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Measurements were obtained with precision of ±0.01 or better for tetrachloroethylene (PCE) in a 2.5 cm thick glass-bead porous medium using a counting time of 1 s.
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Using a count cutoff of at least 2 times the number of time points available for that individual, alleles at a SNP were called as either present or absent in that individual for a given SNP.
Data was collected at room temperature using a variable count time scheme (Supporting Information, Table S6).
Data was collected at room temperature using a variable count time scheme (Table S5 of the Supporting Information).
Scans were taken with a 2θ and a counting time of 1.0 s using a Cu-Kα radiation source (λ = 1.542 Å) and a nickel filter.
Picosecond-resolved spectroscopic studies were carried out using a commercial time correlated single photon counting (TCSPC) setup from Edinburgh Instruments (instrument response function, IRF = 80 ps, excitation at 375 nm).
The time-resolved fluorescence measurements were carried out using a time correlated single photon counting (TCSPC) system (Horiba Jobin-Yvon) at room temperature.
Fluorescence decay times were determined using a time-correlated single photon counting technique on a Fluorolog3 spectrometer equipped with a NanoLED 455 nm laser diode.
Method 2 is also used to calculate the EPT, where consumption is analysed using a real-time sequence instead of counting the total energy consumption over its lifetime.
Hourly emissions for road traffic were created using a time series of normalised traffic counts, taken from 37 automatic sites in London.
The light emission rate manipulation experiment was set up using a time-correlated single-photon counting system [45], and the normalized time-resolved PL spectra are shown in Figure 4.
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