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| 6:33306 | DOI: 10.1038/srep33306
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Orbital Angular Momentum-based
Space Division Multiplexing for
High-capacity Underwater Optical
Communications
Yongxiong
Ren
1
,*
, Long
Li
1
,*
, Zhe
Wang
1
, Seyedeh
Mahsa
Kamali
2
, Ehsan
Arbabi
2
,
Amir
Arbabi
2
, Zhe Zhao
1
, Guodong
Xie
1
, Yinwen
Cao
1
, Nisar
Ahmed
1
, Yan
Ya n
1
, Cong
Liu
1
,
Asher
J.
Willner
1
, Solyman
Ashrafi
3
, Moshe
Tu r
4
, Andrei
Faraon
2
& Alan E.
Willner
1
To increase system capacity of underwater optical communications, we employ the spatial domain
to simultaneously transmit multiple orthogonal spatial beams, each carrying an independent data
channel. In this paper, we show up to a 40-Gbit/s link by multiplexing and transmitting four green
orbital angular momentum (OAM) beams through a single aperture. Moreover, we investigate the
degrading effects of scattering/turbidity, water current, and thermal gradient-induced turbulence, and
we find that thermal gradients cause the most distortions and turbidity causes the most loss. We show
systems results using two different data generation techniques, one at 1064
nm for 10-Gbit/s/beam and
one at 520
nm for 1-Gbit/s/beam; we use both techniques since present data-modulation technologies
are faster for infrared (IR) than for green. For the 40-Gbit/s link, data is modulated in the IR, and OAM
imprinting is performed in the green using a specially-designed metasurface phase mask. For the
4-Gbit/s link, a green laser diode is directly modulated. Finally, we show that inter-channel crosstalk
induced by thermal gradients can be mitigated using multi-channel equalisation processing.
There is growing interest in high-capacity underwater wireless communications in order to support the significant
increase in demand for data, such as from sensor networks, unmanned vehicles and submarines
1–5
. Traditionally,
acoustic waves have been used for underwater communications, but this technique has quite limited bandwidth
capacity
1,2,5–7
. Alternatively, optics in the low-attenuation blue-green region can enable higher-capacity under
-
water transmission links due to the much higher carrier-wave frequency
8–15
. In order to increase the capacity of
underwater communications, a laudable goal would be to simultaneously transmit multiple independent data
channels by using the spatial domain for multiplexing, i.e., space division multiplexing (SDM)
16
. If the beams are
mutually orthogonal, the different beams can then be efficiently (de-)multiplexed, transmitted through a single
transmitter/receiver aperture pair, and co-propagate with little inherent crosstalk.
An orthogonal spatial modal basis set that might enable underwater SDM is orbital angular momentum
(OAM) modes
17
. A light beam with a helical wavefront carries an OAM value corresponding to
per photon,
where
is the reduced Planck’s constant and
is an unbounded integer that represents the number of 2
π
phase
changes in the azimuthal direction
17,18
. The phase front of an OAM beam twists along the propagation direction
and results in a ring-shaped intensity profile with a central null
18
. Previous reports have explored the use of OAM
multiplexing for high-capacity data transmission through the atmosphere using 1.55-
μ
m light
19–23
. In general,
free-space systems may need to deal with atmospheric turbulence, which can disrupt the beams’ phase fronts and
cause intermodal crosstalk
24–27
.
Much has been uncovered in free-space OAM systems in the infrared (IR), yet little has been reported for
underwater blue-green OAM communications. Indeed, the underwater environment presents several different
challenges for a high-speed OAM link
28,29
. For example, the OAM beam itself and the data it carries can be
1
Department of Electrical Engineering, University of Southern California, Los Angeles, CA 90089, USA.
2
T. J. Watson
Laboratory of Applied Physics, California Institute of Technology, Pasadena, CA 91125, USA.
3
NxGen Partners,
Dallas, TX75219, USA.
4
School of Electrical Engineering, Tel Aviv University, Ramat Aviv 69978, Israel.
