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Cary 500 spectrometer

Manufactured by Agilent Technologies
Sourced in United States

The Cary 500 spectrometer is a versatile laboratory instrument designed for accurate and reliable absorbance and reflectance measurements across a wide spectral range. The core function of the Cary 500 is to provide precise spectroscopic data for various applications.

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7 protocols using cary 500 spectrometer

1

Characterization of Cobalt Oxysulfide Micro-Cages

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An FEI Nova NanoSEM 200 was used to investigate the micro-cage structure of cobalt oxysulfide. The crystal lattices and chemical composition of the material were studied under a JEOL JEM-F200 transmission electron microscopy (TEM) with an energy-dispersive X-ray spectroscopy (EDS) detector equipped (accelerating voltage of 200 kV). X-ray diffraction (XRD) measurements were conducted on a Bruker D4 ENDEAVOR with a monochromatic Cu Kα radiation source (λ = 0.154 nm) equipped. X-ray photoelectron spectroscopy (XPS) was performed on a Krato AXIS Supra XPS (dual Al/Ag monochromatic X-ray source equipped) using Al Kα X-rays at 1486.7 eV. The measured XPS spectra were analyzed using CasaXPS (version 2.3.24). The material optical absorption property was investigated using a Cary 500 spectrometer, in which the UV-Vis-NIR spectra were measured on a drop-casted material sample upon a glass substrate. A HORIBA LabRAM HR Evolution was utilized to study the Raman spectra of cobalt oxysulfide with the excitation wavelength of 532 nm.
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2

Transient Absorption Spectroscopy Characterization

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Solution UV-VIS linear absorption spectra were collected with a Cary 500 spectrometer. Film UV-VIS linear absorption spectra were acquired with a Varian Cary-6000i equipped with an integrating sphere. For films, the absorbance was calculated as A = –log10(R + T). Transient absorption datasets were acquired using a Coherent Libra Ti:sapphire laser, with an output of 800 nm at 1 kHz. A TOPAS-C OPA was used to generate the ∼150 fs pump pulse (center wavelength 530–650 nm). A small amount of 800 nm light was used to pump a CaF2 crystal to generate 330–850 nm probe light for UV-VIS TA or a 1 cm thick sapphire crystal to generate 750–1640 nm probe light for NIR TA. A second TOPAS-C OPA was used to generate ∼150 fs 5–6 μm probe pulses for MIR TA. The instrument response function was ∼150–250 fs depending on the probe wavelength. A Janis VPF 100 Cryostat was used for all TA measurements under vacuum. A solution cell was assembled with an o-ring and sapphire windows in a glovebox for measurements with solvent and electrolyte present. All datasets were analyzed using Surface Xplorer software. Charge injection yields were determined by comparing the maximum signal of a Z907/TiO2 sample to the maximum signal of an acene/TiO2 sample of interest under identical excitation conditions.
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3

Photophysical Characterization of Samples

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UV-vis absorptions were measured using a Varian Cary 500 spectrometer (Varian, USA). Steady-state PL was measured using an Edinburgh Instruments FLS920P fluorescence spectrometer, and for PL life time measurement [time-correlated single-photon counting (TCSPC)], a picosecond pulse diode laser (EPL-405; excitation wavelength, 405 nm; pulse width, 49 ps) was used.
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4

Spectroscopic Characterization of Advanced Optoelectronic Materials

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All absorption data was taken on a Varian Cary 500 spectrometer. Rhodamine 6G emission measurements were taken on a Horiba Scientific Fluorolog spectrofluorimeter using a monochromated Xe lamp as the excitation source. CEP blend film and Stilbene-420 emission spectra were taken on a LaserStrobe spectrometer from Photon Technology International using a GL-3300 nitrogen laser and GL-302 dye laser attachment, also from Photon Technology International. Upconverted emission spectra were measured with the emission filtered by a 500 nm short-pass filter from Thorlabs, model FES0500, to prevent reflected excitation light from interfering with the measured emission signal. Laser power was measured with a 919P-003-10 thermopile sensor from Newport. Time-Resolved Single Photon Counting Data (in Extended Data section) was taken using excitation light generated by a Fianium SC400 supercontinuum fibre laser with wavelength selected by a Fianium AOTF system. Detection was measured via a photomultiplier tube connected to a Becker-Hickl SPC-130 system. All data was collected with signal count rate at <2% of excitation rep rate to ensure proper TCSPC statistics. All spectra were corrected for the spectral responsivities of the systems used for data collection.
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5

Optoelectronic Characterization of Materials

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UV–Vis absorptions were measured using Varian Cary 500 spectrometer (Varian USA). Photoluminescence lifetime (TCSPC) was measured using an Edinburgh Instruments lifespec II fluorescence spectrometer; a picosecond pulse diode laser (EPL-510, excitation wavelength 510 nm, pulse width <60 ps, fluence <3 nJ/cm2) was used. Photoluminescence spectral photon flux was measured using an Andor Kymera 193i spectrograph and a 660 nm continuous-wave laser set at 1-Sun equivalent photon flux (1.1 µm beam full-width half-maximum, 632 µW); photoluminescence was collected at normal incidence using a 0.1 NA, 110 µm-diameter optical fiber.
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6

Optoelectronic Characterization of Large-Area Perovskite Films

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UV–vis absorptions were measured using Varian Cary 500 spectrometer (Varian USA). Photoluminescence lifetime (TCSPC) was measured using an Edinburgh Instruments life spec II fluorescence spectrometer; a picosecond pulsed diode laser (EPL-510, excitation wavelength 510 nm, pulse width <60 ps, fluence < 3 nJ/cm2) was used. Photoluminescence spectral photon flux was measured using an Andor Kymera 193i spectrograph and a 660 nm continuous-wave laser set at 1-Sun equivalent photon flux (1.1 µm beam full-width half-maximum, 632 µW); photoluminescence was collected at normal incidence using a 0.1 NA, 110 µm-diameter optical fiber. UV–vis measurement for the large area perovskite films (10 cm × 10 cm) was measured with a BLACK-Comet UV–vis Spectrometer.
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7

Synthesis of 2D SnS2 Flakes

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Subsequently, the solution was heated to 280 o C within 15 min with a vigorous stir (700 rpm).
Sulfide powder (1 mM) was dispersed into 5 mL oleylamine (OAm, >90.0%, Sigma Aldrich) to produce the sulfide precursor which was subsequently injected into the reaction system. The reaction was maintained at 280 o C for 30 min. After cooling the solution to room temperature, the 2D SnS 2 flakes (in powder form) were collected and separated from the solution by centrifugation.
The powder was further washed two times by ethanol and hexane (1/1, V/V) and finally dispersed in ethanol. The powder was stable in air without further protection for characterizations. were examined using a Varian Cary 500 spectrometer in dual beam mode using quartz cuvettes. PL spectroscopy was carried out on a Princeton Instruments SP2500i with a PIXIS100 ExCelon CCD camera detector using a Monochromatic 532 nm laser delivering approximately 200 µW average power to the sample.
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