I. Introduction
Fiber-based distributed acoustic sensing (DAS) technique has recently captured great attention of academia and industry, which has been explored in a wide range of application fields, such as ocean monitoring [1], assessing volcanic eruptions potential [2], earthquake imaging [3], marine geophysics [4], and etc. Because the magnitude of phase variation of Rayleigh backscattered signal (RBS) along optical fibers is linearly related to the magnitude of external acoustic vibrations applied, the phase-sensitive optical time-domain reflectometry (Φ-OTDR) is a promising technique for DAS system, in which the location, amplitude and frequency of external acoustic signals can be demodulated simultaneously [5]. The fiber under test (FUT) gains extreme importance for Φ-OTDR system, which is used as a transducer to convert the acoustic signal into an optical signal that can be measured at the detector [6], [7], [8], [9], [10]. Importantly, the fiber attenuation limits the sensing length of DAS system [11]; the strain-optics and elastic-optics properties of the FUT determine the acoustic sensitivity [12]; the acoustic detection bandwidth is limited by the flat response region of FUT [13]. In order to improve the DAS performance, a number of efforts have been made in terms of sensing fiber, which can be typically categorized as standard single-mode fiber (SMF) or specialty optical fiber.