Single-photon-counting polarization ghost
imaging
YUXIN LIU,
1,3
JIANHONG SHI,
1,
* AND GUIHUA ZENG
1,2
1
State Key Laboratory of Advanced Optical Communication Systems and Networks, Shanghai Key Laboratory on Navigation and Location-Based
Service and Center of Quantum Information Sensing and Processing, Shanghai Jiao Tong University, Shanghai 200240, China
2
College of Information Science and Technology, Northwest University, Xi’an 710127, Shanxi, China
3
e-mail: yuxin_liu@sjtu.edu.cn
*Corresponding author: purewater@sjtu.edu.cn
Received 26 August 2016; revised 10 November 2016; accepted 21 November 2016; posted 21 November 2016 (Doc. ID 274572);
published 16 December 2016
We proposed a method for polarization ghost imaging based on single photon counting. With the time-correlated
single-photon-counting technique, we can construct photon time distribution histograms and select a distance
gate to accurately estimate the light intensity. Experiments are performed to realize discrimination of the object
from the background of different materials in weak illumination. In the situation that ambient noise is signifi-
cantly stronger than the signal, our method still can retrieve an image as ambient noise is mostly filtered out
through distance gate selection. We suppose that our method may facilitate applications in remote target
discrimination and biological imaging.
© 2016 Optical Society of America
OCIS codes: (110.1758) Computational imaging; (260.5430) Polarization; (040.3780) Low light level.
https://doi.org/10.1364/AO.55.010347
1. INTRODUCTION
Ghost imaging (GI) [1–8] is an amazing technique which
exploits the quantum nature of light and has attracted much
attention. In traditional ghost imaging, two spatial correlated
beams are divided from a same optical source: the reference
arm, which does not interact with the target and is measured
with a high-resolution charge-coupled device camera. The sig-
nal arm is collected by a so-called “bucket” detector after illu-
minating the target, which has no spatial resolution. Neither of
the detectors alone can produce an image of the object, but by
correlating the measurements of the two detectors over multiple
intensity patterns produced by the source, the object will ap-
pear. Over the past decades, much improvement of GI has been
made due to its flexible optical design and high signal-to-noise
ratio compared with conventional imaging. Computational
GI [9,10] employs computer-control led spatial light modula-
tors to replace the reference arm, which simplifies imaging con-
figuration. Katz reported an advanced reconstruction algorithm
for pseudothermal GI based on compressive sensing [11],
which can dramatically reduce the measurements and improve
image quality. Moreover, GI shows great potential for imaging
in optically harsh environments, such as in scattering medium
or turbulent atmosphere [12–15].
Generally, it is difficult to distinguish different material ob-
jects with similar reflectivities. Polarization ghost imaging (PGI)
[16–18] was recently proposed to retrieve the image when the
object is buried in the background of different polarization prop-
erties. Polarization [19,20] is an inherent property of light which
can provide extra information compared to the object’sspectra
and intensity. Polarization components of light can be employed
to discriminate the object from the different material back-
ground due to the fact that the polarization properties between
the object and the background are different. Imaging under weak
illumination is highly essential in many fields, ranging from
biological sciences to astronomy. For instance, the signal will be
significantly attenuated with distance increase in remote imag-
ing. Inspired by Yang’swork[21], we integrate PGI with the
time-correlated single-photon-counting (TCSPC) technique to
realize the PGI in low-flux measurements. TCSPC [22,23]is
based on the detection of a single photon of a periodic light
signal, the measurement of the detection time, and the buildup
of the photon distribution over the time in the signal period.
We can set a time gate to acquire accurate signal photons. This
technique can achieve high time resolution to the picosecond
level, and high sensitivity even to the single-photon level. The
weak signal can be detected to retrieve an image. Even when the
ambient noise is significantly stronger than the signal, we still
can discriminate the object from the background of different
materials as mostly ambient noise photons are not in the time
gate and the noise in the gate is quite low and can be neglected.
We suppose that PGI with the TCSPC technique will facilitate
Research Article
Vol. 55, No. 36 / December 20 2016 / Applied Optics 10347
1559-128X/16/3610347-05 Journal © 2016 Optical Society of America