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1 September 2010 Feasibility of noncontact piezoelectric detection of photoacoustic signals in tissue-mimicking phantoms
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The feasibility of air-coupled ultrasound transducers to detect laser-induced ultrasound from artificial blood vessels embedded in an optically scattering phantom is demonstrated. These air-coupled transducers allow new applications in biomedical photoacoustic imaging where contact with tissue is not preferred. One promising application of such transducers is the addition of photoacoustic imaging to the regular x-ray mammographic screening procedure.



Photoacoustic imaging is a novel imaging modality based on the use of laser-generated ultrasound by optically absorbing structures. Due to its ability to visualize increased hemoglobin concentrations, photoacoustic imaging is being explored as a noninvasive method to detect the vascularization of tumors.1, 2, 3, 4 Photoacoustic mammography (PAM)5, 6, 7 is a new approach in the detection of breast cancer that is based on laser-induced ultrasound originating from invasive tumors containing more hemoglobin than in normal tissue due to extensive neovascularisation.8

Detection of laser-induced ultrasound is in general carried out by using piezoelectric transducers in combination with an ultrasonic coupling medium to avoid the large acoustic impedance mismatch between tissue and air. The need for this coupling medium makes application of photoacoustic imaging more complicated in cases where direct contact with the tissue has to be avoided, or in cases where one wants to combine photoacoustic imaging with other imaging modalities. A promising example where photoacoustic imaging can add additional information to existing imaging techniques is mammographic breast cancer screening.

Although mammographic breast cancer screening is an undisputed factor in the reduction of breast cancer mortality, the way to screen9 (starting age, screening interval) and the negative side effects like false positive test results are still causing debates in scientific society.10 The appraisal of these negative side effects can differ strongly between countries, where recall rates can vary by a factor 10 with no clear effects on detection.11

Although considered very successful in screening, x-ray mammography is a far from perfect diagnostic modality. Even in a country like the Netherlands with extremely low recall rates (percentage of women called back for a diagnostic mammogram after the first x-ray screening), in every six recalls five are false positives,12, 13 which cause a lot of stress and unnecessary anxiety. Recall is attributed to the inherent weakness of the x-ray contrast mechanism, the lack of contrast between normal fibroglandular and malignant tissue, which radiologists in the screening have to cope with. Since the purpose of screenings is to find early-stage tumors before they cause symptoms in a normal and healthy population, radiologists are looking for these small and often subtle mammographic signs. None of the false-positive mammographic abnormalities show any degree of neovascularisation like invasive breast cancer.8

On the other hand, PAM has potentially the ability to detect increased vascularizations, and therefore PAM can assist the radiologist in the detection of these tumors.

Since we know that even large tumors can remain hidden from x-ray mammography in dense breast tissue, an increased photoacoustic signal due to increased hemoglobin concentrations in absence of any mammographic abnormality might trigger the radiologist to have a second look or a follow-up examination.

Combining photoacoustic imaging with x-ray screening of breast cancer will add additional information to this procedure. A combined x-ray and ultrasound system for therapy was developed by Novak, which shows that a combination of x-ray and ultrasound is feasible.14 A disadvantage of current detectors used in photoacoustic imaging is that they need to be in contact with the tissue directly or via an ultrasonic coupling medium (water, or gel), which makes integration in a standard x-ray screening procedure more complicated and more time consuming.

Attempts toward noncontact detection of laser-induced ultrasound that are reported in the literature were based on optical detection of tissue-surface displacement.15, 16 However, these systems put requirements on the tissue surface as well as stability of the entire detection system. A solution to this can be found in the use of air-coupled ultrasound transducers used for noncontact material characterization17, 18, 19 and biomedical applications such as burn-depth estimation.20 We hypothesize that when these transducers can be used to detect photoacoustic pressure transients, they can be integrated in an x-ray mammography system to obtain additional information, without any interference with the mammographic procedure or the resulting image quality. The obtained information can be very useful in obvious mammographic abnormalities, but also and especially when an abnormal photoacoustic signal is received in an apparently normal mammogram, thereby theoretically improving the sensitivity and specificity of the mammographic screening test.


