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Microtime 200 system

Manufactured by PicoQuant
Sourced in Germany

The MicroTime 200 is a time-resolved fluorescence microscopy system designed for time-correlated single-photon counting (TCSPC) applications. It provides high-temporal-resolution measurements of fluorescence lifetime and dynamics. The system features configurable detection channels, advanced time-correlated single-photon counting electronics, and high-performance detectors to enable versatile time-resolved fluorescence experiments.

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7 protocols using microtime 200 system

1

Oxygen Sensing Microscopy of Cells

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HT22 cells were seeded at a density of 20,000 cells/mL and cultured on cell culture dishes (35mm) with a cover glass in high glucose DMEM supplemented with pyruvate (1mM), L-glutamine (4 mM), and 10% FBS. For the fluorescence life time imaging microscopy (FLTIM), cells were incubated in tris (2, 2′-bipyridyl) dichlororuthenium (II) hexahydrate (120 μM), an oxygen sensing dye, for 2 h. Washed Cells were incubated in Dextrose (10 mM)-supplemented sterile Dulbecco's phosphate buffered saline. MB (10 μM) and glucose oxidase (GO), as a positive control, were added during microscopy. Time resolved images were obtained on a confocal MicroTime 200 system (PicoQuant GmbH, Berlin). Excitation was provided from 470 nm pulsed diode laser operating at a 320 kHz repetition rate and it was reflected off of a 490 nm dichroic plate into an Olympus IX71 inverted microscope. The light passed through an Olympus 60X 1.2 NA objective, and the collected fluorescence was filtered by a 488 nm long wave pass, interference filter before passing through a 50μm confocal pinhole. The signal from the detector was routed into time correlated single photon counting module (PicoHarp 300). Fluorescence decay curves were analyzed by the software SymPhoTime, v. 5.3.2.
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2

Fluorescence Correlation Spectroscopy

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FCS experiments
were performed using a Microtime 200 system from PicoQuant based on
an inverted confocal microscope (Olympus IX71) and equipped with two
SPADs (single photon avalanche diodes) used in the cross-correlation
mode. The excitation was achieved by a 475 or a 635 nm picosecond
diode laser operated at 20 MHz. Fluorescence emission by EITC–strep
was collected through a band-pass filter (555/20 nm) and split with
a 50/50 splitter between the two detection channels. Fluorescence
from STAR635 was collected through a band-pass filter (670/20 nm).
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3

Fluorescence Correlation Spectroscopy with TCSPC

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Fluorescence
correlation spectroscopy (FCS) experiments were performed using a
Microtime 200 system from PicoQuant, based on an inverted confocal
microscope (Olympus IX71) and equipped with two SPADs (Single Photon
Avalanche Diodes) used in cross-correlation mode. Hyp excitation was
achieved by a 475 nm picosecond diode laser operated at 20 MHz. Fluorescence
emission was collected through a bandpass filter (675/25 nm) and split
with a 50/50 splitter between the two detection channels. The setup
allowed the simultaneous acquisitions of correlation curves and time-resolved
fluorescence decays, measured by time-correlated single photon counting
(TCSPC).
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4

Fluorescence Correlation Spectroscopy of NPs

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For fluorescence correlation spectroscopy (FCS), 0.25 mg of NPs were resuspended in distilled water and incubated with 7 μg of CpG-fluorescein isothiocyanate (FITC) for 60–90 min followed centrifugation and washing at 11,000 × g for 15 min to remove excess CpG ligand. FCS measurements were done using Microtime 200 system from Picoquant GmbH (Berlin, Germany). NPs (approximately 0.25 mg) were diluted in distilled water and 30 μl of solution was dropped onto a 20 × 20 mm No. 1 coverslip (Menzel–Gläser, MA, USA). The focal height was adjusted to 20 μm above this coverslip using an Olympus i × 71 microscope and an Olympus 60 × 1.2 NA objective.
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5

FLIM Imaging of SKOV3 Ovarian Cancer Cells

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SKOV3 overian carcinoma cell line obtained from American Type Culture Collection (ATCC), Manassas, VA (USA) was grown to 70 % confluence in RPMI supplemented with 10 % FBS and 1 % Pen-Strep. Cells were trypsinized using 0.25 % Trypsin EDTA and seeded on 20 mm round glass-bottom petri dishes. After 24 hours, cells were stained with 500nM of BODIPY for 20 min at 37 °C followed by FLIM imaging on Olympus IX7 microscope. Laser excitation was provided by a pulsed laser diode (PDL-470) emitting 470 nm light and driven by a PDL 828 “Sepia II” driver. This driver was operated at 80 MHz. Measurements were performed on a MicroTime 200 time-resolved, confocal microscope by PicoQuant. The excitation and emission light was focused by a 60× 1.2 NA Olympus objective in an Olympus IX71 microscope, and the emission light was filtered by a 488 long wave pass filter before passing through a 50 µm pinhole. Detection was made by a hybrid photomultiplier assembly. The resolution of the time correlated single photon counting (TCSPC) module was set to 4 ps/bin in order to facilitate the detection at the highest possible resolution. All data analyses were performed using the SymPhoTime software, version 5.3.2. All experimental equipment and the SymPhoTime software were provided by PicoQuant, GmbH as part of the MicroTime 200 system.
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6

Probing Nanodisk Dynamics via Pulsed FRET

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PIE-FRET was performed using the MicroTime 200 system (PicoQuant). Alternating 485-nm and 640-nm laser excitation (PIE mode) was carried out at 20 MHz with laser powers 80 and 12 µW, respectively. Fluorescence-labeled nanodiscs were measured at 22 °C with a concentration adjusted to yield an average of less than 0.1 molecules within the confocal detection volume. Each measurement was performed for 15 min using freshly diluted sample. A total of 21 measurements (5.25-h measurement time) were compiled for data analysis. PIE-FRET data were analyzed using PIE analysis with MATLAB (PAM) software (59 (link)). The population with one donor and one acceptor (stoichiometry = nD/(nD + nA) = 0.5) was selected for further analysis (17,000 molecules) and corrected for relative quantum yields (Φ) and detection efficiencies (g) of donor and acceptor. Time-window analysis was performed by dividing each burst into time windows with lengths of 3, 1, 0.3, or 0.1 ms and computing the resulting FRET histogram for time windows with more than 25 photons (DexDem + DexAem) (Fig. 4A). BVA was performed using PAM software (59 (link)) in order to investigate the possibility of dynamic changes at the lateral gate of SecYEG, while diffusing through the confocal volume (Fig. 4B).
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7

Time-Resolved Confocal Microscopy Protocol

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Laser excitation was provided by a pulsed laser diode (PDL-470) emitting 470 nm light and driven by a PDL 828 “Sepia II” driver. This driver was operated at 315 KHz. Measurements were performed on a MicroTime 200 time-resolved, confocal microscope by PicoQuant. The excitation and emission light was focused by a 60× 1.2 NA Olympus objective in an Olympus IX71 microscope, and the emission light was filtered by a 488 long wave pass filter before passing through a 50 μm pinhole. Detection was made by a hybrid photomultiplier assembly. The resolution of the time correlated single photon counting (TCSPC) module was set to 512 ps/bin in order to facilitate the detection of the long-lived dye, producing a measurement window around 1.2 μs in length. All data analysis was performed using the SymPhoTime software, version 5.3.2. All experimental equipment and the SymPhoTime software were provided by PicoQuant, GmbH as part of the MicroTime 200 system.
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