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Flsp920 spectrometer

Manufactured by Edinburgh Instruments
Sourced in United Kingdom

The FLSP920 is a spectrometer designed for laboratory use. It is capable of measuring the spectral characteristics of various light sources and materials. The device uses a combination of optical components and a detector system to analyze the wavelength composition of input light. The FLSP920 provides accurate and reliable spectral data for scientific and research applications.

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14 protocols using flsp920 spectrometer

1

Photophysical Characterization of Compounds

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All photophysical measurements were carried out under an argon atmosphere. All solution state measurements were performed in standard quartz cuvettes (1 cm × 1 cm cross section). UV/Vis absorption spectra were recorded using an Agilent 1100 diode array UV/Vis spectrophotometer. Excitation, emission, lifetime and quantum yield measurements were recorded using an Edinburgh Instruments FLSP920 spectrometer equipped with a 450 W Xenon arc lamp, double monochromators for the excitation and emission pathways, and a red-sensitive photomultiplier (PMT-R928P) and a near-IR PMT as detectors. The measurements were made in right-angle geometry mode and all spectra were fully corrected for the spectral response of the instrument. All solutions used in photophysical measurements had a concentration lower than 10–5 M.
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2

Characterization of Passivated Semiconductor Materials

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The structural and optical properties of the as-deposited and passivated samples were characterized by FTIR (Nicolet iS50, Thermo Scientific, Waltham, MA, USA) and UV-VIS-SE (GESP-5, Semilab, Budapest, Hungary). The room-temperature steady-state PL measurements were performed in an FLSP920 spectrometer from Edinburgh Instruments using a Xe lamp at 300 and 400 nm excitation (Edinburgh Instruments, Livingston, UK). Additionally, TDPL and TD-TRPL studies were conducted by utilizing a closed-loop cold finger cryostat (ST-100, Janis Research, Woburn, MA, USA). TRPL spectra were collected in the same spectrometer utilizing a time correlated single photon counting method, with a pulsed diode laser source [λ = 405 nm (3.06 eV), ~50 ps full width at half maximum (FWHM) and 20 MHz repetition rate].
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3

Structural Characterization of CsPbBr3 Perovskite NCs

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Crystal structure identification of the NCs was carried out using XRD, performed on a Bruker D8 Advance diffractometer using Cu-Kα radiation. The bulk XRD pattern was obtained from the inorganic crystal structure database (ICSD). TEM measurements were performed using a Tecnai F30UHR version electron microscope, equipped with a field emission gun (FEG) at an accelerating voltage of 200 kV and a JEOL JEM-3010 transmission electron microscope with an accelerating voltage of 300 kV. A drop of purified NCs which were dissolved in hexane was placed on a carbon coated Cu grid. The solvent was allowed to evaporate leaving behind the NCs for imaging. UV-visible absorption spectra of CsPbBr3 perovskite NCs dissolved in hexane were obtained using an Agilent 8453 UV-visible spectrometer. Steady state PL spectra were collected using a 450 W xenon lamp as the light source on an FLSP920 spectrometer, Edinburgh Instruments, while the PL lifetime measurements were carried out on the same instrument using an EPL-405 pulsed diode laser as the excitation source (λex = 405 nm).
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4

Photophysical Characterization of Compound 1

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The concentrations of 1 used in all photophysical measurements were ca. 5 × 10−6 M in hexane while those used for the emission spectra have a maximum absorbance less than 0.2 to avoid re-absorption. Absorption spectra were recorded on an Agilent 8453 diode-array UV-Vis spectrophotometer. The emission and excitation spectra were recorded using an Edinburgh Instruments FLSP 920 spectrometer equipped with double monochromators for both excitation and emission, operating in right angle geometry mode. The fluorescence quantum yields were measured using a calibrated integrating sphere (150 mm inner diameter). Lifetime measurements were conducted using the time-correlated single-photon counting method (TCSPC) on the FLSP 920 spectrometer equipped with a high-speed photomultiplier tube positioned after a single emission monochromator. Decays were recorded to 10 000 counts in the peak channel with a record length of at least 1000 channels. The quality of all decay fits was judged to be satisfactory, based on the calculated values of the reduced χ2 and Durbin–Watson parameters and visual inspection of the weighted and autocorrelated residuals. The lifetimes of 1 in polar solvents were not recorded as the emissions were too weak. All absorption and emission spectra were recorded in standard quartz cuvettes (1 cm × 1 cm) under argon.
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5