Materials and Methods

In this study the feasibility of using air-coupled ultrasound (ACU) transducers to detect photoacoustic signals has been studied in tissue-mimicking phantoms.

An artificial blood vessel made of a silicon rubber tube with an inner diameter of 4mm was filled with human blood (anti-coagulated with EDTA). This artificial blood vessel was immersed in a 1% Intralipid-20% dilution with a reduced optical scattering coefficient of 0.14mm1 at a wavelength of 1064nm 21 and an optical absorption coefficient of 0.015mm1 . The vessel was positioned in a glass container and illuminated through the wall of the container, while detection was carried out above the fluid surface. Laser light at a wavelength of 1064nm was applied, as hemoglobin in blood has sufficient absorption at this wavelength to generate photoacoustic signals. A pulse energy of 200mJ /pulse (pulse-to-pulse stability better than 5%) was used with a repetition rate of 10Hz and a pulse duration of 10ns (Quanta Ray DCR-3, Spectra Physics, Newport Corporation, Irvine, California). The laser light had to travel over a distance of 35mm through the Intralipid suspension to reach the artificial blood vessel. The laser beam was expanded to illuminate an area of about 10cm2 , which resulted in an energy density at the interface of about 20mJcm2 . A schematic drawing of the setup is shown in Fig. 1 .

Fig. 1

Schematic drawing of the experimental setup: an artificial blood vessel with an internal diameter (ID) of 4mm is placed in a glass container filled with an Intralipid suspension. The artificial blood vessel was illuminated through the wall of the glass container, and the generated photoacoustic signals were detected with an air-coupled ultrasound transducer placed approx. 7.5mm above the Intralipid interface.


Laser-generated ultrasound originating from the artificial blood vessel and propagating through the Intralipid solution reaches the liquid/air interface. Due to the high acoustic impedance (Z) mismatch between the solution ( Z=1.6 MRayl) and the air ( Z=0.0004 MRayl), only a small fraction of acoustic energy (30dB) enters the air gap. This signal is detected by an unfocused air-coupled ultrasonic piezotransducer, which is supplied with a matching layer to reduce the impact of the high acoustic impedance mismatch between the transducer surface and the ambient air from 43dB to approximately 33dB . Two types of transducers have been used: one with sensor elements from the Murata Piezotite series (200kHz) , and one with Ferroperm (Kvistgaard, Denmark) Soft Piezoceramics and a polymer layer (1MHz) .19 The first type had a central frequency of 200kHz , 6-dB bandwidth of 50kHz , and an active diameter of 9mm . The second type had a central frequency of 1MHz , 6-dB bandwidth of 90kHz , and a 19-mm active diameter. The transducer transformed the acoustic signal into an electric signal, and the latter is amplified by 60dB using a homemade ultralow noise amplifier. The flatness of the amplifier response was better than 0.6dB in the frequency band of interest (200kHzto1MHz) .

The distance between the ultrasonic receiver and the Intralipid solution was approximately 7.5mm .

The nonprocessed time traces from the air-coupled transducers were digitized by a dual-channel oscilloscope ( 100MSamplessec , TDS-220, Tektronix, Beaverton, Oregon) and were stored on a laptop computer.



The photoacoustic time traces recorded by the noncontact transducers were averaged 512 times. The resulting averaged time traces are shown in Fig. 2 . The photoacoustic signal appears as a burst, with an onset occurring at a time of 42μs after the laser pulse. This value is in agreement with the expected time of flight: to reach the air-coupled transducer, the photoacoustic signal had to travel through 30mm of Intralipid suspension, which corresponds to a time delay of 20μs (the speed of sound in the 1%-Intralipid-20% suspension was measured to be 1495ms at 25°C ), and an air gap with a dimension of 7.5mm , which corresponds to a time delay of 22μs (assuming a speed of sound in air of 345ms at 25°C ).

Fig. 2

Photoacoustic time traces from an artificial blood vessel with an inner diameter of 4mm , recorded with air-coupled ultrasound transducers with a center frequency of 200kHz and 1MHz .


