1988
DOI: 10.1088/0022-3735/21/3/005
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The retrieval of low current pulses from noise for attachment measurements in weakly attaching gases

Abstract: Describes the use of a digital storage oscilloscope linked to a microprocessor via a GPIB digital interface for the improvement of the signal-to-random-noise ratio of low-level ( approximately 10-10 A) repetitive current waveforms obtained from drift tubes. The analysis of such signals allows attachment coefficient to be calculated for very weakly attaching gas mixtures.

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Cited by 3 publications
(3 citation statements)
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“…More recently, Woo et al have studied trichloroethene in detail using much higher-resolution photoionisation studies [8,9], while resonanceenhanced multi-photon ionisation spectra for both molecules have been reported by Williams and Cool [10,11]. Multi-photon ionisation spectra for tetrachloroethene have been published by Heath and Robins and Duttont et al [12,13]. The photoabsorption spectrum of trichloroethene has been studied by Walsh and Warsop [14], and the electron energy loss spectra of both molecules has been published by Koerting et al [15].…”
Section: Introductionmentioning
confidence: 99%
“…More recently, Woo et al have studied trichloroethene in detail using much higher-resolution photoionisation studies [8,9], while resonanceenhanced multi-photon ionisation spectra for both molecules have been reported by Williams and Cool [10,11]. Multi-photon ionisation spectra for tetrachloroethene have been published by Heath and Robins and Duttont et al [12,13]. The photoabsorption spectrum of trichloroethene has been studied by Walsh and Warsop [14], and the electron energy loss spectra of both molecules has been published by Koerting et al [15].…”
Section: Introductionmentioning
confidence: 99%
“…For each pulse of photo-electrons the current transient at the collector thus consisted of an initial pulse due to unattached electrons followed by a slower negative ion pulse due to negative ions formed in the attachment process. Successive current transients for the same experimental conditions were passed to a low-noise amplifier and converted into voltage transients, which were signal averaged by a digital waveform recording system, comprising a digital storage oscilloscope, microprocessor and ancillary devices interlinked by a GPIB (IEEE-488) digital interface [ 3 ] . This technique of signal averaging differed from methods employed in other experiments in that the whole current transient was recorded for each pulse.…”
mentioning
confidence: 99%
“…The drift tube was then re-evacuated and the procedure repeated for different gas number densities. For a particular value of E / N and N , calculation of the areas under the electron ( A , ) and negative ion (Ai) pulses from the measured current transients enabled attachment coefficients to be determined [4,5], where a = -1n 1 (T). A , +Ai d 0022-37271871101322 + 02 $02.50 @ 1987 IOP Publishing Ltd ), Lakshminarasimha and co-workers (+) and those calculated by Hayashi (-).…”
mentioning
confidence: 99%