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Timeharp200

Manufactured by PicoQuant
Sourced in Germany

The TimeHarp200 is a high-performance time-correlated single-photon counting (TCSPC) module designed for time-resolved fluorescence and photon timing applications. It features picosecond time resolution, low timing jitter, and high count rate capabilities. The TimeHarp200 provides precise time-of-arrival measurements for individual photons, enabling accurate characterization of fast optical processes and phenomena.

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10 protocols using timeharp200

1

Quantitative Single-Molecule FRET Assay

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spFRET experiments were performed on a home-built confocal microscope, as previously described (34 (link)). Reactions were performed in SigmaCote™ treated 384-well microplates, as described above in 40 μl total reaction volume. DNA was diluted to 30–70 pM and subsequently equilibrated with the specified TBP concentrations in binding buffer (0.5 mM MgCl2) containing the indicated KCl concentration for 20 min; samples additionally contained 0.5–1 mM ascorbic acid to minimize photobleaching. Samples were illuminated with 488 nm laser light with donor (535AF45 filter) and acceptor (HQ705/90 filter) emission signals collected on avalanche photodiodes (SPCM-AQ-14, PerkinElmer) for 30 min. Single photon data from a time-correlated-single-photon-counting board (TimeHarp200, PicoQuant) were analyzed using in-house software; single-molecule events were discriminated against background following a burst selection protocol that is described elsewhere (34 (link)). Proximity ratios and histograms were then generated in IGOR software (Wave Metrics) with data fit using the integrated Gaussian fitting function; Gaussian curve-fits in Figure 2 excluded the donor-only peak.
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2

Quantitative Analysis of Quantum Dot-Protein Interactions

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FCS measurements were performed on a home-built system, which was based on an inverted Olympus IX73 microscope. A NKT supercontinuum white-light pulse laser was used as the excitation laser. The repeat frequency, excitation wavelength, and laser power were 3.123 MHz, 592 nm, and 60 μW, respectively. The excitation light was focused by a 60× water immersion objective. The fluorescence emitted by the sample was collected by the same objective and detected by an Excelis Detector (SPCM-AQRH-16). Timeharp 200 (PicoQuant, Berlin, Germany) was used for photon-counting. The coverslip used in the cuvette was coated with a layer of PEG (2 k) to avoid adsorption of fluorescent molecule. The temperature was controlled by an mK1000 series temperature controller (INSTEC, Inc., USA).
QD solutions (200 µL, 8 nM) were mixed with the equal volume BSA solutions with different concentrations (50 nM to 100 µM) diluted in different phosphate buffers (pH = 6.0, 7.4, and 9.0). The solution was incubated at different temperatures (298 K, 300 K, 303 K, and 308 K) for 1 h before FCS measurements. Each sample was measured at least three times and then the average was taken to reduce the error.
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3

GFP-Protein Mobility Tracking via FCS

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FCS traces were collected in live cells expressing GFP-tagged proteins. For each cell, triplicate measurements were recorded in the nucleus and the corresponding diffusion times were averaged. FCS measurements were performed on a customized system comprised of an Olympus IX71 microscope and a scanning confocal module (Microtime 200, PicoQuant GmbH) for time-correlated single photon counting time-tagged time-resolved measurements (Time Harp 200, PicoQuant GmbH). A picosecond pulsed 467 nm laser line was used as excitation source for GFP via a water immersion objective (60×, NA = 1.2). Emitted fluorescence was collected using the same objective and filtered from the excitation light by a dichroic mirror (z467/638rpc, Chroma). Fluorescence signals were selected through a 50 μm pinhole to exclude the background noise and out-of-focus fluorescence, and finally recorded by a single photon avalanche photodiodes (SPCM-AQR-14, PerkinElmer Inc.) after passing the 520–40 (Chroma) band pass filter. Collected fluorescence fluctuation was autocorrelated using the software SymPhoTime (PicoQuant GmbH) and fitted with a least-square algorithm.
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4

Time-Correlated Single Photon Counting Setup

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A schematic illustration of the TCSPC setup arrangement is shown in Figure 2A. The pulsed, 561 nm pico-second laser (D-TA 560B, PicoQuant) was operated at 10 MHz frequency. The laser beam was spatially filtered by feeding it through a single-mode polarization preserving optical fiber (Point source), and the collimated beam output was further expanded and steered to fill the back aperture of a 63x/1.15 NA water immersion objective (Zeiss). The emitted light was separated from the excitation using an appropriate dichroic mirror and focused onto a 50 μm pinhole located at the focal point of a 200 mm achromatic doublet lens (Thorlabs). The light was then filtered by a 562 nm notch and a 500 nm long pass filters (Semrock) and focused onto a low dark count single photon avalanche diode (SPAD) (PDM-100ct, MPD). The NIM output of the APD was used for superior timing resolution and was fed to the TimeHarp 200 or MultiHarp 150 acquisition hardware (PicoQuant). The sync pulse from the laser driver (PDL-800-D, PicoQuant) was connected through a 3 m long coaxial cable.
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5