The quasi-equal signal levels of the measurements by the noncontact transducers with a different center frequency have a purely coincidental nature. The explanation is found in the intrinsic broad but nonflat frequency spectrum of the photoacoustic signal and the differences in sensitivity, bandwidth, and active surface of the transducers.

The signal-to-noise ratio (SNR), defined as the ratio of the rms value of the burst to the rms value of the noise, was 16.8 in the case of the 1-MHz transducer and 16.3 for the 200-kHz transducer. Assuming a SNR improvement of 512=22.6 , the original signal had a SNR of about 0.72, and at least two averages of the photoacoustic time traces (i.e., two laser pulses) are required to achieve a SNR of 1.

As can be observed in Fig. 2, the noise characteristics of the two sensors are different. This noise is mainly determined by the impedance characteristics of the piezoceramic in combination with the amplifier properties. Since the transducers used have a different design and operate in a different frequency domain, the noise characteristics are different.



To our knowledge, air-coupled ultrasound transducers have so far not been used to detect photoacoustic signals in biomedical applications, which can be attributed to the large acoustic mismatch at the tissue-air interface of about 4 orders of magnitude. This acoustic mismatch allows only a fraction (about 0.1 %) of the ultrasound to be transmitted to the air, which is not only a problem in industrial nondestructive testing (NDT) techniques18 but also in potential biomedical applications. Nevertheless, we have shown that the sensitivity of the air-coupled ultrasound transducers is sufficient to detect photoacoustic signals generated by an artificial blood vessel. These signals were detected at a distance of 7.5mm above the phantom interface, which in practice allows for noncontact scanning over a tissue surface in case an image has to be obtained. Larger distances are possible; however, significant signal losses due to acoustic energy absorption in air and wave divergence should be taken into account. While wave divergence is determined by the complex morphologic nature of the unknown source, the acoustic energy absorption can well be estimated. Typically, a 1-MHz wave experiences an attenuation of 1.6dB per cm in air.22

The attenuation expressed in decibels scales with about the frequency squared. This means that for the detection of higher frequencies, smaller air gaps have to be used. In this work, we have shown that signals with a frequency content up to 1MHz can be detected. This corresponds to photoacoustic sources with a diameter larger than 1.5mm ,23 which is already sufficiently small for mammographic breast cancer screening.

A drawback of the air-coupled transducers is the limitation on the frequency bandwidth, which determines the duration of the detected photoacoustic pressure burst. As is observed in Fig. 2, the duration of the detected ultrasound burst is about 12μs in the case of the 1-MHz transducer and 39μs in case of 200-kHz transducer, while in contact mode using a broadband transducer, a bipolar signal with a peak-to-peak time of 1.33μs would have been detected.23 This long burst length limits the axial resolution of the photoacoustic imaging system in the case of the 200-kHz transducer to 13mm and in the case of the 1-MHz transducer to 4mm . However, the latter might be improved by using signal processing algorithms such as deconvolution with the impulse response of the transducer. Furthermore, air-coupled transducers are subjects of permanent product improvement with bandwidth and sensitivity as main concerns.24

Since we demonstrated that air-coupled detection of photoacoustic signals from absorbers hidden in turbid media is feasible, this allows for integration of photoacoustic detection in the x-ray mammographic screening procedure without interfering with the standard screening procedure and image quality. During the time that the x-ray mammogram is being taken, the breast is illuminated with pulsed light and the air-coupled transducers can be used to detect the presence of malignant tissue by the presence of enlarged blood concentrations due to increased vascularization.

At this moment, the available air-coupled transducers are nonfocused, which makes obtaining an image complicated. However, combination of the signals of the various air-coupled transducers will enable a rough localization of the enlarged blood concentrations of T1 tumors (smaller than 2cm in diameter). Being able to predict the presence of these suspicious regions in one of the four quadrants of the breast will add useful information to the mammographic screening procedure.

