November 2023
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6 Reads
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November 2023
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6 Reads
June 2021
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21 Reads
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6 Citations
Ultra-wideband (UWB) transmission over single-mode fibres (SMFs) is an attractive route in optical transmission, since it allows the available low-loss bandwidth offered in conventional silica SMFs to be utilised more efficiently [1] - [3]. However, data transmission beyond a single span over wavelengths outside the erbium gain band remains challenging, primarily because of the lack of suitable optical amplifiers. Recently, the emergence of bismuth-doped fibre amplifiers (BDFAs) has shown considerable potential for amplified high-speed data communications outside the C+L-bands [4] - [8]. An exciting recent work has reported the development of a BDFA exhibiting a 115nm gain bandwidth, covering the range 1345-1460nm [8]. In this paper, we demonstrate the first data transmission experiment utilising this BDFA as a booster amplifier, and we study its performance across this entire gain band.
September 2019
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355 Reads
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79 Citations
Journal of Lightwave Technology
We report a Nested Antiresonant Nodeless hollow-core Fiber (NANF) operating in the first antiresonant passband. The fiber has an ultrawide operational bandwidth of 700 nm, spanning the 1240–1940 nm wavelength range that includes the O-, S-, C- and L- telecoms bands. It has a minimum loss of 6.6 dB/km at 1550 nm, a loss ≤ 7 dB/km between 1465–1655 nm and ≤ 10 dB/km between 1297–1860 nm. By splicing together two structurally matched fibers and by adding single mode fiber (SMF) pigtails at both ends we have produced a ~1 km long span. The concatenated and connectorized fiber has an insertion loss of approximately 10 dB all the way from 1300 nm to 1550 nm, and an effectively single mode behavior across the whole spectral range. To test its data transmission performance, we demonstrate 50-Gb/s OOK data transmission across the O- to L-bands without the need for optical amplification, with bit-error-rates (BERs) lower than the 7% forward error correction (FEC) limit. With the help of optical amplification, 100-Gb/s PAM4 transmission with BER lower than the KP4 FEC limit was also achieved in the O/E and C/L bands, with relatively uniform performance for all wavelengths. Our results confirm the excellent modal purity of the fabricated fiber across a broad spectral range, and highlight its potential for wideband, low nonlinearity, low latency data transmission.
December 2018
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646 Reads
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17 Citations
Abstract Many scientific and practical applications require the propagation time through cables to be well defined and known, e.g., an error in the evaluation of signal propagation time in the OPERA experiment in 2011 initially erroneously concluded that Neutrinos are faster than light. In fact, there are many other physical infrastructures such as synchrotrons, particle accelerators, telescope arrays and phase arrayed antennae that also rely on precise time synchronization. Time synchronization is also of importance in new practical applications like autonomous manufacturing (e.g., synchronization of assembly line robots) and upcoming 5G networks. Even when the propagation time through a coaxial cable or optical fibre is carefully calibrated, it is affected by changes in the ambient temperature, posing a serious technological challenge. We show how hollow-core optical fibres can address this issue.
April 2017
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48 Reads
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17 Citations
We report an Yb-doped fiber master-oscillator power-amplifier (MOPA) system with the capability of selectively generating doughnut-shaped radially and azimuthally polarized beams with user-defined temporal pulse shapes. The desired output polarization was generated with the aid of a nanograting spatially variant half-waveplate (S-waveplate). The latter was used to convert the linearly polarized fundamental () mode output from the preamplification stages to a doughnut-shaped radially polarized beam prior to the power amplifier stage. A maximum output pulse energy of was achieved for pulses at 25 kHz with user-defined pulse shape for both radial and azimuthal polarization states. The polarization purity and beam propagation factor () were measured to be and 2.2, respectively.
February 2017
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77 Reads
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14 Citations
We report a nonlinear signal processing system based on a SiGe waveguide suitable for high spectral efficiency data signals. Four-wave-mixing (FWM)-based wavelength conversion of 10-Gbaud 16-Quadrature amplitude modulated (QAM) and 64-QAM signals is demonstrated with less than −10-dB conversion efficiency (CE), 36-dB idler optical signal-to-noise ratio (OSNR), negligible bit error ratio (BER) penalty and a 3-dB conversion bandwidth exceeding 30nm. The SiGe device was CW-pumped and operated in a passive scheme without giving rise to any two-photon absorption (TPA) effects.
January 2017
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89 Reads
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26 Citations
We demonstrate all-optical regeneration of both the phase and the amplitude of a 10 GBaud quadrature phase shift keying (QPSK) signal using two nonlinear stages. First we regenerate the phase using a wavelength converting phase sensitive amplifier and then we regenerate the amplitude using a saturated single-pump parametric amplifier, returning the signal to its original wavelength at the same time. We exploit the conjugating nature of the two processing stages to eliminate the intrinsic SPM distortion of the system, further improving performance.
January 2017
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33 Reads
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18 Citations
A high-pulse-energy, diffraction-limited, wavelength-selectable, visible source, based on Raman frequency shifting of a frequency-doubled Yb-doped fiber laser, has been studied. The relative length-scaling laws of Raman gain and self-phase modulation push the design towards short fiber lengths with large core size. It is experimentally demonstrated that the Raman clean-up effect in a graded-index multi-mode fiber is not sufficient to obtain diffraction-limited beam quality in the short fiber length. Thus, a large-core photonic crystal fiber is used to maintain diffraction-limited performance and output pulse energies of ~1 μJ, at a 1-MHz repetition rate and 1.3-ns pulse-width are successfully achieved. This step-tunable visible source should find applications in photoacoustic microscopy.
