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39 protocols using fluotime 200

1

Steady-State and Time-Resolved Fluorescence Measurements

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Fluorescence was measured using an SPEX Fluorolog FL3-22 steady-state fluorescence spectrometer (Jobin Yvon, Edison, NJ) equipped with double-grating excitation and emission monochromators. The measurements were made in a 2×10 mm cuvette oriented perpendicular to the excitation beam and maintained at 25 °C using a Peltier device from Quantum Northwest (Spokane, WA). For NBD measurements, the excitation wavelength was 465 nm and the slits were 5 nm. Fluorescence decays were measured with a time-resolved fluorescence spectrometer, FluoTime 200 (PicoQuant, Berlin, Germany), using a standard time-correlated single-photon counting scheme. Samples were excited at 375 nm by a subnanosecond pulsed diode laser, LDH 375 (PicoQuant, Berlin, Germany), with a repetition rate of 10 MHz. Fluorescence emission was detected at 535 nm, selected by a Sciencetech Model 9030 monochromator, using a PMA-182 photomultiplier (PicoQuant, Berlin, Germany) (Kyrychenko et al. 2009 (link)). The fluorescence intensity decay was analyzed using FluoFit iterative-fitting software based on the Marquardt algorithm (PicoQuant, Berlin, Germany).
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2

Photoluminescence Decay Analysis of Ir Dopants

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Ar-saturated 50 μM solutions in THF were used for the determination of the τobs values of the Ir dopants and H host. Photoluminescence decay traces were acquired based on time-correlated single-photon-counting (TCSPC) techniques using a FluoTime 200 instrument (PicoQuant, Germany). A 377 nm diode laser (PicoQuant, Germany) was used as the excitation source. The burst and normal modes embedded in the Time Harp 260 P module (PicoQuant, Germany) were employed for acquiring the signals from the Ir dopants and H host, respectively. The photoluminescence signals were obtained at 467 nm (Ir1 and Ir2), 460 nm (Ir3), 474 nm (Ir4), and 400 nm (H), through an automated motorized monochromator. Photoluminescence decay profiles were analyzed (OriginPro 2016, OriginLab) using a single exponential decay model.
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Fluorescence Lifetime Spectroscopy Protocol

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All fluorescence lifetime measurements at 640 nm excitation were performed with a FluoTime200 time resolved spectrometer (Picoquant, Berlin, Germany). Decay curves were analyzed using FluoFit 4.4.0.1 software. Measurements of fluorescence lifetimes of dyes with excitation at 400–560 nm were carried out with a MicroTime200 (Picoquant, Berlin, Germany), equipped with a supercontinuum laser SuperK Extreme EXW12 (NKT Photonics, Germany). The setup is attached to an Olympus IX83 with a 60 × /1.2 ultra-plan-apochromat water-immersion objective.
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4

Steady-State and Time-Resolved Fluorescence Measurements

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Fluorescence was measured using an SPEX Fluorolog FL3-22 steady-state fluorescence spectrometer (Jobin Yvon, Edison, NJ) equipped with double-grating excitation and emission monochromators. The measurements were made in a 2×10mm cuvette oriented perpendicular to the excitation beam and maintained at 25 °C using a Peltier device from Quantum Northwest (Spokane, WA). For NBD measurements, the excitation wavelength was 465 nm and the slits were 5 nm. Fluorescence decays were measured with a time-resolved fluorescence spectrometer, FluoTime 200 (PicoQuant, Berlin, Germany), using a standard time-correlated single-photon counting scheme (Posokhov and Ladokhin 2006 (link)). Samples were excited at 375 nm by a subnanosecond pulsed diode laser, LDH 375 (PicoQuant, Berlin, Germany), with a repetition rate of 10MHz. Fluorescence emission was detected at 535 nm, selected by a Sciencetech Model 9030 monochromator, using a PMA-182 photomultiplier (PicoQuant, Berlin, Germany) (Kyrychenko et al. 2009 (link)). The fluorescence intensity decay was analyzed using FluoFit iterative-fitting software based on the Marquardt algorithm (PicoQuant, Berlin, Germany).
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5

Time-resolved Fluorescence Measurements

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Time-resolved
fluorescence measurements were performed using a time-correlated single-photon
counting (TCSPC) setup (PicoQuant FluoTime 200) at 10 °C. The
concentration of the samples was <0.05 cm–1 at
the Qy maximum. A laser diode provided
the pulsed excitation light at a frequency of 10 MHz and a center
wavelength of 466 nm. The instrument response function was determined
to be 92 ps (fwhm) measuring the fluorescence decay of a pinacyanol
iodide dye dissolved in methanol that has a lifetime of 6 ps.33 (link) Power studies were performed to exclude annihilation
effects from the measurements.
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6