Other research groups are working on the development of air-coupled arrays.25, 26 In the future, this might extend our proposed photoacoustic screening procedure to obtain a complete photoacoustic image of the breast.

In conclusion, we demonstrate the feasibility of air-coupled ultrasound transducers to detect photoacoustic signals in biomedical applications, which opens new possibilities of (combined) imaging with other modalities such as x-ray mammography. Besides application in photoacoustic mammographic screening, air-coupled detection of photoacoustic signals allows for a variety of applications, especially in situations where contact with the tissue via ultrasound matching gel is not desired, such as measurements on burn wounds.



R. I. Siphanto, K. K. Thumma, R. G. M. Kolkman, T. G. van Leeuwen, F. F. M. de Mul, J. W. van Neck, L. N. A. van Adrichem, and W. Steenbergen, “Serial noninvasive photoacoustic imaging of neovascularization in tumour angiogenesis,” Opt. Express, 13 89 –95 (2005). 1094-4087 Google Scholar


G. Ku, X. Wang, X. Xie, G. Stoica, and L. V. Wang, “Imaging of tumor angiogenesis in rat brains in vivo by photoacoustic tomography,” Appl. Opt., 44 770 –775 (2005). 0003-6935 Google Scholar


Y. Lao, Y. D. Xing, D. S. Yang, and L. Xiang, “Noninvasive photoacoustic imaging of the developing vasculature during early tumor growth,” Phys. Med. Biol., 53 4203 –4212 (2008). 0031-9155 Google Scholar


H. F. Zhang, K. Maslov, G. Stoica, and L. V. Wang, “Functional photoacoustic microscopy for high-resolution and noninvasive in vivo imaging,” Nat. Biotechnol., 24 848 –851 (2006). 1087-0156 Google Scholar


S. Manohar, S. E. Vaartjes, J. C. G. van Hespen, J. M. Klaase, F. M. van den Engh, W. Steenbergen, and T. G. van Leeuwen, “Initial results of in vivo non-invasive cancer imaging in the human breast using near-infrared photoacoustics,” Opt. Express, 15 12277 –12285 (2007). 1094-4087 Google Scholar


T. Khamapirad, P. M. Henrichs, K. Mehta, T. G. Miller, A. T. Yee, and A. A. Oraevsky, “Diagnostic imaging of breast cancer with LOIS: clinical feasibility,” Proc. SPIE, 5697 35 –44 (2005). 0277-786X Google Scholar


R. A. Kruger, K. D. Miller, H. E. Reynolds, W. L. Kiser Jr., D. R. Reinecke, and G. A. Kruger, “Breast cancer in vivo: contrast enhancement with thermoacoustic CT at 434MHz-feasibility study,” Radiology, 216 279 –283 (2000). 0033-8419 Google Scholar


P. Carmeliet and R. K. Jain, “Angiogenesis in cancer and other diseases,” Nature, 407 249 –257 (2000). 0028-0836 Google Scholar


“Screening for breast cancer: U.S. Preventive Services Task Force recommendation statement,” Ann. Intern Med., 151 (10), 716 –736 (2009). 0003-4819 Google Scholar


P. C. Gøtzsche and M. Nielsen, “Screening for breast cancer with mammography,” Cochrane Database System. Rev., 4 CD001877 (2009). Google Scholar


B. C. Yankaskas, C. N. Klabunde, R. Ancelle-Park, G. Renner, H. Wang, J. Fracheboud, G. Pou, and J. L. Bulliard, International Breast Cancer Screening Network, “International comparison of performance measures for screening mammography: can it be done?,” J. Med. Screen, 11 (4), 187 –93 (2004). 0969-1413 Google Scholar


J. H. Groenewoud, J. D. Otten, J. Fracheboud, G. Draisma, B. M. van Ineveld, R. Holland, A. L. Verbeek, and H. J. de Koning, “Cost-effectiveness of different reading and referral strategies in mammography screening in the Netherlands,” Breast Cancer Res. Treat, 102 211 –218 (2007). 0167-6806 Google Scholar


