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We introduce a new idea, referred to as a multiple-cell cavity, which provides various benefits including a larger detection volume, simpler experimental setup, and easier phase-matching mechanism.
Experimental results on the first pcDD showed an ion rate limitation, caused by the increase in the detector time constant (because of the larger detection area), and a low S/N ratio, due to the specific reduced signal associated with low Charge Collection Efficiency (CCE) of pc diamond.
It was found that in heterocyclic compounds, the most stable binding site for Hg2+ is N atom instead of S atom, although the S atom may be kinetically favored due to the lower spatial hindrance, larger detection radius with longer Hg2+ S bond length, and closer softness between Hg2+ and S groups.
More specifically, a larger value of leads to better rejection capabilities of the side lobe signals and the larger detection loss for matched signals.
Here, we observe a similar situation to the previous plot, except that the LTD has a larger detection loss relative to the WMF and ANMF.
Their results are consistent with a high sensitivity at 200°C; nevertheless, this material, in most cases, has larger detection and recovery times.
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This image shows a simulation for elastic collisions between NO and Ne, assuming an isotropic DCS and an infinitely large detection volume, i.e., all scattered molecules are detected with equal efficiency.
The ultra-high sensitivity, the large detection area, and the simple detection scheme of random lasers allow us to detect prefailure damage in bone at very small strains before any microscale damage occurs.
All ceramic microdevices have revealed high output signal and large detection range.
It was designed to be assembled in array to cover large detection area.
The magnets of large detection depth mode can be obtained by combining the magnets of mobile mode with additional magnets.
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