Multicolor Fluorescence Lifetime Imaging

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Details of this setup have been published elsewhere16 (link),19 (link). The exciation is performed with two pulsed diode lasers from Picoquant, emiting at 405 nm (LDH-P-C-405B, FWHM 60 ps, Picoquant-Germany) and 375 nm (LDH-P-C-375B, FWHM 45 ps, Picoquant-Germany). The diodes are controlled by a driver (PDL-808 “Sepia”, PicoQuant GmbH, Berlin, Germany). The repetition frequency used for this study is 40 MHz.
A single-core fiber with a 200 μm diameter, is used to bring the excitation to the sample. The signal is then collected through a single-core optical fiber with a 365 μm diameter. Then the collected signal goes through a long pass filter (SR420, Semrock) to cut the signal from laser reflection. For spectral measurement, a spectrometer (QEPro 6500, Ocean Optics, 1.5 nm spectral resolution over a 365-950 nm spectral range) was used. For lifetime measurements a filter wheel (FW102C, Thorlabs, Newton, USA) with five filters (Semrock, New York, USA, 450 ± 10 nm, 520 ± 10 nm, 550 ± 30 nm, 620 ± 10 nm and 680 ± 10 nm) in front a photomultiplier link to a TCSPC acquisition card (PMA 182 and Time Harp 200, Picoquant, Germany) was used.
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6

Fluorescence Lifetime Imaging Microscopy

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The setup of FLIM consists of a picosecond diode laser with emission wavelength of 470 nm with laser power of 5 mW (LDH470, PicoQuant, Germany) and a ∼70 ps pulse width for the excitation of o-BMVC under a scanning microscope (IX-71 and FV-300, Olympus, Japan) (23 ). The fluorescence of o-BMVC was collected using a 60X NA = 1.42 oil-immersion objective (PlanApoN, Olympus, Japan), passing through a 550/80 nm bandpass filter (Chorma, USA), and then detected using a fast PMT (PMA182, PicoQuant, Germany). The fluorescence lifetime was analyzed using a time-correlated single photon counting (TCSPC) module and software (TimeHarp-200 and SymPhoTime, PicoQuant, Germany). FLIM images were constructed from pixel-by-pixel lifetime information.
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7

Fluorescence Lifetime Imaging Analysis

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Fluorescence lifetime (τ) is defined as the average time the fluorophore stays at the excited state prior to emitting the first photon and can be expressed as:
τ=ΓΓ+knr where Γ is the emissive rate and knr the non-radiative decay rate. Fluorescence lifetime is independent of the molecular concentration and excitation intensity, but it is quite sensitive to the surrounding physicochemical factors such as pH. In the time-domain lifetime measurement, the pixel-by-pixel emitted photons were recorded using time-correlated single photon counting (TCSPC) module and stored in time-tagged time-resolved (TTTR) format (Time Harp200, PicoQuant GmbH), based on which the lifetime can be calculated as the amplitude of detected photons decays to 1/e: F(t) = F0e−t/τ. In FLIM images, a TCSPC histogram is generated for each pixel to reconstruct a color-coded lifetime image.
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8

Fluorescence Lifetime Measurement Protocol

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For fluorescence lifetime measurements, a pulse picker (Model 350-160, ConOptics) was placed in the laser beam to reduce the pulse frequency from 80 MHz to 20 MHz. Samples (2 μM dye diluted in 50 mM HEPES, pH 7.2, H2O, or CH3OH) were excited at 830 nm laser wavelength and 6 mW laser power. The emitted light was collected by the fast-timing APD and fed to the single-photon counting board (TimeHarp200; PicoQuant). Timing pulses were obtained from a PIN diode (DET01CFC; ThorLabs) monitoring the 20 MHz pulse train. The temporal impulse response of the system was determined by second harmonic generation of laser pulses using a thin nonlinear crystal in place of a dye sample. The lifetime decay data was fit to a single exponential decay function using a custom MATLAB program. Lifetime value of the reference fluorescein dye measured using our system was 4.025 ± 0.015 ns (R2 = 0.99) compared to a literature value of 4.1 ± 0.1 ns.45
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9

Two-Photon Fluorescence Microscopy Protocol

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Fluorescence microscopy measurements were performed on an Olympus IX71 inverted microscope with an UPlanSApo × 60/1.2 W water immersion objective. A Ti:sapphire oscillator (Chameleon, Coherent) centering at 800 nm served as the two-photon excitation source. A dichroic mirror 715DCSPXR (AHF) and a short pass filter E700SP were used to separate the excitation and emission and the dichroic mirror 590DCXR (AHF) to split the fluorescence onto the green and red avalanche photodiode detectors (SPCM-CD 2969, PerkinElmer), selected with band pass filters D525/20m and D680/30m (Chroma). Data were acquired with a router (PRT 400)-coupled TCSPC card (TimeHarp200, PicoQuant) and analysed with the SymPhoTime software version 5.3 (PicoQuant).
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10

Fluorescence Lifetime Measurement Protocol

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For fluorescence lifetime measurements, a pulse picker (Model 350-160, ConOptics) was placed in the laser beam to reduce the pulse frequency from 80 MHz to 20 MHz. Samples (2 μM dye diluted in 50 mM HEPES, pH 7.2, H2O, or CH3OH) were excited at 830 nm laser wavelength and 6 mW laser power. The emitted light was collected by the fast-timing APD and fed to the single-photon counting board (TimeHarp200; PicoQuant). Timing pulses were obtained from a PIN diode (DET01CFC; ThorLabs) monitoring the 20 MHz pulse train. The temporal impulse response of the system was determined by second harmonic generation of laser pulses using a thin nonlinear crystal in place of a dye sample. The lifetime decay data was fit to a single exponential decay function using a custom MATLAB program. Lifetime value of the reference fluorescein dye measured using our system was 4.025 ± 0.015 ns (R2 = 0.99) compared to a literature value of 4.1 ± 0.1 ns.45
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