2000
DOI: 10.1021/jp0010379
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Absolute O2(aΔ) Concentration Measurement in Singlet Oxygen Generator by Using the Piston Source Method

Abstract: A calibrated piston source of light, which simulates a cylindrical-volume luminosity source, has been used to measure the absolute concentration of O2(a1Δ). It is proved that this piston source method is one of the simplest and most convenient ways to measure the O2(a1Δ) concentration in a singlet oxygen generator, especially in real time measurements. Discussions about the method and the results are also given.

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Cited by 9 publications
(4 citation statements)
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“…This pressure was chosen to reduce the residence time and, hence, the wall quenching of 1 O 2 inside the cold traps, gas tubing, and emission cell, so that maximum emission intensity could be detected. The emission detection system consists of a 5 nm bandwidth interference filter centered at 1270 nm (Andover, blocked to 1.55 μm), an optical chopper (SRS model SR540), a thermo-electrically cooled InGaAs photodetector (Newport model 71887 detector and 77055 TE-cooler controller), and a digital dual phase lock-in amplifier (SRS model SR830). ,, 1 O 2 emission from the emission cell was collected by a plano-convex BK7 lens (ThorLabs LA1805, f = 30 mm), passed through the optical chopper and the interference filter. The chopped emission was focused by another plano-convex BK7 lens (ThorLabs, LA1131, f = 50 mm, AR coated for 1050−1620 nm) into the InGaAs detector, and the signal was measured by the lock-in amplifier.…”
Section: Methodsmentioning
confidence: 99%
“…This pressure was chosen to reduce the residence time and, hence, the wall quenching of 1 O 2 inside the cold traps, gas tubing, and emission cell, so that maximum emission intensity could be detected. The emission detection system consists of a 5 nm bandwidth interference filter centered at 1270 nm (Andover, blocked to 1.55 μm), an optical chopper (SRS model SR540), a thermo-electrically cooled InGaAs photodetector (Newport model 71887 detector and 77055 TE-cooler controller), and a digital dual phase lock-in amplifier (SRS model SR830). ,, 1 O 2 emission from the emission cell was collected by a plano-convex BK7 lens (ThorLabs LA1805, f = 30 mm), passed through the optical chopper and the interference filter. The chopped emission was focused by another plano-convex BK7 lens (ThorLabs, LA1131, f = 50 mm, AR coated for 1050−1620 nm) into the InGaAs detector, and the signal was measured by the lock-in amplifier.…”
Section: Methodsmentioning
confidence: 99%
“…The absolute concentrations of O 2 (a 1 ∆ g ), O 2 (b 1 Σ g ), and O( 3 P) were not determined using emission detection in the present experiment, but such a discharge typically produces 2.5-9% O 2 (a 1 ∆ g ), 10 -3 -10 -2 % O 2 (b 1 Σ g ), and 10 -4 % O( 3 P). 42,43 We calculated the deactivation of 1 O 2 (a 1 ∆ g ) due to self-quenching and collisional quenching by the wall and gaseous species 44,45 in the downstream tubing. The overall quenching rate is ∼0.05 s -1 , and the travel time of 1 O 2 (a 1 ∆ g ) downstream is <50 ms; thus the deactivation of 1 O 2 ( 1 ∆ g ) during its residence time in the system is <0.3%.…”
Section: Experimental Details a Instrument And Operating Conditionsmentioning
confidence: 99%
“…Freshwater discharge to the Arctic Basin impacts ocean salinity as well as marine processes including sea ice formation and thermohaline circulation. Oceanographers typically define freshwater as the amount of zero salinity water contained in a volume compared to a reference salinity; Arctic Ocean freshwater budgets have been computed and updated since Aagaard and Carmack (1989).…”
Section: Introductionmentioning
confidence: 99%