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28 protocols using f 4600 spectrofluorometer

1

Quantifying Hydroxyl Radicals in Amyloid Beta Aggregation

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CCA was used as a fluorescence probe for OH· determination [31 (link)] with a Hitachi F-4600 spectrofluorometer from Hitachi High-Tech Corporation (Tokyo, Japan). CCA fluorescence was recorded at 540 nm, with an excitation wavelength of 390 nm. The widths of the entrance and exit slits were both 5 nm. The OH· amounts in the solutions of the Aβ(1–42) (10 μM)/Cu2+ (5 μM)/AA (1 mM) mixtures in different concentrations of DHPA (0.5, 4, 10 μM) were detected with a CCA probe. The fluorescence ratio was calculated as follows:
where F is the CCA fluorescence intensity in each solution and F0 is the CCA fluorescence intensity of the Aβ(1–42) (10 μM)/Cu2+ (5 μM)/AA (1 mM) mixture.
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2

ROS Measurement in SH-SY5Y Cells

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DCFH-DA was used to detect the level of intracellular reactive oxygen species (ROS). The SH-SY5Y cells were treated with different solutions for 24 h and then treated according to the instruction of the DCFH-DA kit. The fluorescence intensity was recorded with the Hitachi F-4600 spectrofluorometer from Hitachi High-Tech Corporation (Tokyo, Japan) with the excitation and emission wavelengths at 485 nm and 525 nm. The fluorescence ratio was calculated as follows:
Where F is the DCFH-DA fluorescence intensity of Aβ (1–42) (10 μmol/L)/Cu2+ (5 μmol/L)/AA (1 mmol/L)/Ma-3-gal-Cl (0.5, 4, 10 μmol/L) mixtures treated SH-SY5Y cells, and F0 is the DCFH-DA fluorescence intensity of the Aβ (1–42) (10 μmol/L)/Cu2+ (5 μmol/L)/AA (1 mmol/L) treated SH-SY5Y cells.
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3

Fluorescence-based Quantification of HHWH Peptide

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Fluorescence measurements of HHWH peptide solutions were carried out at room temperature using an F-4600 spectrofluorometer (Hitachi, Japan). An excitation wavelength (λex) of 280 nm was used, and an emission peak was recorded at 353 nm for HHWH. Both the entrance and exit slits had a width of 5 nm. Fluorescence measurements were performed three times, and the standard deviation was plotted as an error bar.
The quantum yield (f) of HHWH was determined using the following expression:
where FHHWH and FTrp are the fluorescence emission intensities of the HHWH samples and the reference, which is tryptophan (Trp) dissolved in 10 mM HEPES buffer (pH 7.4). AHHWH and ATrp are the absorbance values at 280 nm of the HHWH samples and the tryptophan solutions, respectively, whereas fHHWH and fTrp are the quantum yields of the respective solutions.
Determining the concentration of Cu 2+ in real samples HHWH (10 μL, 200 μM) was added into the HEPES (188 μL, 10 mM, pH 7.4) buffer, and then a real sample (2 μL) was added into the mixture. The fluorescence intensities of the resulting mixtures were recorded. Each experiment was repeated three times.
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4

Spectroscopic Characterization of Compounds

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All reagents were of commercially analytical grade and used directly.
Fluorescent spectra were recorded using a Hitachi F-4600 spectrofluorometer (Tokyo, Japan), and UV-Vis spectra were determined on a Hitachi U-2910 spectrophotometer. 1H- and 13C-NMR spectra were carried out with a Brucker AV 400 nuclear magnetic resonance instrument (Faellanden, Switzerland), and the chemical shift is given in ppm from tetramethylsilane (TMS). Mass spectra were obtained using a thermo TSQ Quantum Access Agilent 1100 mass spectrometer (Santa Clara, CA, USA). Fluorescence imaging was performed with Olympus FluoView Fv3000 laser scanning microscope (Tokyo, Japan).
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5

Comprehensive Characterization of Perovskite Materials

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The surface morphology of 3D FACs and 1D/3D PyPbI3/FACs perovskite was characterized by using scanning electron microscopy (SEM, Regulus-8100, HITACHI, Tokyo, Japan) operating at 20 kV. The crystal structure was investigated by X-ray diffraction (XRD, DX2700, Dandong Kemait NDT C., Ltd, Liaoning, China) with a 2θ ranging from 5 to 37° in a step of 5° min−1, using a monochromatic Cu Kα radiation source. Before the 3D FACs and 1D/3D PyPbI3/FACs perovskite were exposed to gases, the XRD measurement was held on a glass substrate different from the deposited material on electrodes in order to avoid any interaction of sensing elements from the X-ray beam. The absorbance spectrum of the 3D FACs and PyPbI3/FACs perovskite were measured by UV-visible spectroscopy (T9, PERSEE, Beijing, China) in the wavelength ranging from 400 to 870 nm on a quartz glass substrate. The photoluminescence (PL) spectrum of 3D FACs and 1D/3D PyPbI3/FACs hybrid-structured perovskite were investigated with a Hitachi F-4600 spectrofluorometer, Tokyo, Japan.
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6

