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17 protocols using fluofit

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

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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3

Probing VIPP1 Binding to Liposomes

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VIPP1 (Preps #4, #5, and #6) and liposomes were mixed at 4 °C with protein and lipid concentrations of 0.4 mg/mL and 0.15 mg/mL, respectively, and incubated for 20 min at 22 °C before being transferred to a 3 mm × 3 mm quartz glass cuvette (Hellma Analytics) for measurement. TRF anisotropy measurements were recorded at 22 °C on a FluoFit 300 fluorescence lifetime spectrometer (PicoQuant) using time-correlated single photon counting. The excitation source was a pulsed LED emitting at λexc = 281 nm ± 5.5 nm. Emission was detected at λem = 355 nm ± 5 nm. Fluorescence decays were recorded with horizontal and perpendicular orientations of polarizers in the excitation and emission paths, respectively, each for 5 min. Photons were counted for 100 ns after each pulse in 4000 channels of 25 ps. The measurements were repeated after the addition of Mg2+ to a final concentration of 10 mM and an incubation at 22 °C for 20 min. Fluorescence anisotropy decays were fitted by a bi-exponential decay curve with FluoFit (PicoQuant) using data from 3–40 ns after excitation. Two rotational correlation times were obtained, where the fast one, corresponding to segmental tryptophan motions, was essentially constant at values < 0.5 ns, while the slow one, reflecting larger-scale protein motions, was exploited to probe VIPP1 binding to liposomes.
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4

Fluorescence Lifetime Decay Analysis

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The fluorescence lifetime decay is deconvoluted with the instrument response function (shown e.g. in Fig. 1e) using the commercial reconvolution software FluoFit (Picoquant). The software fits a convolution of an exponential decay with the IRF plus a multiple of the IRF as scattering contribution
I(t)=AsIRF(t)+tIRF(t)Aettτdt
to the experimental lifetime decay. For this, a time independent background of the IRF and the experimental decay are considered as well as a shift of the decay with respect to the IRF. The fitting function stems from the FluoFit software information.
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5

Ultrafast Fluorescence Lifetime Measurement

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Fluorescence lifetimes ranging from 10 ps to 20 ns were obtained by time-correlated single photon counting (TCSPC) technique (PicoHarp 300, PicoQuant). By use of deconvolution/fit program (FluoFit, PicoQuant), the time detection limit decreased to 10 ps. The second harmonic of a Titanium-sapphire laser (150 fs, 80 MHz) (Mai Tai DeepSee, Spectra-Physics) at 400 nm was used as the excitation source. Femtosecond fluorescence lifetimes were measured by a fluorescence spectrometer (TRFLS, Newport) with 100 fs resolution in combination with a mode-locked Ti-sapphire laser, the same as mentioned in TCSPC. The femtosecond laser system generated light pulses at 800 nm of duration 150 fs at a repetition rate 80 MHz, average power of 2.9 W. The frequency of the laser pulse was doubled with a BBO crystal and served for excitation (pump). The emitted fluorescence was focused into a BBO crystal together with the gate beam (800 nm) to create the up-converted signal at the sum-frequency generation. The overall time resolution of the setup was 100 fs. Fluorescent images were acquired with confocal microscopy Olympus FV1000.
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6

Photophysical Characterization of Ru(II) Complexes

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Absorbance measurements
of the Ru(II) complexes at 20 μM were performed using a Jasco
V670 spectrophotometer. Emission spectra were collected using a Varian
Cary Eclipse fluorescence spectrophotometer and luminescent lifetime
measurements were performed on a PicoQuant FluoTime 100 FLS TCSPC
system using a 450 nm pulsed laser and an external pulse generator.
Lifetime decay curves were analyzed using the PicoQuant Fluofit software
with fitting criteria; 0.9 < X2 <
1.1. For O2 sensitivity studies, the emission spectrum
and luminescent lifetime of each complex (10 μM) were recorded
under O2 saturation, and after N2 purge for
20 min. All measurements were performed in triplicate and reported
as the mean ± SD.
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7

Time-resolved Fluorescence Measurements

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Time-resolved
fluorescence measurements were conducted using the FluoTime300 instrument
from PicoQuant with a 510 nm laser (actual wavelength, 507 nm) or
a 561 nm laser as excitation source. All time-resolved data were analyzed
using FluoFit version 4.6 from PicoQuant.
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8

Photoluminescence Lifetime Measurements

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The PL lifetimes were measured
at room temperature using 568 nm excitation (4 ps pulsewidth, 40 MHz
repetition rate) and a single quantum nanowire detector. Spectral
filtering to resolve each PL peak was achieved with appropriate band-pass
(BP)/long-pass (LP) filters in front of the detector, including BP
1000/50 for E11, BP 1100/10 for E11, and LP1200 for ET. The collected decay curves were reconvolution
fitted with the corresponding instrument response function for each
detector in FluoFit (Picoquant).
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9

Fluorescence Lifetime Measurements of Fullerenol, ADH, and HSA

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The fluorescence excited-state lifetimes of fullerenol, ADH, and HSA with and without C60OH36 were measured using a FluoTime 200 lifetime fluorometer (PicoQuant, GmbH, Berlin, Germany) equipped with an R3809U-50 microchannel plate photomultiplier (MCP-PMT, Hamamatsu, Hamamatsu City, Japan) and a PicoHarp300 TCSPC module (PicoQuant, GmbH, Berlin, Germany). All the samples were measured at a temperature of 25 °C. The fluorescence lifetimes were calculated using the FluoFit software package (version 4.4)—PicoQuant, GmbH, Berlin, Germany.
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10

Fluorescence Anisotropy Analysis of Myofibrils

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To ascertain
whether the phalloidin probe is immobilized so that the transition
dipole of the fluorophore reflects the orientation of the protein,
we measured the decay of anisotropy of AP inserted into myofibrils.
Anisotropy is defined as r = (II)/(I + 2I). The fluorescence anisotropy was measured by the time domain technique
using a FluoTime 200 fluorometer (PicoQuant, Inc.) at room temperature.
The excitation was provided by a 635 nm pulsed diode laser, and the
observation was conducted through a 670 nm monochromator with a supporting
650 nm long pass filter. The full width at half-maximum (fwhm) of
the pulse response function was <100 ps, and the time resolution
was <10 ps. The intensity decays were analyzed by a multiexponential
model using FluoFit (PicoQuant, Inc.).
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