorescence intensities inside to outside DNA droplets.
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10

Fluorescent Ca2+ Imaging of Ciona Larvae

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The fixed Ciona larvae on a glass-based dish were observed by fluorescence microscopy with a 3CCD camera. A long-term Ca2+ transient was captured with pSP-CiVAChT:GCaMP6s or pSP-CiVAChT-H2B:GCaMP6s transduced Ciona embryos (N = 10, Figure 2; Figure 3., Supplementary Table S1). The same results can be obtained with either pSP-CiVAChT:GCaMP6s or pSP-CiVAChT-H2B:GCaMP6s (data not shown). An inverted microscope (Nikon Eclipse, IX71) with a 10×, 20×, 60× oil immersion objective lens (LUCPlanFLN) was used for fluorescence imaging with a U-MWBV2 mirror unit (Olympus, Shinjuku, Japan). SOLA LED light (Lumencor, Beaverton, OR) was used as a light source; fluorescence images were acquired with a 3CCD camera (C7800-20, Hamamatsu Photonics, Hamamatsu, Japan) and processed by the AQUACOSMOS software (Hamamatsu Photonics). Room temperature was maintained at 20°C. As a result, Ca2+ transients for both MN2L and MN2R, located at the Ciona motor ganglion region (Figure 1C), were continuously imaged from St.22 (mid tailbud II) to St.34 (late tail absorption) (N = 10, Supplementary Table S1). Ciona developmental staging (Hotta et al., 2007 (link)) was used to estimate the developmental stage from morphology and time after fertilization.
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