*
These authors
contributed equally to this work. Correspondence and requests for materials should be addressed to Y.R. (email:
yongxior@usc.edu) or A.E.W. (email: willner@usc.edu)
r
eceived: 15 June 2016
a
ccepted: 24 August 2016
P
ublished: 12 September 2016
OPEN
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significantly degraded due to various widely-varying effects, such as dynamic scattering/turbidity, water currents,
and temperature gradients
12–15,30–34
. Although these issues are challenging for non-OAM, single beam underwater
links, the problem may escalate for systems using phase front-sensitive OAM beams
25,33–34
.
Recent reports have shown a 4.8-Gbit/s underwater link using a conventional Gaussian beam by directly mod-
ulating a 1.2-GHz bandwidth 450-nm laser diode with orthogonal-frequency-division-multiplexing (OFDM)
data
11
. Moreover, it has been shown recently that two multiplexed blue OAM beams each with a 1.5
Gbit/s data
signal can propagate through 3-metre of water, which includes a scattering solution
28
. However, little has been
reported on the performance degradation of OAM-multiplexed underwater data transmission due to other
underwater effects (e.g., current and thermal gradients) as well as potential mitigation approaches to increase
system performance.
In this paper, we explore OAM multiplexing for high-speed underwater communications, and we demon-
strate up to a 40
Gbit/s link by transmitting four multiplexed green OAM beams through 1.2-metre of water
35
.
Furthermore, we investigate the impact of various underwater conditions (e.g., scattering/turbidity, current, and
thermal gradients) on beam quality and system performance, finding that thermal gradients can produce signif-
icant beam-quality degradation (e.g., modal distortion and beam wander). Importantly, we show systems results
using four beams but with two different approaches for data modulation, one at 10-Gbit/s/beam in the infrared
(IR) and one at 1-Gbit/s/beam in the green); we show both approaches since data modulation technologies are
currently faster in the IR
5,36
. For the IR approach, we modulate a 1064-nm beam at 10-Gbit/s/beam and frequency
double it into the green by using a periodically poled lithium niobate (PPLN) nonlinear crystal, and a specially
designed integrated dielectric metasurface phase mask
37
imprints the OAM on the beam; note that this 40-Gbit/s
aggregate capacity is ~8 times higher than the previously reported result using a single conventional Gaussian
beam
11
. For the green approach, we directly modulate the 532-nm laser diode and achieve a total capacity of
4 Gbit/s. Finally, in order to take advantage of the multiple beams traversing the same medium, we demonstrate
that inter-channel crosstalk induced by thermal gradients can be mitigated using a multi-channel equalisation
digital signal processing (DSP) algorithm at the receiver
38
.
Results
Figure 1 illustrates a prospective application scenario of using OAM multiplexing for high-speed underwater data
transmission. We explore such a scenario under laboratory conditions to (a) help determine the challenges of
OAM-based SDM underwater communications, (b) demonstrate ~8 times increase in underwater transmission
capacity, and (c) show DSP-based mitigation of inter-channel crosstalk effects induced by thermal gradients.
OAM beam propagation through various water conditions.
We first investigate the influence of
underwater propagation on green OAM beams. In general, a light beam propagating through water may suf-
fer degradation from various effects, including scattering/turbidity, currents, and turbulence. We emulate these
underwater conditions in a 1.2-metre-long rectangular tank (with 17
cm in width and 30
cm in height) filled with
tap water. Specifically, underwater scattering/turbidity is produced with suspensions of Al(OH)
3
and Mg(OH)
2
,
which are obtained by adding a commercial antacid preparation (Maalox
®
)
8,12,14
. Circulation pumps pointing
perpendicular to the propagation direction are evenly placed along the link path inside the water tank to produce
a water current. Additionally, thermal gradient-induced water turbulence is created by introducing temperature
inhomogeneity along the optical link, which is accomplished via mixing room temperature and heated water. The
Figure 1.
Prospective application scenario for a high-capacity underwater optical communications link
with OAM-based space division multiplexing.
Key modules including light source, signal modulation, OAM
generation/multiplexing, OAM demultiplexing/detection and receiver signal processing are shown.
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measured power loss induced by traversing the tank and the 1.2 metres of tap water is around 2.5
dB, which is
mainly caused by the reflections at the tank’s glass interfaces.
