Broadband all-fiber optical phase modulator based on photo-thermal effect in a gas-filled hollow-core fiber

We report broadband all-fiber optical phase modulation based on the photo-thermal effect in a gas-filled hollow-core fiber. The phase modulation dynamics are studied by multi-physics simulation. A phase modulator is fabricated using a 5.6-cm-long anti-resonant hollow-core fiber with pure acetylene filling. It has a half-wave optical power of 289 mW at 100 kHz and an average insertion loss 0.6 dB over a broad wavelength range from 1450 to 1650 nm. The rise and fall time constants are 3.5 and 3.7 μs, respectively, 2–3 orders of magnitude better than the previously reported microfiber-based photo-thermal phase modulators. The gas-filled hollow-core waveguide configuration is promising for optical phase modulation from ultraviolet to mid-infrared which is challenging to achieve with solid optical fibers.


Introduction
Phase modulators are key components in optical communication, sensing, and signal processing systems. Alloptical modulators, which modulate the phase or intensity of a light signal by a control light beam, have attracted great research attentions 1−13 . Based on stimulated Brillouin scattering and cross-phase modulation, all-optical phase shifters with fast response have been demonstrated 3,4 . However, due to the intrinsic weak nonlinearity of silica, high-power control beams and long optical fibers are required to make useful devices. Yu et al. reported an all-optical phase modulator using a graphenecoated microfiber (MF) 5 . Utilizing the evanescent field of the MF and the strong Kerr nonlinearity of graphene, phase modulation up to 0.18π rad was achieved with a graphene coated length of 15 μm. However, it is challenging to further enhance the phase modulation by reducing the fiber diameter or coating a longer length of fiber with graphene, which will lead to significantly increased insertion loss (IL) due to the intrinsic absorption and imperfect coating of graphene.
All-optical phase modulators have also been demonstrated based on the photo-thermal (PT) effect in nanowaveguides and microfibers coated with low-dimensional materials 6−13 . Nano-waveguide-based phase modulators are compact in size and have fast response, but the coupling loss is large when connecting with optical fibers 6,7 . Gan et al. demonstrated a MF-based PT optical phase modulator with graphene coating 8 . Graphene absorption of the evanescent field of a control light beam heats up the MF, and modulates the refractive index of silica. With a control light power of 230 mW, a signal phase change of 21π is achieved. The IL of the device is 5.4 dB at 1540 nm, mainly due to the absorption of graphene. MF-based PT phase modulators have also been demonstrated with other low-dimensional materials, including tungsten disulfide (WS 2 ) 9 , phosphorene 10 , bismuthene 11 , boron nanosheets 12 , and boron quantum dots (BQDs) 13 . These phase modulators typically have high IL, limited by the absorption and imperfect deposition of low-dimensional materials, and long response time of several milliseconds.
In this work, we demonstrate a new type of all-fiber optical phase modulator based on a gas-filled hollowcore fiber (HCF). In the HCF, most of the optical mode power propagates in the hollow core, which is free from absorption of the solid fiber materials. This enables extremely broadband low-loss transmission, from the ultraviolet to the mid-infrared, apart from a few narrow resonant loss bands 14−18 . The HCF can confine gas phase material, a high intensity control beam and a signal beam simultaneously in the hollow core, providing an ideal platform for strong light-gas interaction over a long interaction length 19,20 . The broad transmission band of the HCF in combination with narrow absorption lines of the gas material enables broadband modulators which are challenging to realize with solid core fibers.
Principle and multi-physics simulation Figure 1(a) shows the basic idea of the HCF-based optical phase modulator. Optical absorption of the control beam excites gas molecules to a higher energy level, which releases heat through non-radiative relaxation. This changes the gas temperature (T) and pressure (p) in the hollow core, which modulates the effective refractive index and hence the phase of the signal beam propagating through the HCF. By modulating the intensity of the control beam, the phase of signal beam is modulated accordingly.
Acetylene (C 2 H 2 ) is selected as the filling gas because it has strong absorption lines at the edge of C-band, which enables a compact modulator with a cost-effective   control light source. Besides, C 2 H 2 is nontoxic and has ro-vibrational relaxation time of 74 ns at P(9) absorption line 21 , which is much faster than the heat conduction time from the gas core to the silica cladding with a typical value of several microseconds. The wavelength of the control beam is fixed at the center of the P(9) absorption line of C 2 H 2 at 1530.371 nm. The absorption coefficient is almost independent of pressure around 1 atm according to HITRAN database 22 and can be fitted to an exponential function of temperature as shown in Fig. 1 The HCF considered here is an anti-resonant hollowcore fiber (AR-HCF) with a mode field diameter of 22 μm at 1550 nm and its SEM image is shown in the inset of Fig. 1(c). The AR-HCF has a broad transmission window with transmission loss less than 3 dB/m from 1200 nm to 2200 nm. When the control light power is sinusoidally modulated, the heat source Q(r,z,t) due to PT effect may be expressed as: (1) where P ctrl (z), ψ nor,ctrl (r) and f represent the average power, normalized intensity distribution and modulation frequency of control beam, respectively. It should be noted that the absorption coefficient α v0 is related to both the radial position r and the axial position z. This is because that α v0 depends on temperature, which is nonuniform in the cross-section and along the HCF.
Based on the fiber structure shown in Fig. 1(c), we have simulated the distribution of temperature and pressure inside the HCF based on the compressible flow equations using COMSOL Multiphysics software 23,24 . The main thermodynamic parameters of materials used for simulation are shown in Table 1 25,26 . The calculated results for P ctrl =500 mW and f=100 kHz are shown in Fig.  1(c). Here the moments when the temperature reaches maximum and minimum are labeled as t 1 and t 2 , respectively. Within a modulation period, T changes up to 80 K in the core center and p changes only about 0.06 atm which is independent of the radial position.
The phase modulation of signal beam at position z within a step length dz may be calculated by using 27 : where λ and ψ nor,sig (r) represent the wavelength and normalized intensity distribution of signal beam, respectively, and μ equals to 0.154 K/atm for pure C 2 H 2 . According to Eq. (2), dφ(z) along the HCF with a step length of 1 mm is calculated as the solid black line shows in Fig. 1(d). Due to gas absorption, the control light power P ctrl (z) reduces with propagation distance, resulting in a decrease of the phase modulation along the fiber length. As a result, the accumulated phase modulation increases nonlinearly with the fiber length, which increases only slightly from 1.53π rad to 1.67π rad when the HCF length doubles from 5 cm to 10 cm.

