Efficient modeling and compensation of ultrasound attenuation losses in photoacoustic imaging

Wave attenuation can be considered from the dual viewpoints of assuming a complex wavenumber or a complex frequency. Experimentally, the first viewpoint is preferable if the wave signal can be measured over time, and the second is preferable if the wave signal can be measured over space. These two approaches are discussed in the context of photoacoustic imaging where a short laser pulse excites a broadband ultrasound signal in a sample (e.g., some biological tissue) which can be recorded by detectors configured around the target. Reconstruction of the initial pressure distribution from the detector signals clearly poses an inverse problem. For the complex frequency viewpoint the damping rates of the spatial Fourier modes are calculated using Szabo's wave equation which describes ultrasound propagation in attenuating media obeying a frequency power law. For a symmetric sample problem, a mathematical regularization method is applied to compensate for attenuation losses. It is shown for this important special case that with the complex frequency approach regularization can be performed faster and with more accurate results.

[1]  Patrick J La Rivière,et al.  Image reconstruction in optoacoustic tomography for dispersive acoustic media. , 2006, Optics letters.

[2]  Markus Haltmeier,et al.  Full field detection in photoacoustic tomography. , 2010, Optics express.

[3]  B T Cox,et al.  k-space propagation models for acoustically heterogeneous media: application to biomedical photoacoustics. , 2007, The Journal of the Acoustical Society of America.

[4]  George Gabriel Stokes,et al.  Mathematical and Physical Papers vol.1: On the Theories of the Internal Friction of Fluids in Motion, and of the Equilibrium and Motion of Elastic Solids , 2009 .

[5]  P. Hansen Rank-Deficient and Discrete Ill-Posed Problems: Numerical Aspects of Linear Inversion , 1987 .

[6]  H. Weber,et al.  Temporal backward projection of optoacoustic pressure transients using fourier transform methods. , 2001, Physics in medicine and biology.

[7]  Thomas Berer,et al.  Photoacoustic tomography using integrating line detectors , 2010 .

[8]  Hughes,et al.  On the applicability of Kramers-Kronig relations for ultrasonic attenuation obeying a frequency power law , 2000, The Journal of the Acoustical Society of America.

[9]  P. Burgholzer,et al.  Thermoacoustic tomography with integrating area and line detectors , 2005, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.

[10]  Thomas L. Szabo,et al.  Time domain wave equations for lossy media obeying a frequency power law , 1994 .

[11]  A. Bell On the production and reproduction of sound by light , 1880, American Journal of Science.

[12]  D. Royer,et al.  Elastic waves in solids , 1980 .

[13]  F. John Partial differential equations , 1967 .

[14]  R. Waag,et al.  An equation for acoustic propagation in inhomogeneous media with relaxation losses , 1989 .

[15]  M. Haltmeier,et al.  Exact and approximative imaging methods for photoacoustic tomography using an arbitrary detection surface. , 2007, Physical review. E, Statistical, nonlinear, and soft matter physics.

[16]  Eugène Dieulesaint,et al.  Elastic Waves in Solids II , 2000 .

[17]  S. Holm,et al.  Fractional Laplacian time-space models for linear and nonlinear lossy media exhibiting arbitrary frequency power-law dependency. , 2004, The Journal of the Acoustical Society of America.

[18]  S Holm,et al.  Modified Szabo's wave equation models for lossy media obeying frequency power law. , 2003, The Journal of the Acoustical Society of America.

[19]  Bradley E. Treeby,et al.  Fast tissue-realistic models of photoacoustic wave propagation for homogeneous attenuating media , 2009, BiOS.

[20]  Lihong V. Wang,et al.  Photoacoustic imaging in biomedicine , 2006 .

[21]  P. Beard,et al.  Measurement of Broadband Temperature-Dependent Ultrasonic Attenuation and Dispersion Using Photoacoustics , 2009, IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control.