Figure 2(a) shows the intensity profiles of the individually transmitted and received Gaussian (
=
0) and
OAM beams (
=
+
1 and
+
3) at 520
nm under various conditions: (i) only tap water (a1–a3), (ii) tap water with
only current (a4–a6), (iii) tap water with only Maalox solution (a7–a9), and (iv) tap water with only thermal gra-
dient (a10–a12). The OAM beam with either
=
+
1 or
+
3 is generated by shining the Gaussian beam onto a
spatial light modulator (SLM) loaded with a helical phase pattern of
=
+
1 or
=
+
3. The water current is created
using three circulation pumps, each with a flow rate of 26.8 litters per min. The Maalox solution added into the
water tank containing 30 litters of water is 1.5-millilitre of 0.5% diluted Maalox, and the water after adding the
Maalox is circulated by pumps for 1
minute to obtain a uniform scattering suspension (see Fig. S1(a,b) in
Supplementary Section 1 for the case of a nonuniform suspension when there is no added water circulation). The
room temperature and heated water that are mixed for turbulence emulation have a temperature difference of
0.2
°C; such an approach has been used previously to emulate thermal gradients in water
33,34
.
We observe that the ring-shaped intensity profiles of the OAM beams tend to be maintained after propagating
through tap water, and are slightly distorted by water current, as shown in Fig. 2(a1–a6). When a 1.5-millilitre
Maalox solution is added into still water, there is a small, time-varying change in the intensity profiles. This
change might be a result of the natural dynamic diffusive movement of Al(OH)
3
/Mg(OH)
2
particles in the water.
However, when the particles become evenly distributed in the water after 1-minute circulation from one pump:
(i) the distortions of the OAM intensity profiles tend to be small (Fig. 2(a7–a9)), and (ii) an additional power loss
of 4.5
dB to the link is measured; note that the additional power loss is only 2.2
dB with a 0.5-millilitre of 0.5%
diluted Maalox solution (see Supplementary Section 1). We expect a larger power loss for a higher concentration
of scattering particles.
Figure 2(a10–a12) depict snapshots of intensity profiles under thermal gradient-induced turbulence, show-
ing significant distortions in the beam profiles. We believe that this is mainly due to the higher-order wavefront
Figure 2.
OAM beam propagation through various underwater channel conditions.
(
a
) Intensity profiles of
OAM beams under various channel conditions: (a1–a3) with only tap water, (a4–a6) with water current, (a7–a9)
with the Maalox solution, and (a10–a12) with thermal gradient-induced turbulence. (
b
) Statistics for beam
wander at the receiver with respect to the propagation axis due to water current and thermal gradient-induced
turbulence. (
c
) OAM power spectrum when transmitting OAM channel
=
+
3 under various conditions.
(
d
) Power transfer between all OAM channels under water current.
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aberrations that can result from the refractive index inhomogeneity induced by the water thermal gradient
33,34
.
Moreover, the thermal gradient introduces a dynamic beam wander at the receiver, as depicted in Fig. 2(b).
(obtained from 600 sequentially measured images). The maximal displacement of the received beams is esti-
mated to be ~1
mm, which increases with a larger thermal gradient (as shown in Supplementary Fig. S1(c)). The
beam wander (tip/tilt aberrations) combined with other higher-order wavefront aberrations (high-order Zernike
polynomial terms) could cause the spreading of the transmitted OAM beam power into neighbouring modes,
resulting in significant performance degradation (Supplementary Fig. S1(d)).
The beam wander plot due to water current is also provided in Fig. 2(b), showing a
<
0.1
mm beam displace-
ment, which is much smaller than that with the thermal gradient. We believe this is because that water current
introduces little effect on the homogeneity of water. Figure 2(c) shows the OAM power spectrum for beam
=
+
3
under the above underwater conditions. Due to the relatively small beam degradation caused by water current, the
crosstalk value onto adjacent modes is less than 0.5
dB with only current. However, this value significantly
increases to be
>
7 dB with thermal gradient-induced turbulence. Figure 2(d) presents the power transfer between
OAM modes
=
±
1 and
±
3 under water current. It is estimated that the total crosstalk for each mode is below
−
10.3
dB if all four beams are simultaneously transmitted.
The above measurements indicate that the thermal gradient-induced turbulence has a larger impact on beam
quality than scattering or current, yet the Maalox-induced scattering if uniformly distributed may introduce sig-
nificant link loss; additionally, non-uniform scattering may result in beam quality degradation.
System performance measurements of four OAM multiplexed underwater links.
