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To evaluate the proposed system, measurements were performed in a room with T 60=0.16 s using the setup illustrated in Fig. 3.
To test the performance of our double-layer grating as a sensor, we simultaneously measured the 0th-order and 1st-order powers in transmission through the grating and substrate using the setup illustrated in Figure 2 at a wavelength of λ = 1,565 nm.
Measurements of the sensing ability of the grating were performed using the setup illustrated in Figure 2. The sample was held on a glass plate in the xy-plane of the table, while the transmission through the grating was detected by two InGaAs detectors arranged to detect the 0th-order (I0) and 1st-order (I1) power.
The measurements were conducted using the setup illustrated in Fig. 4. Firstly, the influence of the stitching pattern ('M' and 'V') was evaluated.
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For this purpose, we used the procedure detailed by ETSI in [56] and the setup illustrated in Fig. 18.
To verify this LC mode, we use the experimental setup illustrated in Fig. 3b and compare with simulations from the combined FEM-Jones approach.
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Use the setup in the picture for the previous step.
We used the GFP-tailswap haploid inducer (Ravi and Chan, 2010; Ravi et al., 2014) in the experimental setup illustrated in Figure 1.
The used setup is illustrated in Fig. 5 and experiments were conducted on concrete test blocks containing various man-made defects to simulate natural ones.
All MD simulations were performed using the following setup.
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