Analytical Techniques for Photocatalytic Experiments

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The amount of the hydrogen product was analyzed by gas chromatography (Shimadzu GC-2014+AT 230C, TDX-01 column, TCD, argon carrier). UV-vis absorption spectra were recorded on a LAMBDA750 UV-vis spectrophotometer. FL spectra were taken on Hitachi F4600 spectrofluorometer. Transient absorption spectra were measured on the LP980 laser flash photolysis instrument (Edinburgh, UK). FL lifetime was performed by time-resolved confocal FL instrument (MicroTime 200, PicoQuant, Berlin, Germany). Photocatalytic experiments were conducted with 450 and 525 nm LED light (Zolix, MLED4) and 175 W Xenon lamp (LX-175, PEILC, Japan) with 420 nm filter. Electrochemical measurements were carried out on a CHI 760E electrochemical workstation at room temperature.
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7

Luminescent CaSr2(PO4)2:Sm3+,Li+ Phosphors

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A series of the obtained CaSr2−2x(PO4)2:xSm3+,xLi+ phosphors were measured by XRD analysis (XD-3, PGENERAL, China) in the 2θ range of 10° to 70°, with Cu Kα radiation (λ = 0.15406 nm) operating at 40 kV and 40 mA. The step scanning rate (2θ values ranging from 5° to 120°) used for Rietveld analysis was 1 s per step with a step size of 0.02°. The PL and PLE spectra of the phosphors were measured on a F-4600 spectrofluorometer (HITACHI, Japan) with a photomultiplier tube operating at 500 V, and a 150 W Xe lamp used as an excitation source. A 400 nm cut-off filter was used to eliminate the second-order emission. The temperature-dependent PL spectra were also measured on the same spectrofluorometer with a home-made heating controller. The CaSr2(PO4)2 were observed by SEM using a HitachiS-520 instrument. The X-ray photoelectron spectroscopy (XPS, ESCALab250, Thermo Scientific, America) with monochromatic 150 W Al Kα radiation was used to detect Sm3+. The room-temperature luminescence decay curves were recorded with a spectrofluorometer (Horiba, JobinYvon TBXPS), using a tunable pulse laser radiation as the excitation source.
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8

Nanoparticle Characterization Techniques

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The fluorescence emission spectra shown in this paper were measured on a F4600 spectrofluorometer (Hitachi, Japan) with 380 nm excitation. FT-IR spectra and UV–vis spectra were respectively recorded on a FTIR-8400S spectrometer (Shimadzu, Japan) and WFN-203B spectrometer (Jingke, China). The transmission electron microscopic images (TEM) were measured by a JEM-2100 transmission electron microscope (JEOL, Japan). The size distribution of nanoparticles was determined by the Nicomp380ZLS dynamic light scattering technique (Santa Barbara, USA).
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9

Hydroxyl Radical Detection in Nanoparticles

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To assess whether the as-generated ROS species include hydroxyl radical, we performed similar fluorescence-based ROS detection assays but using p-phthalic acid (PTA) as the probe for hydroxyl radical33 (link). PTA is virtually non-fluorescent but, upon oxidation selectively by hydroxyl radical, becomes brightly green fluorescent (λex/λem = 315 nm/320–600 nm). Specifically, PTA powder was dissolved in NaOH aqueous solution (0.2 M), to a PTA concentration of 50 mM. The resulting TPA solution was then mixed with a nanoparticle dispersion in PBS (at an expected mass concentration of nanoparticle) to a final mixture volume of 200 μL and a final TPA concentration of 500 μM, followed by incubation at 37 °C for 3 h. The resulting mixture was subsequently centrifuged at 8000 × g for 10 min to remove the nanoparticles, and the resulting supernatant was then subjected to fluorescence emission spectrum recording (λex/λem = 315 nm/320–600 nm, with slit-widths of 5 and 10 nm for excitation and emission wavelengths, respectively) using a fluorimeter (F-4600 spectrofluorometer, Hitachi). Control is PTA in PBS-treated similarly but without any nanoparticle. Hydroxyl radical generation was indicated by the relative enhanced fluorescence intensity at 400 nm of a nanoparticle-containing dispersion compared to that of PTA in PBS. The reported results are averages of two independent trials.
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10

Measuring Drug Encapsulation in Gold Nanoparticles

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ICG and DOX drug loading (DL) yields and encapsulation efficiency (EE) within the GNP were determined by measuring ICG absorbance at 800 nm and DOX fluorescence intensity at 595 nm (λex = 488 nm) and comparing them to standard curves of the free ICG and DOX. Briefly, the standard curve of ICG in PBS was obtained by measuring the absorbance at 800 nm in solutions of free ICG at different concentrations with a UV–Vis spectrometer (Molecular Devices). The standard curve of DOX in PBS was obtained by measuring the emission fluorescence at 595 nm for different DOX concentrations with a fluorimeter (F-4600 spectrofluorometer, Hitachi, Tokyo, Japan). The DL and EE were calculated based on Eqs. (1), (2), respectively: DL (%)=WeightofloadeddrugTotalweightofGNP-DOX/ICG×100 EE (%)=WeightofloadeddrugTotalweightoffeedingdrug×100
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