In this section,
we present the system performance measurements for simultaneously transmitting four OAM beams but using
two different source data generation techniques. The first link transmits a 1-Gbit/s signal at 520
nm on each beam
using the direct modulation of a laser diode, resulting in a capacity of 4
Gbit/s. For the second link, each beam
carries a 10-Gbit/s signal generated using frequency doubling of a data signal at 1064
nm, achieving a significantly
higher capacity of 40
Gbit/s.
4-Gbit/s data link using directly modulated laser diodes.
Two 1-Gbit/s on-off-keyed (OOK) signal beams at
520
nm are generated by directly modulating each of the two 520-nm green laser diodes. The two modulated
green light beams are converted into two different OAM beams with
=
+
1 and
+
3 by adding different spiral
phase patterns using SLMs. The generated OAM beams are coaxially combined and then split into two identical
copies. Another two beams with opposite
values of
−
1 and
−
3 can then be obtained by reflecting one of the
copies three times. We note that this beam copy is relatively delayed with respect to the original one in free-space
for data sequence decorrelation. Subsequently, the resulting four beams are spatially multiplexed and then prop-
agated through the above-mentioned water conditions. At the receiver, each of the four OAM channels is sequen-
tially demultiplexed using another SLM and detected using a high-sensitivity silicon avalanche photodiode
(APD) with 1-GHz bandwidth. The detected signal is amplified, filtered and sent to a 1-Gbit/s receiver for
bit-error rate (BER) measurements (see Supplementary Section 2 for implementation details).
Figure 3(a) depicts the eye diagrams of the 1-Gbit/s OOK signal for OAM channel
=
+
3 under various con-
ditions when the other channels (
=
−
3,
−
1, and
+
1) are turned off or on. The inter-channel crosstalk effects can
be clearly observed in Fig. 3(a4–a6). In the presence of a thermal gradient, the eye diagram of channel
=
+
3 is
time-varying due to fluctuations in the received power and crosstalk, and is not shown here. Figure 3(b) shows
measured BERs as a function of received power for all four channels with and without water. The BER curve for
the back-to-back (B2B) 1-Gbit/s signal is also provided as a benchmark. We observe that tap water introduces
power penalties of less than 2.9
dB at the forward error correction (FEC) limit of 3.8
×
10
−
3
for all channels.
Figure 3(c) presents BER curves for OAM channels
=
+
1 and
+
3 under various conditions. Power penalties are
measured to be 2.2, 2.3, and 2.7
dB in the cases of tap water, Maalox-induced scattering and current, respectively.
Due to the effects of thermal gradient-induced turbulence, the BERs are all above the FEC limit, exhibiting a
severe error-floor phenomenon, and power penalties are above 12
dB for all channels.
40-Gbit/s OAM link using PPLN-based frequency doubling.
Due to water absorption, underwater optical com-
munication links generally use blue-green light. However, data modulation technologies in this spectral region
tend to have much lower bandwidths (e.g., around 1
GHz) than are available for IR light (e.g., beyond 10
GHz)
9,36
.
An important goal would be the achievement of higher data rates for each underwater OAM channel. Therefore,
modulating data in the IR region at a much higher speed and then wavelength converting it into the blue-green
region for subsequent OAM generation and underwater transmission might enable significantly higher system
capacities. Specifically, whereas we previously described data rates on each OAM beam of 1
Gbit/s, we show here
the ability to transmit 10
Gbit/s on each beam using frequency doubling (see Supplementary Section 3 for imple-
mentation details).
A 10-Gbit/s OOK signal at 1064
nm is generated using a lithium niobate modulator and then amplified with a
high power ytterbium-doped fibre amplifier (YDFA). The 1064-nm light after amplification is sent to a
frequency-doubling module that consists of a PPLN crystal and a temperature stabilized crystal oven for fre-
quency doubling. As a result, a 532-nm green light carrying a 10-Gbit/s data stream is generated, where its power
depends upon both the oven temperature and the input pump power. The generated green light acts as a light
source, being converted into OAM beams using specially-designed efficient dielectric metasurface phase
masks
37,39
. Each phase mask has a diameter of 1.5
mm and is composed of a large number of square cross-section
SiN
x
nano-posts that locally modify the light’s phase with subwavelength spatial resolution. The nano-posts are
630-nm tall and are nested on a square lattice with the lattice constant of 348
nm. By changing the nano-post
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width in the range of 60
nm to 258
nm, the transmission phase of each point on the phase mask can be varied from
0 to 2
π
at 532
nm, based on which any arbitrary phase pattern can be designed. Phase masks of
=
±
1 and
=
±
3 each having a blazed grating ‘fork’ phase pattern (i.e., combination of the spiral phase structure of the desired
Figure 3.
