Emission spectra were measured on a PTI Quantamaster emission spectrometer equipped with a Hamamatsu R550942 near-infrared photomultiplier tube behind a 1000 nm long pass filter. Emission and excitation spectra were corrected for nonlinearities in lamp output and detector response. The longest wavelength in the excitation spectrum that maximized emission at 1276 nm was selected for the excitation wavelength. The emission spectra were collected over 1200–1350 nm and integrated with baseline correction. The values were generally reproducible within ±5%.
R5509 42
The R5509-42 is a near-infrared photomultiplier tube (PMT) developed by Hamamatsu Photonics. It is designed to detect light in the wavelength range of 900 to 1700 nanometers. The R5509-42 features a large photocathode area and high sensitivity, making it suitable for various applications that require detection of low-level near-infrared signals.
Lab products found in correlation
13 protocols using r5509 42
Singlet Oxygen Quantum Yield Determination
Emission spectra were measured on a PTI Quantamaster emission spectrometer equipped with a Hamamatsu R550942 near-infrared photomultiplier tube behind a 1000 nm long pass filter. Emission and excitation spectra were corrected for nonlinearities in lamp output and detector response. The longest wavelength in the excitation spectrum that maximized emission at 1276 nm was selected for the excitation wavelength. The emission spectra were collected over 1200–1350 nm and integrated with baseline correction. The values were generally reproducible within ±5%.
Singlet oxygen emission measurement
Singlet Oxygen Photophysical Characterization
Singlet oxygen decay curves were monitored using a photo detector (Spectra-Physics, CA, USA). The excitation wavelength was 585 nm. Emission was detected using a photomultiplier (R5509-42, Hamamatsu Photonics K.K., Hamamatsu, Japan) combined with a monochrometer (HR-320, Jobin Yvon, France). Data were stored in a multichannel scaler (SR430, Stanford Research Systems, CA, USA). All measurements were performed at 22°C. The absorption spectra were measured before and after decay measurements to monitor the photobleaching of the dye.
Singlet Oxygen Emission Sensitized by Complexes
Singlet Oxygen Quantum Yield Determination
Singlet Oxygen Quantum Yield Determination
Photophysical Characterization of Photosensitizers
Singlet oxygen quantum yields (ΦΔ) were also estimated using eqn (1) with [Ru(bpy)3](PF6)2 as the standard (ΦΔ = 0.57 in aerated MeCN).75 (link) Absorption spectra were recorded using a Jasco V-530 spectrophotometer, and luminescence spectra were collected using a PTI Quantamaster equipped with a standard photomultiplier tube (K170B) and a Hamamatsu R5509-42 photomultiplier tube for NIR detection (<1400 nm). Luminescence lifetimes were measured using a PTI LaserStrobe system incorporating a nitrogen-dye laser (GL-3300/GL-301) integrated with an R928 stroboscopic detector. Emission was also probed by gated methods using a pulsed xenon flash lamp and gated detector. Exponential curve fitting and corrections to the wavelength-dependence of lamp output and detector response were done with PTI Felix32 software.
Singlet Oxygen Phosphorescence Measurement
at an emission wavelength of 1270 nm with a Horiba-Jobin-Ivon SPEX
Fluorolog 3.22 spectrofluorimeter using a Hamamatsu R5509-42 photomultiplier
cooled with liquid nitrogen. A Schott RG1000 filter, to eliminate
all of the first-harmonic contributions of the sensitizer emission
in the region below 850 m, from the IR signal, was used. The singlet
oxygen formation quantum yield was subsequently determined by direct
measurement of the phosphorescence signal at 1270 nm, Emission1270 nm (in
MeCN. The standard used was 1H-phenal-1-one in MeCN
(ϕΔ= 0.98),55 (link) and
using
oxygen formation quantum yield of our compounds was obtained. where ϕΔref stands for the singlet oxygen formation
quantum yield of the reference compound.
Singlet Oxygen Quantum Yield Measurement
Absorption and Emission Spectroscopy
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