Fabrication and characterization connector
The schematic of the fabricated gas-filled HCF phase modulator module is shown in Fig. 2(a). Thermally expanded core fibers (TECFs), directly fabricated by heating standard single mode fiber (SSMF) locally to expand its mode field diameter to 22 μm, with anti-reflective coating (R<0.25% at 1550 nm) were used to reduce the connection loss 17,18 . Both ends of a 5.6-cm-long AR-HCF were packaged using capillary glass tubes with inner and outer diameter of 230 μm and 1.8 mm, respectively. It is then inserted into a 5-cm-long hollow glass tube with inner diameter of 1.81 mm and fixed with glue. The HCF and two TECFs were precisely aligned using a pair of 5axis alignment stages and fixed using a 5-mm-long glass connectors with inner diameter of 1.81 mm. There is a micro hole on the glass connector which allows gas diffusion freely. After the low-loss connection between different fibers, we put the module in a glove box with inner volume of 1 L and pure C 2 H 2 was filled into the box with a flow rate of 300 sccm to replace the air. The loss spectrum of the module was monitored using a supercontinuum source and an optical spectrum analyzer. As the gas filling, the absorption loss at 1530.371 nm gradually increased and reached its maximum after about 15 min. The C 2 H 2 concentration inside the HCF was close to be 100% with gas pressure of 1 atm. The micro holes were sealed with glue in the box and a compact gas-filled HCF module was fabricated as shown in Fig.  2(b). The module forms the PT phase modulator together with two wavelength-division multiplexers (WDMs). WDM1 was used to combine the control beam and the signal beam. WDM2 based on thin-film filter reflected the unabsorbed control beam within 1530.3±0.4 nm and passed the signal beam at other wavelength. It can also be replaced by other optical filters such as a fiber Bragg grating. Figure 2(c) shows the loss spectrums of the device before and after C 2 H 2 filling. The average IL without C 2 H 2 filling is about 0.6 dB with a wavelength-dependent loss about 0.2 dB from 1450 to 1650 nm, except for the higher loss induced by the WDMs at 1530.3±0.4 nm. The wavelength dependent loss shows a beat period of 14 nm, which coincides well with the calculated mode effective index difference of 3.0×10 -3 between LP 01 and LP 02 mode in the AR-HCF and the mode extinction ratio of LP 02 mode is estimated to be 40 dB. It can be further sup-pressed by optimizing mode field matching or using HCF with better mode purity. The beating corresponding to the interference of LP 01 and LP 11 mode is not observable, thanks to the accurate alignments. After C 2 H 2 filling, the overall loss keeps unchanged while additional loss peaks appear due to C 2 H 2 absorption, which are shown as the blue lines.
The phase modulator was characterized by using the setup shown in Fig. 2(d). Light beam from a distributed feedback (DFB) laser at 1530.371 nm was modulated by an acoustic optical modulator (AOM) and amplified by an erbium-doped fiber amplifier (EDFA), which acts as the control beam with intensity modulation. A wavelength tunable laser covering wavelength from 1480 to 1640 nm was used as the signal light source. The phase modulator under test formed the one arm of the Mach-Zehnder interferometer (MZI) and a segment of SMF coiled on a piezoelectric transducer (PZT) worked as the second arm. The voltage applied on the PZT was feedback controlled by using the output from PD1 to keep MZI at quadrature. PD2 and PD3 were used to detect the phase modulation and monitor the power level of the control beam, respectively.