System performance measurements for the 4-Gbit/s underwater link using directly modulated
laser diodes.
(
a
) Eye diagrams for OAM channel
=
+
3, (
b
) BERs as a function of received power with and
without tap water, and (
c
) BERs with Maalox-induced scattering, current and thermal gradient-induced
turbulence.
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OAM mode and a linear phase ramp
18
) are designed, fabricated, and characterized (see Supplementary Section 4).
The fabricated phase masks are used to generate high-quality OAM beams with a 50% conversion efficiency
(~3 dB).
Employing a setup similar to the one described in the previous section, the four OAM beams with
=
±
1 and
±
3 are spatially combined and propagate through the underwater channel. At the receiver, each of the four OAM
data channels is sequentially demultiplexed using a metasurface phase mask with an inverse spiral phase pattern.
The beam of the desired channel is spatially filtered after demultiplexing, detected using a high-bandwidth APD
(3-dB cut-off frequency of 9
GHz) and sent to a 10-Gbit/s receiver for BER measurements.
Figure 4(a) depicts the eye diagrams of the 10-Gbit/s OOK signal for OAM channel
=
+
3 when the other
channels are turned off and on. The total crosstalk from all the other channels are
−
11.2,
−
10.7,
−
11.0
dB for the
cases of tap water, current, and Maalox scattering, respectively. Because of this, the quality of the eye diagrams
degrades when other channels are turned on. Figure 4(b) shows measured BER curves for OAM channels
=
+
1
and
+
3 in the cases of tap water and current with and without crosstalk from the other channels. The B2B BER
curve of the 10-Gbit/s signal is also provided. The power penalties are observed to be less than 2.2
dB for all cases
when all channels are on.
Mitigation of thermal gradient-induced crosstalk using multi-channel equalisation.
Previous
sections found various OAM beam degradations and consequent data-channel crosstalk based on underwa-
ter effects. In this section, we address the data degradation problem and show the mitigation of inter-channel
crosstalk due to thermal gradient-induced turbulence. We employ a constant modulus algorithm (CMA)-based
multi-channel equalisation in the receiver DSP to reduce channel crosstalk effects and thus recover the transmitted
Figure 4.
System performance measurements for the 40-Gbit/s underwater link using PPLN-based
frequency doubling for signal generation.
(
a
) Eye diagrams for OAM channel
=
+
3 at a fixed transmitted
power when other channels are turned off or on, and (
b
) BERs as a function of received power with tap water
and current.
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data streams
40–42
. This approach has been previously employed in few-mode and multi-mode fibre-based mode
division multiplexed systems to mitigate the mode coupling effects among multiple spatial modes
43,44
. In general,
it is required that all the transmitted channels are simultaneously detected to enable multi-channel equalisation
processing. Due to receiver hardware limitations, we only show crosstalk mitigation between two OAM channels.
With a similar system approach, two OAM beams with
=
+
1 and
+
3 are generated using metasurface phase
masks, spatially combined using a beam splitter and transmitted through water with a thermal gradient of 0.2
°C.
Each OAM beam carries a 10-Gbit/s OOK signal generated by doubling the frequency of a modulated 1064-nm
signal using a PPLN nonlinear crystal. After demultiplexing and detection, the two OAM channels are simultane-
ously received, converted into Gaussian-like beams and detected by two 9-GHz bandwidth APDs. The two signals
are then amplified, sampled by a real-time scope and recorded for offline DSP. A 2
×
2 CMA equalisation algorithm
is implemented in the DSP to recover two OAM data channels with
=
+
1 and
=
+
3. For a 2
×
2 CMA equalisa-
tion, the equaliser includes four adaptive finite-impulse-response (FIR) filters each with a tap number of 11, the
coefficients of which can be adaptively updated until convergence based on the CMA algorithm (see Supplementary
Section 5). The obtained FIR filter coefficients are used to equalise the crosstalk between the two OAM channels.