Characterization of Organic Compounds

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All the chemicals, reagents, oligos (dA20, dT20, dA10, dT10, dG10, dC10 and d(AATT)5), control probes (Hoechst 33258, ethidium bromide and propidium iodide), primary antibody, Alexa A488-coupled secondary antibody, DNase I and RNase were purchased from Sigma-Aldrich. 1H and 13C-NMR spectra were recorded on a Bruker AV-400 MHz spectrometer with chemical shifts reported as parts per million (ppm)(in CDCl3/DMSO-d6, tetramethylsilane as an internal standard) at 20 °C. UV-vis absorption and emission spectra were measured in quartz cuvettes of 1 cm path length. The absolute fluorescence quantum yields were determined using an integrating sphere for the samples on FLSP920 spectrometer (Edinburgh Instruments). High resolution Mass spectra (HRMS) were obtained on Agilent Technologies 6538 UHD Accurate-Mass Q-TOF LC/MS spectrometer.
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6

Characterization of Perovskite Thin Films

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Fourier transform infrared (FT-IR) spectroscopy measurements were conducted on a Fourier transform infrared spectrometer (model: IRPrestige-21, range 4000–1000 cm−1). Ultraviolet-visible (UV-vis) absorption measurements were measured on a Lamba 35 spectrophotometer (Perkin-Elmer, Waltham, MA, USA). The X-ray diffraction (XRD) patterns of the films were obtained by a Bruker D8 ADVANCE X-ray diffractometer (Bruker Corp, Berlin, Germany) under the operation conditions of 40 kV and 40 mA. The morphology of perovskite films was obtained by field emission scanning electron microscopy (FESEM, S4800 microscope, Hitachi Ltd., Tokyo, Japan). The transient-state photoluminescence (PL) was measure by FLSP920 spectrometer (Edinburgh Instruments Ltd., Livingston, UK). H nuclear magnetic resonance (NMR) spectra were collected by using Bruker DELL PC1 equipment. X-ray photoelectron spectroscopy (XPS) was studied using a PHI Quantera SXM (ULVAC-PHI Inc., Tokyo, Japan). The current density-voltage (J-V) curves of the devices were measured by a Keithley 2400 Source Meter under an illumination of 1 sun (100 mW/cm2 AM 1.5 G, generated by a solar simulator Oriel Sol3A, Newport Corp., Irvine, CA, USA), which was calibrated with a standard Si photodiode. The active area was 0.096 cm2.
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7

Fluorescence Lifetime Measurements with TCSPC

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Fluorescence lifetime measurements were performed on a Horiba Delta Flex time-correlated single photon counting (TCSPC) instrument. A 560 nm nano-LED with a pulse repetition rate of 1 MHz was used as the light source. The instrument response function (IRF) was collected using a scatterer (Ludox AS40 colloidal silica). Fluorescence lifetime (λexc = 560 nm) and gated emission was measured on FLSP920 spectrometer, Edinburgh Instruments equipped with a micro flash lamp (µF2) set-up. From the measured decay traces, the data were fitted with a multi-exponential decay, and χ2 was less than 1.1.
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8

Fluorescence Quantum Yield Measurement

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Fluorescence quantum yields of the samples were measured using a calibrated integrating sphere (150 mm inner diameter) from Edinburgh Instruments combined with the FLSP920 spectrometer described above. For solution-state measurements, the longest wavelength absorption maximum of the compound in the respective solvent was chosen for the excitation. In order to avoid self-absorption, the emission spectra were measured with dilute samples (ca. 0.1 OD at the excitation wavelength).
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9

Comprehensive Characterization of Upconversion Materials

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Powder X-ray diffraction (XRD) was performed on a Rigaku Smartlab diffractometer with Cu Kα radiation at a scanning rate of 10° min−1. Scanning electron microscope (SEM, FEI Quanta 400F) and transmission electron microscope (TEM, FEI Tecnai G2 F30) were employed for the observation of the morphology. Energy dispersive X-ray spectroscopy (EDS) data were obtained using the SEM equipped with the energy dispersive X-ray spectrometer. TEM images, high-resolution TEM (HRTEM) images and selected-area electron diffraction (SAED) patterns were performed at an accelerating voltage of 300 kV. Fourier transform infrared (FTIR) spectra were obtained in transmission mode on a Bruker Equinox 55 FTIR spectrometer with the samples sandwiched between two KBr plates. Photoluminescence excitation and emission spectra were recorded on an Edinburgh FLSP920 spectrometer equipped with a 980 nm diode laser, a 450 W continuous xenon lamp and a 60 W microsecond flash lamp as excitation sources and a R928 red-sensitive photomultiplier tube as detector. The samples were annealed at 500 °C for 1 h prior to upconversion luminescence measurements. All the measurements were performed at room temperature except for the thermometric upconversion photoluminescence.
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10

Steady-State and Time-Resolved Luminescence Measurements

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The steady-state and time-resolved luminescence measurements were performed with an Edinburgh Instruments FLSP920 spectrometer setup, using a 450 W xenon lamp as the steady-state excitation source and an EPLED as the timeresolved excitation source with a fixed excitation wavelength of 331 nm. The emission was detected with a Hamamatsu R928P photomultiplier tube (PMT). Excitation spectra were corrected for the xenon lamp emission profile, whereas emission spectra were corrected for the detector response curve. All measurements were carried out at a step size of 1 nm.
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