Results and discussion
The control light power was sinusoidally modulated at 100 kHz and the P ctrl in the HCF was estimated considering the connection loss between SMF and HCF. Figure  3(a)   different P ctrl . The amplitude of the signal phase modulation is determined from the time-domain MZI output waveform 28 , which increases nonlinearly with P ctrl as shown in Fig. 3(b). Here we define the control light power required to achieve the phase modulation amplitude of π rad as the half-wave power P π , which is determined by curve fitting to be 289 mW at 100 kHz. We believe that the temperature change at high P ctrl is responsible for the nonlinear response. As P ctrl increases, the gas temperature in the HCF also increases, leading to reduced absorption coefficient and gas density, as well as increased heat capacity and heat conductivity of C 2 H 2 at the core center. These different factors contribute to the nonlinear response observed in Fig. 3(b). Due to the above reasons, the phase modulation decreases from 1.41π rad to 1.23π rad at 1550 nm when the environment temperature rises from 25 °C to 100 °C. The temperaturedependence of the phase modulator may be minimized by optimizing gas concentration and fiber length. We also investigated the wavelength dependence of the PT phase modulation and the result is shown in Fig.  3(c). According to Eq. (2), the phase modulation has a 1/λ dependence, and it is approximately linear with λ over a small wavelength span from 1480 nm to 1640 nm with an average decline rate of -8.3×10 -4 π rad/nm.
The frequency response at 1550 nm with P ctrl =502 mW is shown in Fig. 4(a). As the frequency increases from 10 kHz to 1 MHz, the phase modulation decreases from 1.92π to 0.22π with a 3-dB modulation bandwidth of 180 kHz.
The response time is investigated using square pulses with frequency of 10 kHz and duty cycle of 50%, shown as the black dotted line in Fig. 4(b). The MZI output received by PD2 shows a near-square waveform which confirms the fast response of the phase modulator. By fitting to exponential functions, the rise and fall time constants are determined to be 3.5 μs and 3.7 μs, respectively. For HCF-based PT phase modulators, the heat source locates at the gas core region and the heat dissipates quickly once it reaches the silica cladding, whose thermal conductivity is 53 times higher than that of the air. The characteristic time constant is mainly limited by the thermal conduction time from the gas core to the silica cladding with typical value of several microseconds. However, for MF-based PT phase modulators, the heat source surrounds the MF with diameter about several micrometers and the heat dissipates through the 2D-material/air interface. Due to the low thermal conductivity of surrounding air, longer time is required to reach thermal equilibrium. It benefits the heat accumulation and hence higher phase change, but comprises the response time to milliseconds level. Table 2 summarizes the performances of state-of-theart all-fiber optical phase modulators. The HCF-based PT phase modulator reported here shows impressive overall performance with moderate phase modulation ability and low IL over a broad wavelength band. Benefited from the high thermal conductivity of silica cladding, the response time of our modulator is 2-3 orders faster than the MF-based PT phase modulators working in the air 8−13 . Without fiber tapering and low-dimensional material deposition, the gas-filled HCF-based PT phase modulator is easy to fabricate. Compared with commercial electro-optics modulators, the HCF-based PT phase modulator has unique merits, including ultralow loss within a wide wavelength span, all-optical and hence immune to electromagnetic interference, high power handing capability. It would have promising applications in fiber optic interferometer-based phase demodulation systems in particular for harsh environment and remote applications 2,29 , as well as for all-fiber actively Q-switched lasers 13 .

Conclusions
In summary, we have reported, for the first time to our knowledge, an optically controlled all-fiber PT phase modulator based on a gas-filled HCF. Preliminary experiment achieves effective optical phase modulation with a half-wave power of 289 mW at 100 kHz. It shows impressive low IL of ~0.6 dB and broad operational wavelength band from 1480 to 1640 nm. The measured rise and fall time constants are 3.5 μs and 3.7 μs, respectively, 2-3 orders of magnitude faster than the reported MF-based PT phase modulators. The modulator performance could be further improved by optimizing the HCF structure and length as well as gas composition and pressure. The broad transmission bands of the state-ofthe-art HCFs in combination with the many available gas species would allow the development of all-optical modulators from ultraviolet to mid-infrared, which are quite challenging to realize with solid state materials.  This work PT AR-HCF C 2 H 2 π@289 mW b 3.5/3.7 μs 0.6 dB@1550 nm a peak phase modulation for a step change of control power, b dynamic phase modulation measured at 100 kHz.