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Life 888

Manufactured by Oxford Instruments

The Life 888 is a laboratory equipment product designed for scientific applications. It serves as a core instrument for conducting various experiments and analyses. The product's primary function is to provide a controlled environment for carrying out research and testing procedures. The specific details and intended use of the Life 888 are not available within the scope of this response.

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6 protocols using life 888

1

Live Imaging of Cellular Dynamics

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Live imaging was performed using a custom-built inverted spinning disk confocal microscope (3i imaging systems; model CSU-W1) attached to an Andor iXon Life 888. Image acquisition was controlled by SlideBook 6 software. Images were acquired with a Plan-Apochromat 63x/1.4 NA. Oil objective, M27 with DIC III prism, using a CSU-W1 Dichroic for 488/561 nm excitation with Quad emitter and individual emitters, at laser powers 1.1 mW (488 nm) and 0.8 mW (561 nm) for photoactivation and Vapb OE (Vapb-emerald) experiments; and laser powers 2 mW (488 nm) and 2.7 mW (561 nm) for spine structural plasticity measurements. During imaging, the temperature was maintained at 32 °C using an Okolab stage top incubator with temperature control.
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2

Live-Cell Imaging of Intracellular Dynamics

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Fluorescence images and movie files were obtained using microscope (Olympus IX73) equipment with total internal reflection fluorescence (TIRF) illumination and spinning‐disk confocal imaging mode (Yokogawa W1). A 60× oil‐immersed objective (1.50 N.A., Olympus) and a back‐illuminated EMCCD camera (Andor iXon Life 888) were used. The pixel size is 0.2166 µm. To maintain cell physiology, an on‐stage incubator (OKO Lab) was installed on the microscope to maintain 37 °C and 5% CO2 for cells during imaging. To track the movements of fluorescent particles, highly inclined and laminated optical sheet (HILO) imaging was performed by properly decreasing the incident angle of the laser. A 561 nm laser was used to excite the QD, 70‐kD, and 2000‐kD dextrans, Qtracker, 100 and 500‐nm fluorescence beads. The movements of QDs and 2000‐kD dextrans in cells were acquired as movie files with a total of 1 min at 30 ms intervals, the 70‐kD dextrans were recorded with a total of 30 s at 10 ms intervals, and the endocytic fluorescence beads were recorded with a total of 3 min at 100 ms intervals. To track the movements of SGs, the spinning‐disk confocal mode was applied, with recording for 3 min at 100 ms intervals. A 488 nm laser was used to excite EGFP‐G3BP1.
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3

Fluorescent Ca2+ Imaging of Endothelial Cells

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Arteries were incubated in a loading solution containing a fluorescent Ca2+ indicator, Cal-520 acetoxymethyl ester (Cal-520/AM; 5 µM), 0.02% Pluronic F-127, and 0.35% dimethyl sulfoxide in PSS for 30 min (37 °C). All Ca2+ measurements were carried out in PSS. Cal-520 was excited with 488-nm wide‐field epifluorescence illumination provided by a light-emitting diode illumination system (PE-300Ultra, CoolLED) and imaged using an EMCCD camera (13-µm pixel size iXon Life 888; Andor), through a 16× (water immersion; numerical aperture of 0.8; Nikon CFI75) objective lens or 40× (water immersion; numerical aperture of 0.8; Nikon CFI Apo) objective lens. Fluorescence emission was recorded at 10 Hz. Fluorescence illumination was controlled, and images (16-bit depth) were captured by µManager.
Ca2+ imaging recordings were analyzed using custom FIJI macros and custom analysis software written in the Python 2.7 programming language (5 (link), 24 (link)). ROIs were automatically generated for each endothelial cell so that a direct comparison of the Ca2+ activity in each cell between various pharmacological applications could be made (24 (link), 47 (link)).
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4

Multi-color Super-Resolution Imaging Protocol

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Dual-color SRRF imaging was performed on a spinning disc confocal microscope (14 (link)). HMRef and Alexa Fluor 647 phalloidin excitation was conducted with a 488-nm/150-mW diode laser (LM-488-150, Andor) and a 637-nm/140-mW diode laser (LM-637-140, Andor), respectively. The two lasers were fiber coupled (seven-line laser combiner, multimode ×2, single mode ×1; LC-ILE-700-M2-S1, Andor) to a spinning disk confocal unit (CR-DFLY505, Andor) equipped with a multiband dichroic mirror (DFly laser dichroic for 405/488/561/640). The fluorescence was processed with appropriate filter sets for HMRef (TR-DFLY-F525-050, Andor) and Alexa Fluor 647 (TR-DFLY-F700-075, Andor) to capture fluorescence images with a charge-coupled device (CCD) camera (iXion Life 888, Andor), driven by Fusion software (version 2.0 for Fig. 2 and version 2.2 for fig. S19; Andor). Images were taken using a 60× objective (APON60XOTIRF, numerical aperture (NA) 1.49, Olympus], mounted on an inverted microscope (IX83, Olympus), and equipped with Z-drift compensator (IX3-ZDC2, Olympus).
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5

Two-Photon Excitation Microscopy Protocol

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It mainly comprises two‐photon excitation and visible fluorescence detection, as illustrated in Figure S5, Supporting Information. The intensity of the femtosecond laser source (either a 920 nm (Spark Lasers, ALCOR 920) or a 1036 nm (YSL, Femto YLTM)) was controlled by a 1/2 λ wave plate (Thorlabs, AHWP05M‐980) and a polarizing beam splitter (PBS) cube (Thorlabs, CCM1‐ PBS252). The laser beam was then expanded by lenses (L1 and L2) and reflected to a high‐speed spatial light modulator (SLM, Meadowlark, HSP1920‐1152) at ≈10°. Another 1/2 λ wave plate was used to facilitate the desired polarization of the SLM. L3 and L4 create magnified phase patterns of the SLM at the rear pupil plane of the objective (Nikon, CFI Apo LWD 25X, 1.1 NA, and 2 mm WD). The fluorescence beam was focused by L5 and then captured by an EMCCD (Andor, Life 888, 1024 × 1024 pixels, 13 × 13 µm2).
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6

Non-invasive NIR Imaging of PEI-CDs@BSA

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6–8‐week‐old nude mice were used for the NIR fluorescence imaging. The mouse was intragastric with 0.4 mL PEI‐CDs@BSA aqueous solution (PEI‐CDs 15 mg mL−1, BSA 15 mg mL−1) through gavage injection. An ANDOR iXon Life 888 electron‐multiplying CCD camera coupled with a 750 nm long‐pass optical filter was employed to perform real‐time in vivo NIR fluorescence imaging under an excitation laser of 690 nm. Imaging was performed at various time points.
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