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The distance between elements of the ULA array is assumed to be, where is the carrier wavelength.
In the initial setup, each antenna comprising the array is assumed to be an isotropic radiator (three dimensions).
In this study, a uniform linear microphone array is assumed, where the coordinates of the elements are denoted by (see Figure 3) and is the number of microphones.
The total width of the array is assumed to be W = n ⋅ (a + b), where n is the number of wires.
A cuboidal array is assumed for convenient analysis, and the results in this section can be easily applied to the uniform linear array (ULA)s or UPAs which are placed on arbitrary 1D line or 2D plane in the space.
The signal intensity that we measure on the array is assumed to be proportional to the ratio of bound-to-total surface of the peptide spot, S i.
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Due to short distances, the communication over the first hop (i.e., from main transmitter to elements of the distributed array) was assumed to be costless in terms of transmission power and radio resource usage.
Laplacian noise and the changes along the probe array are assumed to be sparse.
Both of the arrays are assumed symmetric around the origin.
The transmit and receive arrays are assumed to be distantly separated.
Angle of ULAs in the L-shape and V-shape arrays are assumed 90° and 120°, respectively.
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