Characterization of Nitrogen-Doped Graphene Quantum Dots

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The absorbance spectra of the NGQDs were recorded using a UV–vis–near-infrared spectrophotometer (Carry-5000, Agilent Technologies). The PL spectra were recorded at excitation wavelengths (λex) of 379 and 405 nm using a PL spectrophotometer (Darsa, PSI Trading Co. Ltd.) with a Xe lamp. Time-resolved PL decay was measured via the time-correlated single-photon counting (TCSPC) technique using a time-resolved spectroscopy system (TRSS, Fluo Time 200, PicoQuant). A laser with an excitation wavelength of 379 nm was used to excite all of the NGQD samples. A photomultiplier tube (PMT) was used for the detection of the emitted light by the NGQD samples. To study the atomic structure of the NGQDs, HRTEM (HF-3300/NB5000/S-4800, Hitachi) was utilized. The elemental composition of the NGQDs was determined via XPS (ESCALAB 250Xi, Thermo Fisher Scientific). The XPS peaks were calibrated using the C1s peak. The Raman spectra were recorded using a confocal Raman spectrometer (Nicolet Almega XR, Thermo Fisher Scientific) with a λex value of 532 nm.
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7

Fluorescence Spectroscopy of Bimane-Labeled T-Domain

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Fluorescence was measured using an SPEX Flurolog FL 3–22 steady-state fluorescence spectrometer (Jobin Yvon, Edison, NJ, USA) equipped with double grating excitation and emission monochromators. The measurements were made at 25 °C in 2 × 10 mm cuvettes oriented perpendicular to the excitation beam. For the bimane fluorescence measurement, the excitation emission wavelength was 380 nm and the emission spectra were recorded between 395 and 700 nm using excitation and emission spectral slits of 2 and 4 nm, respectively. Solution acidification was achieved by the addition of small amounts of 2.5 M acetic buffer. All the spectra were recorded after 30 min of incubation to ensure the equilibrium of the sample.
The fluorescence lifetime kinetics of bimane-labeled T-domain were measured with a time-resolved fluorescence spectrometer FluoTime 200 (PicoQuant, Berlin, Germany) using a standard time-correlated single-photon counting scheme. Samples were excited at 373 nm by a sub-nanosecond pulsed diode laser LDH 375 (PicoQuant, Berlin, Germany) with a repetition rate of 10 MHz. Fluorescence emission was detected at 480 nm, selected by a Sciencetech Model 9030 monochromator, using a PMA-182 photomultiplier. The fluorescence intensity decay was analyzed using the FluoFit version 2.3 iterative-fitting software based on the Marquardt algorithm (PicoQuant, Berlin, Germany).
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8

Time-Resolved Fluorescence Lifetime and Anisotropy

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Fluorescence lifetime and anisotropy decays of all the solutions were measured using FluoTime 200 (PicoQuant, GmbH, Berlin, Germany) time domain fluorometer. This instrument contains multichannel plate detector (Hamamatsu, Japan) and a 485 nm laser diode was used as the excitation source. The fluorescence lifetime was measured in magic angle conditions and data was analyzed with FluoFit version 5.0 software (PicoQuant GmbH, Berlin, Germany) using a multiexponential deconvolution model:
Where IRF (t) is the instrument response function at time t′, α is the amplitude of the decay of the ith component at time t and τi is the lifetime of the i-th component.
Excitation used for time resolved anisotropy measurement was 485 nm while emission was observed at 625 nm with vertical and horizontal polarizer position on the emission side using appropriate filters on both excitation and emission side. Anisotropy decay was analyzed with an associate anisotropy decay model using fitting routine design in MathCad 15 platform.
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9

Fluorescence Lifetime Measurement Protocol

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Fluorescence intensity decays were measured using time-correlated single-photon-counting with a FluoTime200 fluorimeter (PicoQuant, Inc., Berlin, Germany). Excitation was at 295 nm. Emitted light at 340 nm was selected using a monochromator. To avoid effects of Brownian rotation a polarizer oriented at the magical angle was placed on the emission side. A micro channel plate was used to detect the emitted light. The intensity decay data were fitted with FluoFit software (PicoQuant version 4).
Some fluorescence lifetimes were measured using Fluorolog fluorimeter equipped with Nano-LED laser (Horiba Scientific Inc., Edison, NJ). Excitation was at 278 nm. The emitted light at 340 nm was selected using a monochromator. A photomultiplier tube (Hamamatsu 928, Japan) was used to detect emitted light. The intensity decay data were fitted with Data Analysis Software (Horiba Scientific Data Station 2.7).
The data were analyzed in terms of a sum of exponentials: I(t) = Σαi exp (−t/⊤i) where αi are the amplitudes of the intensity decay times ⊤i with Σαi = 1.0. The intensity mean lifetime is defined as ⊤mean = Σαii2/Σαii.
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10

Fluorescence Lifetime and Anisotropy of Doxorubicin

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Fluotime 200 (Picoquant, Berlin, Germany) was used to measure the fluorescence lifetime and time-resolved anisotropy of Doxorubicin in PBS and PVA. Time resolved measurements were collected using a front-face set-up for both samples. The fluorometer is equipped with an ultrafast detector from Hamamatsu, Inc. A 470 nm laser diode was used as the excitation source, and the emission observed at 600 nm, with both vertical and horizontal polarizer orientations on the observation. These measurements were done at room temperature.
The fluorescence lifetimes were measured in magic angle conditions, and the data was analyzed using Fluofit3 program using a multi-exponential fitting model:
where, αi is the amplitude of decay of the ith component at time t, and τi is the average decay time of the fluorophore. In the case of multi-exponential decay, the mean lifetime is given by,
where,
The anisotropy decays were analyzed using a single-exponential fitting model using the Fluofit3 program using the following equation:
where, r0 is the anisotropy at t = 0, and ϕ is the rotational correlational time of the fluorophore.
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