Fig. 2. Photoacoustic measurement configuration for K-wave toolbox simulation. The inset: sectional image of the absorbing sphere. (b) Spatial photoacoustic spectra for 3 mm and 1.5 mm diameter absorbing spheres in (a) simulated by K-wave toolbox.
Fig. 5. Variation of SNRs for photoacoustic signals from a 3 mm absorbing sphere to the upper frequency values of (a) the rectangular filter in time-domain photoacoustic measurement and (b) the matched filtered chirp with a rectangular filter in frequency-domain photoacoustic measurement.
Fig. 6. Variation of SNRs for photoacoustic signals from a 1.5 mm absorbing sphere to the upper frequency values of (a) the rectangular filter in time-domain photoacoustic measurement and (b) the matched filtered chirp with a rectangular filter in frequency-domain photoacoustic measurement.
Fig. 1. (a) Simulated ultrasound transducer’s transfer function from the simple modeling of Eq. (14). (b) Spectra of matched filtered chirp and Rect function filtering in frequency- and time-domain photoacoustic measurements, respectively.
Fig. 3. (a) Time-domain and (b) frequency-domain photoacoustic SNRs calculated based on brute-force simulations and the theoretical equation, which are indicated as superscripts, b1, b2, and t in the legends.
Fig. 4. (a) Frequency-domain photoacoustic signal’s SNR improved by additionally filtering off the DC terms in the matched filtered chirp spectrum. (b) Comparison of SNRs between time- and frequency-domain photoacoustic measurements before and after additionally applying a rectangular (Rect) filter to matched filtered chirp.
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