Figure 5(a) depicts the received power and crosstalk of OAM channels
=
+
1 and
+
3 measured every 2 sec-
onds under the effects of thermal gradient-induced turbulence. The received power and crosstalk fluctuate by up
to 4.5 and 12.5
dB, respectively. The corresponding BERs for the two OAM channels during the same time period
are shown in Fig. 5(b). Without CMA equalisation, the measured BERs fluctuate significantly between 1.7
×
10
−
2
and 7.4
×
10
−
6
, and dramatically decrease, reaching below the FEC limit of 3.8
×
10
−
3
after 2
×
2 CMA
Figure 5.
Mitigation of thermal gradient-induced crosstalk using CMA-based multi-channel equalisation.
(
a
) Received power and channel crosstalk of OAM
=
+
1 and
=
+
3 over 28
seconds and (
b
) instantaneous
BER of OAM
=
+
1 and
=
+
3 over 28
seconds with and without CMA equalisation under thermal gradient-
induced turbulence when both channels are transmitted. (
c
) Measured BER curves of OAM channel
=
+
1 and
=
+
3 with and without CMA equalisation. Ch.: channel. Eq.: equalization.
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equalisation. We note that only a length of 2,000,000 symbols is recorded for each data sequence due to the lim
-
ited memory of the real-time scope, and therefore the minimum BERs that can be measured are around 5
×
10
−
7
.
To further illustrate the improvement, Fig. 5(c) shows the measured BERs averaged over 1
minute as a function of
received power for channels
=
+
1 and
+
3. Due to inter-channel crosstalk, the measured BER curves without
2
×
2 equalization also have BER error floors. The power penalties at the FEC limit, compared to the B2B case, are
below 2.0
dB for the two channels after equalisation.
Discussion
The experiments described in this paper explore the potential of using OAM-based SDM to increase the transmis-
sion capacity of underwater optical communications, and several issues lend themselves to further exploration.
In general, the use of OAM multiplexing may require a more precise alignment between the transmitter and
receiver compared to a single-channel underwater optical link. This is due to the fact that orthogonality among
OAM channels relies on a common optical axis, and any misalignment may result in inter-channel crosstalk
45
.
Given the beam wander that is introduced by thermal gradients, the above problem is exacerbated and may
require an accurate pointing and tracking system.
Additionally, given that small thermal gradients can produce system degradation, we assume that this problem
could become more severe for longer links for which different types of water may exist. Moreover, this problem
may depend on the transmission direction, such that a vertical link may experience a different thermal gradient
than a horizontal link. Furthermore, whereas we used a channel equalisation algorithm to help mitigate the ther
-
mal gradient-induced crosstalk, it might be necessary under harsher and wider-ranging underwater conditions to
explore the use of multiple mitigation techniques
46–48
. We emphasise that other effects, such as spatial dispersion
and object obstructions, are not considered in this paper but might cause beam spreading and link outage
49,50
.
Finally, we investigated the effects of underwater propagation on OAM-multiplexed data transmission and the
mitigation of inter-channel crosstalk over a short link of metre-length scale. However, we believe our results could
potentially be expanded to longer distances and scaled to a larger number of OAM channels through both careful
system design
45
and the use of multiple mitigation approaches for channel degradation effects. The potential trans-
mission distance of an OAM multiplexed underwater link is limited by various factors, including thermal gradients,
transmitter/receiver aperture size, and attenuation caused by water absorption; such attenuation depends critically
on water type, e.g., coastal water, and oceanic water
3,12
. If we assume that the OAM beams are fully collected by the
receiver aperture and the thermal gradients are mostly compensated by signal processing, we believe it could be
possible to achieve a link distance over 50
metres given a link power loss of ~32
dB for a water type with an attenua-
tion coefficient of 0.15
m
−
1
. OAM multiplexing is in principle compatible with advanced modulation formats (e.g.,
quadrature-amplitude-modulation and OFDM) and wavelength division multiplexing. Particularly, beams with the
same wavelength in the blue-green region can be reused by applying different OAM values to each of the many
beams. When coupling the advances with implementing those techniques, we envision that the underwater trans-
mission capacity of 40
Gbit/s achieved in this paper could be extended by an order-of-magnitude.
