Optics Communications 446 (2019) 72–76
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Optics Communications
journal homepage: www.elsevier.com/locate/optcom
Photonic quantization using dual-output Mach–Zehnder modulators and
balanced photodetectors
Hongxia He
a
, Shuna Yang
b
, Tao Jin
a
, Hao Chi
b,
∗
a
College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China
b
School of Communication Engineering, Hangzhou Dianzi University, Hangzhou 310018, China
A R T I C L E I N F O
Keywords:
Photonic analog-to-digital conversion (ADC)
Dual-output Mach–Zehnder modulators
(DOMZMs)
Balanced detection
Photonic sampling
A B S T R A C T
A novel approach for photonic quantization using dual-output Mach–Zehnder modulators (DOMZMs) and
balanced photodetectors (BPDs) is proposed and experimentally demonstrated. Based on the phase-shifting
technique, all DOMZMs used in the scheme have identical half-wave voltages but are biased at different
voltages. Due to the use of BPDs and DOMZMs with complementary outputs, the threshold voltages of
comparators can be kept at zero, which eliminates the influence of power fluctuation of the input sampling
pulses and improves the effective number of bits (ENOB) of the analog-to-digital conversion (ADC) system.
After the comparators, a digital Gray code that represents the analog signal to be digitized is obtained. Proof-
of-concept experiments with 8 and 16 quantization levels are implemented to verify the feasibility of the
proposed approach. Bit resolution, ENOB degradation induced by bias voltage errors and potential for photonic
integration are also discussed.
1. Introduction
High-speed analog-to-digital converters (ADCs) have a wide range
of applications in modern wireless and optical communications, ad-
vanced radars, real-time measurements, as well as other scenarios with
the requirement of wideband signal acquisition. However, the develop-
ment of electronic ADC is hindered by inherent bandwidth limitation
of electronic components and timing jitter of sampling clock [1]. Due
to the high bandwidth offered by photonic components, realizing ADCs
with photonic technologies has attracted much research interest in the
past decades. Moreover, mode-locked lasers with high repetition rate
and low timing jitter are considered as excellent sampling sources that
could improve the performance of ADC systems [2]. Typical schemes
of photonics-assisted ADCs include the photonic quantization using
electro-optic modulators [3–11], the photonic time stretch for slowing
down an ultrafast signal prior to electronic digitization [12–17], the
photonic quantization based on amplitude-to-frequency conversion in-
duced by optical nonlinearities [18–21], as well as the optical sampling
using high-speed optical pulse train as sampling source [22–25]. An
ADC based on the technique of photonic time stretch, with an effective
number of bits (ENOB) of 8.27 bits and a bandwidth of 10 GHz, was
demonstrated in [14], despite that some issues, such as dispersion
penalty, nonlinear distortion and continuous-time operation, need to
be solved before its practical applications [15–17]. For the photonic
ADCs based on amplitude-to-frequency conversion, a recent report
demonstrated an ultra-high sampling rate of 40 GS/s and an ENOB
∗
Corresponding author.
E-mail address: chihao@hdu.edu.cn (H. Chi).
of 3.79 bits [18]. More recently, it was pointed out that the time–
frequency uncertainty principle puts a fundamental limit on this type
of ADCs in [21]. Benefit from the ultra-low timing jitter of mode-
locked lasers, the technique of optical sampling shows high potential
for realizing ADCs with ultra-high sampling rate. In [24], an ADC
based on optical sampling with a correction algorithm for compensating
mismatch among multiple channels was demonstrated, which realizes
a sampling rate of 40 GS/s, an ENOB of 7.5 bits, and a bandwidth of
12.1 GHz. In [25], a 4-channel time–wavelength pulse interleaver, as an
important component of high-speed wavelength-interleaved photonic
ADCs, was implemented on a silicon photonic chip, which can be used
to realize photonic ADCs with a sampling rate of 4 GS/s.
In 1975, Taylor proposed a photonic quantization approach based
on Mach–Zehnder modulator (MZM) array [3]. To achieve the correct
quantization and coding, the half-wave voltage (𝑉
𝜋
) of each MZM
should be half as that of its nearest more significant bit. However, it is
difficult to fabricate such an MZM array even with the state-of-the-art
photonic integration technology when four or more MZMs are needed.
To overcome the difficulty relating to the geometrically scaled half-
wave voltage, some alternative solutions have been proposed [4–10].
A scheme using cascaded MZMs with identical 𝑉
𝜋
was presented by
Jalali and Xie in [4]. A similar scheme that uses cascaded phase mod-
ulators (PMs) was proposed by Currie, where the employed PMs have
identical 𝑉
𝜋
and support orthogonal polarization modes [5]. Though
the cascading of MZMs or PMs is able to realize equivalent scaling 𝑉
𝜋
,
https://doi.org/10.1016/j.optcom.2019.04.069
Received 7 March 2019; Received in revised form 19 April 2019; Accepted 23 April 2019
Available online 26 April 2019
0030-4018/© 2019 Elsevier B.V. All rights reserved.