
1
On Landau’s Eigenvalue Theorem for
Line-of-Sight MIMO Channels
Andrea Pizzo Member, IEEE, Angel Lozano, Fellow, IEEE
Abstract—An alternative derivation is provided for the
degrees of freedom (DOF) formula on line-of-sight (LOS)
channels via Landau’s eigenvalue theorem for bandlimited
signals. Compared to other approaches, Landau’s theorem
provides a general framework to compute the DOF in
arbitrary environments, this framework is herein specialized
to LOS propagation. The development shows how the
spatially bandlimited nature of the channel relates to its
geometry under the paraxial approximation that applies to
most LOS settings of interest.
Index Terms— Degrees of freedom, line-of-sight MIMO,
paraxial approximation, Landau’s eigenvalue theorem.
I. INTRODUCTION
The number of distinct waveforms able to transport
information via electromagnetic waves is an inherent
property of a physical channel. It is upper bounded by
the number of degrees of freedom (DOF), a quantity
of interest in information theory [1]–[3], optics [4]–[8],
electromagnetism [9]–[11], and signal processing [12],
[13]. Given the continuous nature of channels, waveforms
span an infinite-dimensional space, yet the noise allows
for a certain error in the representation [10]. Channels are
thus amenable to a discrete representation over a space of
approximately DOF dimensions [14].
There are various ways to compute the number
of DOF in a wireless channel, say by leveraging
diffraction theory [4]–[6], by studying the eigenvalues
of the Green’s operator [3], [7]–[9], or by pursuing a
signal-space approach [1], [13]. This paper provides an
alternative derivation via Landau’s eigenvalue theorem
for multidimensional bandlimited signals (or fields)
[15]. Analogously to time-domain waveforms of finite
bandwidth, an electromagnetic channel may be regarded
as spatially bandlimited due to a low-pass filtering
behavior of the propagation [1], [9], [13]. In this
analogy, time is replaced by space and frequency by
spatial-frequency (or wavenumber) [14].
Originally devised for waveform channels [16],
Landau’s theorem has been generalized to electromagnetic
A. Pizzo and A. Lozano are with Univ. Pompeu Fabra
(email: {andrea.pizzo, angel.lozano}@upf.edu). Work supported by
the European Research Council under the H2020 Framework
Programme/ERC grant agreement 694974, by the ICREA Academia
program, by the European Union-NextGenerationEU, and by the
Fractus-UPF Chair on Tech Transfer and 6G.
ˆ
z
ˆ
x
ˆ
y
S
e(r)
D
R
transmit
array j(s)
Fig. 1. LOS communications between continuous arrays.
propagation [15], and lately applied to non-line-of-sight
(NLOS) channels [13]. Prompted by the interest in LOS
multiple-input multiple-output (MIMO) communication
at high frequencies [17], here the connection is drawn
with such channels under the paraxial approximation
that holds when the propagation is focused about the
axis connecting the two arrays [18]. The development
builds on signal theory concepts, without relying on
unconventional mathematics. A bridge between LOS and
NLOS propagation is also uncovered, with implications
for MIMO communication and Nyquist reconstruction at
high frequencies.
Notation: Fnis the n-dimensional Fourier operator,
(Fnh)(f) = RRnh(t)e−j2πfTtdt=g(f), whereas F−1
n
is its inverse, (F−1
ng)(t) = h(t), with the shorthand
notation F1=Fand F−1
1=F−1. In turn, (Rh)(t) =
R(t)h(t)with R(t)the indicator function of a set
R⊂Rnwhile RAis the set obtained by applying any
invertible linear transform Ato the axes of R, and m(·)
is the Lebesgue measure.
II. PLANE-WAVE REPRESENTATION
OF LOS CHANNELS
Consider two n-dimensional continuous-space arrays
(n= 1 or 2) communicating with scalar electromagnetic
waves at wavelength λin a 3D free-space environment.
We denote by Dthe distance between the array centroids.
Capitalizing on that an arbitrary source can always be
replicated by a flat source on a given plane thanks to
Huygen’s principle [19], we let S⊂Rnand R⊂Rnbe
arXiv:2210.05631v1 [cs.IT] 11 Oct 2022