Methods Summary
Generation and detection of data-carrying green OAM beams.
Two different data-modulation
approaches are employed to generate high-speed green light signals:
1-Gbit/s signal generation at green using internal modulation.
By directly modulating the driving current of a
520
nm laser diode, a 1-Gbit/s signal at 520
nm is produced. Due to the bandwidth limitation of the internal mod-
ulation of the laser diode, the maximal data rate of the green beam is 1
Gbit/s. The generated signal is then
launched onto a programmable SLM with a specific helical phase pattern to create an OAM beam with either
=
+
1 or
+
3. Multiple generated OAM beams are then multiplexed using a beam splitter-based combiner and
the resulting beams propagate through the underwater channel. The received signal after demultiplexing is
detected using a high sensitivity Si APD with a 3-dB bandwidth of 1-GHz.
10-Gbit/s signal generation at green using PPLN-based frequency doubling.
Generally, the modulation bandwidth
of both internal and external modulations for green light is limited to GHz
4,7
. To overcome this, the frequency
doubling of a data-carrying 1064-nm signal is thus used to produce a high-speed green light signal. Specifically,
we perform high-speed data modulation using a 1064-nm lithium niobate modulator and use a PPLN-based
frequency-doubling module to convert the carrier wavelength from 1064
nm to 532
nm. Consequently, a green
light signal at 532
nm is generated, which is then split into multiple copies and converted into OAM beams using
transmissive metasurface phase masks. At the receiver, a Si APD with a 3-dB bandwidth of 9-GHz but a lower
sensitivity than the detector used for the 520-nm signal detection is employed for signal detection.
Crosstalk mitigation using multi-channel equalisation.
The multiplexed OAM beams may be dis
-
torted due to underwater propagation, causing the power spreading of each transmitted OAM mode onto neigh-
bouring modes. Consequently, each OAM channel experiences interferences from the other channels, resulting in
a non-diagonal channel matrix. Theoretically, to recover the data streams, the received signals of all OAM chan
-
nels could then be multiplied with the inverse channel matrix. In our experiment, we use a 2
×
2 CMA adaptive
channel equalisation in the receiver to reduce the effects of interferences and recover the two data channels. In
general, the dimension of the equalisation processing is determined by the total number of OAM channels. The
CMA-based equalisation utilises an FIR filter-based linear equaliser for each channel. The FIR-CMA equaliser
contains four FIR filters, the coefficients of which can be adaptively updated until convergence based on the CMA.
The obtained FIR filter coefficients are used to equalise the crosstalk between two OAM channels.
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9
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RepoRts
| 6:33306 | DOI: 10.1038/srep33306
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Acknowledgements
We acknowledge James M. Krause, Michael J. Luddy, and Jack H. Winters for valuable help and fruitful
discussions. S.M.K. is supported by ‘Light-Material Interactions in Energy Conversion’ Energy Frontier Research
Center funded by the US Department of Energy, Office of Science, Office of Basic Energy Sciences. E.A. and A.A.
are supported by Samsung Electronics. Device nanofabrication was performed at the Kavli Nanoscience Institute
at California Institute of Technology. This work is supported by Vannever Bush Faculty Fellowship from ASD
(R&E) and ONR, the National Science Foundation, and NxGen Partners.
Author Contributions
Y.R., L.L. and A.E.W. developed the concept and designed the experiments. Y.R., L.L., Z.Z., G.X., Z.W., N.A.,
Y.Y., C.L. and A.J.W carried out the measurements and analysed the data. L.L., Y.C. and Y.R. designed and
implemented the multiple-input-multiple-output equalisation algorithm. S.M.K., E.A., A.A. and A.F. designed,
fabricated, and characterized the metasurface OAM generator phase masks. S.A., M.T., A.F. and A.E.W. provided
technical support. The project was conceived and supervised by A.E.W.
Additional Information
Supplementary information
accompanies this paper at http://www.nature.com/srep
Competing financial interests:
The authors declare no competing financial interests.
How to cite this article
: Ren, Y.
et al.
Orbital Angular Momentum-based Space Division Multiplexing for High-
capacity Underwater Optical Communications.
Sci. Rep.
6
, 33306; doi: 10.1038/srep33306 (2016).
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