224 IEEE TRANSACTIONS ON COMPUTATIONAL IMAGING, VOL. 7, 2021
Electromagnetic Field Imaging in Arbitrary
Scattering Environments
Karteekeya Sastry , Chandan Bhat , Raffaele Solimene , Senior Member, IEEE, and Uday K.
Khankhoje , Senior Member, IEEE
Abstract—In this article, we propose a method to reconstruct
the total electromagnetic field in an arbitrary two-dimensional
scattering environment without any prior knowledge of the incident
field or the permittivities of the scatterers. However, we assume
that the region between the scatterers is homogeneous and that
the approximate geometry describing the environment is known.
Our approach uses field measurements and a compressive sensing
inspired algorithm to estimate the incident field and the tangential
electric and magnetic fields on the scatterers’ surfaces. These esti-
mates are then used to predict the field everywhere using Huygens’
principle. Further, we identify the best measurement locations in
the environment, which reduces the estimation error to approxi-
mately half of the error obtained when using random locations.
We show that in an indoor scenario with up to four scattering
objects, the total electric field is recovered with less than 10% error
when the number of measurements is just 0.3 times the number of
unknowns in which the problem is formulated. The formulated
problem is solved using ‘Total field - Compressive sensing based
subspace optimization method’ – an algorithm that leverages the
sparsity of the tangential fields in known transformation domains
to obtain an optimal solution.
Index Terms—Compressive sensing, electromagnetic fields,
sensor placement, subspace optimization.
I. INTRODUCTION
K
NOWLEDGE of the electromagnetic (EM) fields is useful
in many applications like network planning, WiFi access
point planning in indoor scenarios, and indoor localization [1]–
[4]. Existing methods in the literature that address this problem
are based on ray tracing [5], [6]. It is well known that the
ray-tracing model fails to account for the effects of diffraction
Manuscript received August 22, 2020; revised November 29, 2020; accepted
January 27, 2021. Date of publication February 1, 2021; date of current version
February 19, 2021. This work was supported by the Microwave Inverse Scat-
tering for Breast Cancer Detection project through the Science and Engineering
Research Board, Department of Science and Technology, Government of India,
under Grant ECR/2018/001953. The associate editor coordinating the review
of this manuscript and approving it for publication was Dr. Ilaria Catapano.
(Karteekeya Sastry and Chandan Bhat contributed equally to this work.) (Cor-
responding authors: Chandan Bhat; Uday K. Khankhoje.)
Karteekeya Sastry is with the Department of Electrical Engineering,
California Institute of Technology, Pasadena, CA 91125 USA (e-mail:
karteekdhara98@gmail.com).
Chandan Bhat and Uday K. Khankhoje are with the Department of Electrical
Engineering, Indian Institute of Technology Madras, Chennai 600036, India
(e-mail: chandanbhat21@gmail.com; uday@ee.iitm.ac.in).
Raffaele Solimene is with the Universita della Campania Luigi Vanvitelli,
Italy, and is also an Adjunct Faculty with the Department of Electrical Engi-
neering, Indian Institute of Technology Madras, Chennai 600036, India (e-mail:
raffaele.solimene@unicampania.it).
Digital Object Identifier 10.1109/TCI.2021.3055982
Fig. 1. Problem depiction with a source (J ) radiating in the presence of objects,
enclosed within a wall. Field measurements are made at strategic locations
as indicated by filled dark circles. The objective is to predict the field at any
point outside the object(s) and within the walls. To achieve this, tangential
electromagnetic fields are estimated on object and wall boundaries.
around the corners of the objects, waveguiding in the corridors,
and multiple reflections [7, Fig. 3]. Another popular approach is
to assume that the EM fields are sparse in the spatial Fourier
domain, and to leverage this information to reconstruct the
fields [8]. This assumption works well when the domain of
interest is far from the scatterers and the sources. Moreover,
in most of the literature on EM inverse problems, information
on the scattered fields is needed to solve the problem, which
implies that the incident field should also be known [9], [10].
In this paper, we present a method to reconstruct the total
EM field from total field measurements at optimal sampling
locations. We do not assume any prior knowledge of the incident
field or the permittivities of the scatterers. However, we assume
that the region between the scatterers is homogeneous and that
the approximate geometry of the scatterers and the source is
known. Our method is based on surface integral formulations and
is therefore a significant improvement over existing ray tracing
methods in the literature. In recent work [11], we presented a
method for reconstructing the scattered EM fields by making
measurements at random locations, but assumed knowledge of
the incident field. In the current work, we generalize this method
to recover the total field without any prior knowledge of the
incident field. We also identify optimal sampling locations in
the environment. The problem setup is graphically represented
in Fig. 1.
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