NETB (National Evaluation Team for Breast cancer screening in the Netherlands), LETB XII (2009) National Evaluation of Breast Cancer Screening in the Netherlands, 12 Department of Public Health, Eraxmus MC, Rotterdam (2009). Google Scholar


P. Novák, E. G. Moros, W. L. Straube, and R. J. Myerson, “SURLAS: a new clinical grade ultrasound system for sequential or concomitant thermoradiotherapy of superficial tumors: applicator description,” Med. Phys., 32 (1), 230 –240 (2005). 0094-2405 Google Scholar


B. P. Payne, V. Venugopalan, B. B. Mikić, and N. S. Nishioka, “Optoacoustic tomography using time-resolved interferometric detection of surface displacement,” J. Biomed. Opt., 8 (2), 273 –280 (2003). 1083-3668 Google Scholar


S. L. Jacques, P. E. Andersen, S. G. Hanson, and L. R. Lindvold, “Noncontact detection of laser-induced acoustic waves from buried absorbing objects using a dual-beam common-path interferometer,” Proc. SPIE, 3254 307 –318 (1998). 0277-786X Google Scholar


M. C. Bhardwaj, “Non-destructive evaluation,” Encyclopedia of Smart Materials, 690 –714 John Wiley and Sons, New York (2002). Google Scholar


E. Blomme, D. Bulcaen, and F. Declercq, “Air-coupled ultrasonic NDE: experiments in the frequency range 750kHz2MHz,” NDT & E Int., 35 417 –426 (2002). 0963-8695 Google Scholar


T. E. Gómez, “Acoustic impedance matching of piezoelectric transducers to the air,” IEEE Trans. Ultrason. Ferroelectr. Freq. Control, 51 624 –633 (2004). 0885-3010 Google Scholar


J. P. Jones, D. Lee, M. Bhardwaj, V. VanderKam, and B. Achauer, “Non-contact ultrasonic imaging for the evaluation of burn depth and other biomedical applications,” Acoust. Imaging, 23 89 –93 (1997). 0270-5117 Google Scholar


H. J. van Staveren, C. J. M. Moes, J. van Marle, M. J. C. van Gemert, and S. Prahl, “Light scattering in Intralipid-10% in the wavelength range of 4001100nm,” Appl. Opt., 30 4507 –4514 (1991). 0003-6935 Google Scholar


“Ultrasonic testing,” Nondestructive Testing Handbook, 320 –325 ASNT, Columbus, OH (1991). Google Scholar


R. G. M. Kolkman, J. H. G. M. Klaessens, E. Hondebrink, J. C. W. Hopman, F. F. M. de Mul, W. Steenbergen, J. M. Thijssen, and T. G. van Leeuwen, “Photoacoustic determination of blood vessel diameter,” Phys. Med. Biol., 49 4745 –4756 (2004). 0031-9155 Google Scholar


J. Kunkle, R. Vun, T. Eischeid, M. Langron, N. Bhardwaj, and M. Bhardwaj, “Phenomenal advancements in transducers and piezoelectric composites for non-contact ultrasound and other applications,” Fr.2.3.1 (2006). Google Scholar


A. I. Korobov, M. Y. Izosimova, and S. A. Toschov, “Development of ultrasound focusing array for air-coupled ultrasound generation,” Phys. Procedia, 3 201 –207 (2010). 1875-3892 Google Scholar


F. Blum, J. Jarzynski, and L. J. Jacobs, “A focused two-dimensional air-coupled ultrasonic array for non-contact generation,” NDT & E Int., 38 634 –642 (2005). 0963-8695 Google Scholar
©(2010) Society of Photo-Optical Instrumentation Engineers (SPIE)
Roy G.M. Kolkman, Erik Blomme, Tijl Cool, Mattias Bilcke, Ton G. van Leeuwen, Wiendelt Steenbergen, Kees A. Grimbergen, and Gerard J. den Heeten "Feasibility of noncontact piezoelectric detection of photoacoustic signals in tissue-mimicking phantoms," Journal of Biomedical Optics 15(5), 055011 (1 September 2010).
Published: 1 September 2010

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