Towards the Development of Phased Array Systems
for Deep Brain Stimulation
Virgilio Valente and Andreas Demosthenous
Department of Electronic Engineering
University College of London
London, WC1E 7JE, United Kingdom
Email: v.valente@ee.ucl.ac.uk
Richard Bayford
Department of Natural Sciences
Middlesex University
Middlesex, EN3 4SF, United Kingdom
Abstract—Deep brain stimulation (DBS) is a clinical technique
adopted for the treatment of various neurological disorders. One
major limitation of today’s DBS systems is the inability to focus
the electric field in the desired direction and provide a more
efficient stimulation. This study adopted 2D and 3D FEM tools
to explore the the application of phased array (PA) techniques to
control the direction of the stimulation pattern delivered during
DBS. Results illustrate that a PA DBS system can be used
to steer the stimulation pattern from broadside to endfire, by
driving the electrode contacts with high frequency sinusoids with
phase delays varying from 0
◦
to 90
◦
. This study can provide a
framework for future investigation in the development of more
efficient DBS systems based on PA technology.
I. I NTRODUCTION
Deep brain stimulation (DBS) is a clinical tool used to
treat various neurological disorders, including chronic pain,
incontinence and movement disorders. Today’s routine use
of such therapy comes from promising results obtained by
the pilot study of Benabid and colleagues [1], who assessed
the benefits of applying high-frequency stimulation to the
ventral intermediate nucleus. Substantial long-term improve-
ments were reported on several cases of patients affected
by Parkinson’s disease, essential tremor and other movement
disorders. The therapeutic effectiveness of DBS has lead to
its adoption as standard treatment for movement disorders.
Clinical applications, however, have preceded research and
left researchers with a number of challenges to optimize this
therapeutic technique in terms of quality, minimization of costs
and understanding of its underlying mechanisms [2].
One of the major challenges reported in several studies
consists of determining the electric field and volume of tissue
activated (VTA) by stimulation, which is strictly related to the
clinical benefit of DBS and its potential side effects [3]. Due to
the inability of measuring the VTA during therapeutic stimula-
tions, researches have attempted to quantitatively characterize
the VTA by the adoption of two- and three-dimensional repre-
sentations of the DBS electrodes and the anatomical structure
of the stimulation target including the neural response to DBS
[3]–[8]. These studies have highlighted the limited control over
the effects of stimulation and, in particular, over the shape and
direction of the electric field propagating around the electrode.
These issues suggest the need for a system which allows
control of the direction, shape and intensity of the electric field
To achieve this, we propose the use of stimulation based on
phased arrays (PAs). So far application of PAs to stimulation of
human tissue has not been extensively investigated. Abbas and
colleagues [9] have presented a preliminary study of using PA
stimulation to control cardiac activation wavefronts and their
work shows promising results for the application of PAs to
control deep brain stimulation.
This study represents a first investigation on the applicability
of PA systems to DBS. Computational models were adopted
to simulate the behavior of the electric field generated by an
electrode, driven as a PA. These models aim at exploring
the ability of current DBS systems to drive phased array
stimulation (PAS) and investigate the major problems related
to this.
II. METHODS
This study aims at evaluating the use of PA for DBS. In
order to do so we have analyzed the main properties of PAs
and developed 2D and 3D finite element models (FEM) of PA
DBS electrodes, with the aid of a FEM commercial package
(Comsol, Sweden) to simulate the steering of the electric
field around the stimulating electrode. The models adopted
the structure of a commercially available DBS electrode (3389
Model, Medtronic, USA) used for clinical DBS.
A. Phased Arrays (PAs)
PAs consist of multiple antenna elements which use variable
phase or time-delay control at each element to scan the
radiation beam to a desired angle. A particular geometrical
arrangement of the array elements results in the radiation from
each element adding up in a particular direction. The radiated
electric field, E(R
0
, ϑ, φ), at a point Q(R
0
, ϑ, φ) of an antenna
array consisting of N elements is the sum of the contributions
of the electric fields radiated from each element:
E(R
0
, ϑ, φ)= f
e
(ϑ, φ)
e
-jkR0
R
0
N
i=1
[A
i
e
jikdcosϑ
] (1)
where f
e
(θ,φ) is the pattern generated by a single ele-
ment, e
-jkR0
/R
0
represents the spherical propagation factor,
e
jikdcosθ
indicates the phase of the propagation factor of each
element, described but the wavenumber k =2π/λ, where
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