The design and fabrication of high frequency single element ultrasonic transducers present a multitude of challenges for the transducer engineer, from size constraints to electrical impedance matching. This paper discusses the trade-offs involved in procedures used to fabricate lithium niobate (LiNbO/sub 3/) and lead titanate (PbTiO/sub 3/) transducers in the 25 MHz to 75 MHz range. Transducers of varying dimensions were built according to an f-number range of 2-3.5. Desired focal depths were achieved with use of either an acoustic lens or a spherically focused piezoceramic. Silver epoxy backing with an acoustic impedance of approximately 5.9 MRayls was used in all designs. All transducers were designed around a 50/spl Omega/ send and receive circuit. Electrical tuning of the transducer to the receive circuitry was achieved by using an RF transformer and/or a length of coaxial cable. All transducers were tested in a pulse-echo arrangement using a Panametrics 5900PR pulser, a Wavetek function generator and a LeCroy digital oscilloscope. The bandwidth, insertion loss, and depth of focus were measured. Numerous transducers were fabricated with -6 dB bandwidths ranging from 40% to 74%, and two-way insertion loss values ranging from -14 dB to -28 dB.
[1]
K. Shung,et al.
Medical imaging arrays for frequencies above 25 MHz
,
1999,
1999 IEEE Ultrasonics Symposium. Proceedings. International Symposium (Cat. No.99CH37027).
[2]
K. Kirk Shung,et al.
Passive materials for high-frequency ultrasound transducers
,
1999,
Medical Imaging.
[3]
F. Foster,et al.
Fabrication of high frequency spherically shaped ceramic transducers
,
1994,
IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.
[4]
K. Shung,et al.
Piezoceramics for high-frequency (20 to 100 MHz) single-element imaging transducers
,
1997
.
[5]
Benjamin M. W. Tsui,et al.
Principles of Medical Imaging
,
1992
.