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Lateral sensitivity was characterized using a microfabricated silicon cantilever force sensor.
This test was an important benchmark for designing a larger array with an improved lateral sensitivity and statistical accuracy.
Here, Slat is the lateral sensitivity of the cantilever defined as Slat = PHSnorm/aR*L[36], where P is a proportionality factor (≈2.5 for the triangular cantilever), Snorm is the vertical deflection sensitivity of the cantilever, a is the amplification factor of the lateral signal measured, and R* is the ratio of the beam height to the beam width (R* = 0.5) [36].
The most important performance parameters related to any given gamma detection probe system are generally thought to be: (1) overall sensitivity (i.e., efficiency); (2) spatial selectivity (i.e., radial sensitivity distribution); (3) spatial resolution (i.e., lateral sensitivity distribution); (4) energy resolution (i.e., spectral discrimination); and (5) contrast [ 46].
Similarly, lateral sensitivity (A ix + A iy)1/2 = D r/(2 EI) should be the same for different cavities as in Eq. (9); however, our experimental values are 43.2nm/mN, 35.0nm/mN, and 33.1nm/mN for the first, second, and third FP cavities, respectively.
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Experimental data confirm lateral displacement sensitivity of 2.32 mV/μm.V.
In this context, a possible role for DAergic signaling is in the gating of lateral line sensitivity during motor behavior.
The difference in the lateral force sensitivities might be the result of the asymmetry in mechanical property of our FS, as well as the misalignment of the fibers.
Besides high sensitivity, lateral actuated MEMS sensor reveals better parameter reproducibility and tight control of both: electrical and mechanical characteristics.
The influence of various design parameters on the lateral resolution and sensitivity of the measurements is investigated.
In a way, lateral and depth sensitivity are separated, being the former encoded in the detector position, and the latter in the time gate t G. Furthermore, depth information is reached just by increasing t G, without changing source-detector position, thus keeping exactly the same collection efficiency.
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