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Variation of each parameter by ±2% did not have a significant effect on the detector response.
The detector thus permits simultaneous photometric and conductometric detection in the same place of the capillary, while exchanging of the separation capillary is easy and without effect on the detector geometry and performance.
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In this paper we will discuss the spatial detector response focusing on the effects of the detector design.
As described above, the pulse length does not have an effect on the expected detector response shape as the pulse length is a lot longer than the ToF of photons scattering in the objects.
In this paper, we present an experimental study on the improvement of the sensitivity with this new compact matrix, and a characterisation of its effects on the overall detector performance.
This intensity scaling has no effect on the Laplacian of Gaussian detector, since the detector is only sensitive to the local image contrast gradient (Fig. 1a).
Variation of the flow rates from 0.5 to 3.0 ml/min has no effect on the performance of the detector.
To study the effects of doping on the detector characteristics, we varied (a) the relative position of the δ-doping layer with respect to the QD plane, (b) the distance between the δ-doping layer and the QD plane, and (c) the doping level.
The effect that the detector has on a traversing beam's macroscopic dose deposition was determined as being a mean reduction in dose of (1.44 ± 0.15) % for depths in water between 5 and 35 mm.
Thus, the negative effect of the nonstationary texture on the detector can be effectively eliminated.
This paper examines such effects on the detection performance of the CC detector.
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