December 2016
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107 Reads
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86 Citations
We demonstrate efficient four-wave mixing among different spatial modes in a 1-km long two-mode fiber at telecommunication wavelengths. Two pumps excite the LP01 and LP11 modes, respectively, while the probe signal excites the LP01 mode, and the phase conjugation (PC) and Bragg scattering (BS) idlers are generated in the LP11 mode. For these processes we experimentally characterize their phase matching efficiency and bandwidth and find that they depend critically on the wavelength separation of the two pumps, in good agreement with the numerical study we carried out. We also confirm experimentally that BS has a larger bandwidth than PC for the optimum choice of the pump wavelength separation.
May 2016
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94 Reads
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70 Citations
Short wavelength operation (1650–1800 nm) of silica-based thulium-doped fiber amplifiers (TDFAs) is investigated. We report the first demonstration of in-band diode-pumped silica-based TDFAs working in the 1700–1800 nm waveband. Up to 29 dB of small-signal gain is achieved in this spectral region, with an operation wavelength accessible by diode pumping as short as 1710 nm. Further gain extension toward shorter wavelengths is realized in a fiber laser pumped configuration. A silica-based TDFA working in the 1650–1700 nm range with up to 29 dB small-signal gain and noise figure as low as 6.5 dB is presented.
... Further, some application cases of high-performance BDFAs in practice transmission are starting to emerge, which makes the O-band a promising candidate for the next amplified transmission band [14][15][16][17]. In the last year, Mikhailov et al. demonstrated that a simple, single-stage BDFA can be used to amplify 400 Gb/s LR-8 LAN-WDM signal from a module designed for 10 km reach, enabling an increase in transmission distance up to 50 km [18]. ...
June 2021
... In addition to low dispersion and nonlinear effects, the multi-band transmission (MBT) of HCF stands out as a promising approach that can improve system throughput by utilizing the previously untapped spectrum of optical fiber transmission systems [8,9]. By exploiting the low-loss multiple spectral windows for data transport, the overall transmission capacity can be significantly increased without requiring drastic changes to existing infrastructure [10]. ...
September 2019
Journal of Lightwave Technology
... By adjusting the core offset, cladding modes were excited and the sensor was endowed with ultra-low thermal characteristics. Additionally, hollow-core photonic bandgap fiber has also been utilized and proven effectively [2], [3]. Material or structure design of sensors are another way to compensate the temperature [4], [5], [6], [7], [8], [9]. ...
December 2018
... Meanwhile, a strong longitudinal electric field can interfere with electron acceleration. For obtaining a radially polarized beam, various methods have been demonstrated, such as the S-wave plate [6], long period fiber Brag grating [7,8], offset splicing [9], mode superposition [10], and coherent polarization beam combination [11]. ...
April 2017
... The extinction of Mach Zehnder interferometer with this Ge-rich silicon-germanium waveguide is higher than 10 dB, and the low loss bends with radii are 12 µm at a wavelength of 1550 nm [16]. The nonlinear signal processing system with the SiGe waveguide is suitable for high spectral efficiency data signals, and 64-QAM signals of this system is less than −10-dB conversion efficiency [17]. According to the plasma dispersion effect and the internal reflection, a SiGe/Si asymmetric optical waveguide switch is proposed at the wavelength of 1550 nm. ...
February 2017
... To mitigate channel crosstalk in optical nodes, all-optical crosstalk suppression schemes are more attractive [6]. All-optical signal processing is usually based on nonlinear effects such as cross-phase modulation (XPM) and four-wave mixing (FWM) in highly nonlinear fibers (HNLFs), semiconductor optical amplifiers (SOAs), periodically poled lithium niobate (PPLN), and so on [7][8][9][10][11]. For example, the data-pump FWM and the mid-span pumpphase shifting (MPPS) techniques in HNLFs were used for crosstalk mitigation [12][13][14]. ...
January 2017
... Actually, compared to other types of pulses, the square-wave pulse is more conducive to transferring energy from pump light to long-wave Raman light through the SRS process [16,17]. Since the peak power of the square-wave pulse is nearly constant over the entire time profile, it is beneficial to provide constant Raman gain. ...
January 2017
... A general theory on N-mode intermodal FWM processes is reported in [17]. Successful intermodal (IM) BS within the telecommunication wavelength range has been demonstrated in both silica fibers [18,19], silicon waveguides [20], and silicon nitride waveguides [21]. In the latter, dispersion engineering of the waveguide was utilized to achieve a record 3-dB bandwidth of 70 nm. ...
December 2016
... It necessitates a high population inversion to achieve an appreciable gain in the short-wavelength region of 1600-1700 nm and effective suppression of long-wavelength (>1700 nm) amplified spontaneous emission (ASE) for reducing the gain competition from the long-wavelength region (>1700 nm) [5]. Many efforts have been made to explore 1600-1700 nm Tm 3+ -doped fiber lasers and amplifiers in the past three decades for their potential application in multiband transmission systems [6][7][8][9][10]. In 1990, Barnes and Townsend demonstrated the possibility of obtaining a Tm 3+ -doped fiber laser at 1650 nm by using a Tm 3+ -doped GeO 2 -SiO 2 fiber as the gain medium, which provides preferential gain at short wavelengths as compared to Tm 3+ -doped Al 2 O 3 -SiO 2 fiber [6]. ...
May 2016
... The four-intensity signal can be used as a pump to modulate the local probe into a four-phase signal according to the property that phase shift during XPM effect depends on intensity. However, during the pump-probe interaction, we cannot consider the XPM effect in isolation, and other nonlinear effects can perturb the results, so the actual power and phase of the output signal are [23]: ...
February 2016