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Tcspc system

Manufactured by PicoQuant

The TCSPC (Time-Correlated Single Photon Counting) system is a sophisticated device designed for the precise measurement of photon arrival times. It enables the detection and analysis of low-light signals with high temporal resolution. The core function of the TCSPC system is to record the time difference between the emission of an excitation pulse and the detection of a single photon, providing detailed information about the dynamic processes under investigation.

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4 protocols using tcspc system

1

Time-Resolved Photoluminescence of f-SiC

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In this research,
the TRPL measurements on f-SiC samples are realized by the time-correlated
single-photon counting (TCSPC) system from PicoQuant GmbH. The key
components of the TCSPC system are (a) a picosecond laser diode head
(LDH-D-C-375) with λ of 375 nm and FWHM of ∼44 ps; (b)
a computer-controlled diode laser driver (PDL 828 “Sepia II”,
two channel version); (c) a hybrid photomultiplier detector assembly
(PMA Hybrid 40); and (d) a TCSPC board (TimeHarp 260 PICO) with a
digital resolution of around 25 ps. Both the injected laser pulse
and the emitted photon signal are fiber-coupled to a 50× microscope
lens with the configuration of front excitation–front detection.
After excitation, the emitted photons are filtered by a 405 nm long-pass
filter and then transferred to a photomultiplier tube. A 2 ms time
span for photon decay sampling, a 500 Hz repetition rate of laser
pulse (i.e., 80 ns resolution), a 1 h integration time were chosen
for the TRPL measurement.
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2

Cy3 Fluorescence Lifetime Measurement by TCSPC

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The fluorescence lifetime of Cy3 was measured using a TCSPC system (PicoQuant) with a TCS SP8 confocal laser‐scanning microscope (Leica Microsystems) at room temperature. The fluorescently labeled Cas9 constructs (1 μM) were loaded in a glass chamber prepared by the same procedure for smFRET measurements and absorbed onto the glass surface via Neutravidin. The buffer condition was same as that of smFRET measurement: 20 mM HEPES‐KOH, pH 7.5, 100 mM KCl, 2 mM MgCl2, 0.5 mM EGTA, 1 mM DTT, 2.5 mM TSY, 2.5 mM PCA, and 2% PCD. The Cas9 constructs on the glass surface were illuminated with a pulsed diode laser (PDL 800‐B, PicoQuant, 470 nm) through a confocal pinhole (hole size: 1 Airy unit = 0.896 μm) at a repetition rate of 20 MHz. The emission light in a range of 540–660 nm was collected through an HCX PL APO Ibd.BL 63× 1.4 NA oil objective (Leica Microsystems) in a 128 × 128 pixel format. The fluorescence lifetime data were collected on a time scale of 50 ns, resolved into 3,200 channels (i.e., 15.6 ps for each channel), and accumulated for 30 s. The data of each pixel were averaged within the whole image and then fitted with double exponential decay curves using the OriginPro 8.0J software (OriginLab). Mean lifetime (τmean) was calculated as τmean=(A1τ12+A2τ22)/(A1τ1+A2τ2) where τ and A were lifetime and amplitude, respectively.
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3

Time-resolved Fluorescence Lifetime Imaging

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Time domain FLIM experiments were performed on a Time Correlated Single Photon Counting (TCSPC) system (PicoQuant) attached to an Olympus FV-1000 confocal microscope (Olympus) with a 60 × 1.2 W objective. The excitation light source was a 485-nm pulsed diode laser controlled by a Sepia II (PicoQuant) driver with a dichroic mirror of 488/559 and a 520/30 emission filter. Individual photon arrivals were detected using a SPAD detector, and events were recorded by a PicoHarp 300 TCSPC module. Lifetime analysis was carried out using SymPhoTime 200 software. Mono- and bi-exponential fittings were applied. The percentage of binding was calculated from the amplitudes derived from the bi-exponential fitting, as previously shown (Orthaus et al., 2009 ).
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4

Fluorescence Lifetime Imaging Microscopy

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FLIM was performed on Leica TCS SP8 SMD, which consists of an inverted LEICA DMi8 microscope equipped with a TCSPC system from PicoQuant. The excitation of the CFP donor at 440 nm was carried out by a picosecond pulsed diode laser at a repetition rate of 40 MHz, through an oil immersion objective (×63, N.A. 1.4). The emitted light was detected by a Leica HyD detector in the 450–500 nm emission range. Images were acquired with acquisition photons of up to 1500 per pixel. From the fluorescence lifetime images, the decay curves were calculated per pixel and fitted (by Poissonian maximum likelihood estimation) with a tri-exponential decay model using the SymphoTime 64 software (PicoQuant, Germany).
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