IEEE TRANSACTIONS ON BIOMEDICAL ENGINEERING, VOL. 57, NO. 1, JANUARY 2010 185
Local Harmonic Motion Monitoring of Focused
Ultrasound Surgery—A Simulation Model
Janne Heikkil¨ a
∗
, Laura Curiel, Member, IEEE, and Kullervo Hynynen, Senior Member, IEEE
Abstract—In this paper, a computational model for localized har-
monic motion (LHM) imaging-based monitoring of high-intensity
focused ultrasound surgery (FUS) is presented. The LHM tech-
nique is based on a focused, time-varying ultrasound radiation
force excitation, which induces local oscillatory motions at the fo-
cal region. These vibrations are tracked, using pulse-echo imag-
ing, and then, used to estimate the mechanical properties of the
sonication region. LHM is feasible for FUS monitoring because
changes in the material properties during the coagulation process
affect the measured displacements. The presented model includes
separate models to simulate acoustic sonication fields, sonication-
induced temperature elevation and mechanical motion, and pulse-
echo imaging of the induced motions. These 3-D simulation models
are based on Rayleigh–Sommerfield integral, finite element, and
spatial impulse response methods. Simulated-tissue temperature
elevation and mechanical motion were compared with previously
published in vivo measurements. Finally, the simulation model was
used to simulate coagulation and LHM monitoring, as would occur
with multiple, neighbouring sonication locations covering a large
tumor.
Index Terms—Biomedical applications of acoustic radiation,
finite-element (FE) methods, focused ultrasound surgery (FUS),
local harmonic motion (LHM) imaging, simulation.
I. INTRODUCTION
W
HEN an ultrasound wave propagates in a medium, such
as soft tissue, some of its energy is absorbed, resulting
in an increase in the tissue temperature. Many applications of
noninvasive thermal therapy, using high-intensity focused ultra-
sound surgery (FUS) have been published [1]–[3].
In order to achieve consistent tissue coagulation, the actual
temperature must be monitored during the therapy. For ex-
ample, some tissue-specific parameters (e.g., blood perfusion
and ultrasound absorption coefficient) may have local vari-
ations that affect the temperature elevation and distribution.
Presently, the tissue temperature distribution around the son-
ication point is monitored by using magnetic resonance imag-
Manuscript received November 28, 2008; revised June 19, 2009. First pub-
lished October 9, 2009; current version published January 4, 2010. This work
was supported by the Academy of Finland, Finnish Cultural Foundation, North
Savo Regional fund, National Institutes of Health (NIH) Grant R33 CA102884,
the CRC program, and a grant from Ontario Research Fund. Asterisk indicates
corresponding author.
∗
J. Heikkil¨ a was with the Department of Physics, University of Kuopio, 70211
Kuopio, Finland. He is now with the Department of Oncology, Kuopio Univer-
sity Hospital, 70211 Kuopio, Finland (e-mail: janne.heikkila@ kuh.fi).
L. Curiel is with the High Intensity Focused Ultrasound (HIFU) Laboratory,
Thunder Bay Regional Research Institute, Thunder Bay, ON P7B 6V4, Canada
(e-mail: curiell@ tbh.net).
K. Hynynen is with the Imaging Research, Sunnybrook Health Science Cen-
ter, Toronto, ON M4N 3M5, Canada (e-mail: khynynen@ sri.utoronto.ca).
Color versions of one or more of the figures in this paper are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TBME.2009.2033465
ing (MRI) during clinical treatments. Due to the high-cost and
technical limitations of MRI monitoring, alternative treatment
monitoring techniques are being studied. Most of these alterna-
tive approaches to real-time temperature monitoring are based
on diagnostic ultrasound and the detection of changes in the tis-
sue’s temperature-dependent properties, such as backscattered
power [4], speed of sound [5], and stiffness [6]–[8]. Estima-
tion of stiffness changes has been proven feasible for FUS
monitoring, since the contrast between thermally coagulated
and surrounding tissues can be as high as one order of mag-
nitude [9]. Several ultrasound radiation force-based techniques
estimating stiffness-related tissue parameters have been pub-
lished, including acoustic radiation force impulse (ARFI) imag-
ing [10], ultrasound-stimulated acoustic emission (USAE) [11],
ultrasound-stimulated vibro-acoustography (USVA) [12], shear
wave elasticity imaging (SWEI) [13], or localized harmonic
motion (LHM) imaging [14].
LHM imaging [14] is a recently developed technique that
evaluates the mechanical properties of soft tissue. In LHM,
mechanical properties of tissue are estimated, using pulse-
echo imaging to detect tissue harmonic displacements in-
duced by a time-varying ultrasound radiation force. Different
sonication beam configurations can be used to produce this
time-varying radiation force excitation; for two-element ex-
citation systems, overlapping beams at slightly different fre-
quencies are used, whereas for single-beam configurations,
bursts or amplitude-modulated sonication are used [10]–[15].
The LHM technique is considered an elastographic tool be-
cause the characteristics of the induced harmonic motions at
the sonication point are dependent on local mechanical tissue
properties.
FUS monitoring based on LHM has shown to be feasible for
FUS monitoring [7], [8], [16], [17], as tissue motion induced
by amplitude-modulating. A therapy beam can be monitored by
a separate diagnostic pulse-echo transducer. The advantage of
combining LHM with FUS is that the time-varying sonication
beam used to make tissues vibrate that can also be used to
coagulate the target tissue.
The aim of our study was to develop and optimize a com-
plete simulation model of the LHM monitoring technique that
can potentially be used to understand the physical phenomenon
involved. A simulation study of LHM imaging has been pub-
lished [17], however that study investigated only the mechanical
properties of the tissue. In our study, an ultrasound propagation
model was combined with a mechanical and thermal model of
the tissue. In addition, a second ultrasound model was used to
simulate the detection of tissue motion. The effects of tempera-
ture elevation and thermal coagulation on the tissue parameters
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