D.J. Richardson’s research while affiliated with University of Southampton and other places

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Publications (300)


102-nm-wide, high-gain, low-noise lumped Raman amplifier
  • Conference Paper

November 2023

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6 Reads

S. Liang

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L. Xu

O+E-band Transmission over 50-km SMF using A Broadband Bismuth Doped Fibre Amplifier

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.


Fig. 2 (a) Measured loss spectrum of the reported NANF; (b) loss of the fabricated NANF (red curve) compared to previous generations of ultrawide bandwidth antiresonant fibers operating in the 2 nd and 3 rd telecoms window (purple: 'hexagram ARF with nodes [14], and green: nodeless tubular ARF [8]); a SoTA wide bandwidth data-transmitting PBGF is also shown for comparison (orange, dashed [4]).
Fig.3. (a) Measured (solid red) vs. simulated loss of the NANF reported herein; (b) simulated fundamental mode and its radial Poynting vector at 1550 nm, showing that a considerable fraction of the loss arises from the gaps created by one smaller than the average tube.
Fig. 4. Measured Loss of the NANF reported in ref. [11] (A; solid blue) vs. current fiber (B; cf. Fig. 1; solid red). Also shown is the simulated optical loss of an ideal geometry, allowing for regular inter-tube gaps with the same average size as in the fabricated fiber (C; gaps of 6.5 µm; dashed purple), and with small inter-tube gap size (D; gaps of 2 µm; dotted grey).
Fig.5. S 2 measurement of the reported NANF showing that no appreciable high order mode content remains after 350 m.
Fig. 6. (a) Schematic of the fully spliced 960-m span comprising of two structurally matched lengths of NANF; (b) SEM images and photograph of the spliced fiber; (c) OTDR trace of the span measured at  = 1550 nm highlighting reflection from the spliced joint; (d) insertion loss of the spliced span which shows 10.15±0.15 dB at 1300 nm and 10.26±0.15 dB at 1550 nm.

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Interband Short Reach Data Transmission in Ultrawide Bandwidth Hollow Core Fiber
  • Article
  • Full-text available

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.

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Figure 1. Examples of applications in which better timing/synchronization than currently available is important. (a) Emerging 5G networks: significantly higher capacity will be achieved by sending information only in the direction of the user. To do so, the precise position of the user must be known. To steer the signal direction, tight synchronization amongst a large array of antennae is needed. (b) For precise coordination of cars and machines that work together, tight synchronization is needed. (c) Financial markets, and also data centres rely on precise synchronization to establish order of the transactions. (d) Signal from widely-spaced telescopes need to be precisely time managed to establish the direction of the incoming signal.
Figure 2. Thermal sensitivity (TCD) of various types of fibres. (a) In standard fibre the TCD is dominated by the thermo-optic coefficient of the glass material in the fibre core through which the light propagates. (b) This is eliminated in HCF (e.g., HC-PBGFs) in which light propagates through air, making thermally-induced fibre elongation the dominant effect that determines the TCD. (c) In engineered HC-PBGF, changes in the waveguide properties (e.g., a larger fraction of the guided mode is inside the central hollow fibre core as the fibre is heated up and the transverse fibre structure expands) can be set to have a contribution to the TCD that has the opposite sign and equal magnitude contribution to the fibre elongation, making HC-PBGF thermally insensitive. n g : group index; ΔL: change of length; HC-PBGF: Hollow Core Photonics Bandgap Fiber; SMF: single-mode fiber.
Figure 4. Fibre temperature (a) and corresponding OEO oscillating frequency change (b) for three selected laser wavelengths of 1550 nm (positive change), 1609 nm (close-to-zero, but still a positive change) and 1612 nm (close-to-zero, but a negative change). The expected change (from our simulations) is also shown. During the 'temperature stabilizing' time period, the temperature inside the thermal chamber does not change uniformly across the chamber, producing ripples in the measured curve. The results shown in (b) were used to evaluate the HC-PBGF TCD (c), shown together with our prediction based on simulations. For comparison, the TCD of SMF-28 4,5 is also shown.
Figure 5. Phase noise properties of the OEO. (a) at 1550 nm and (b) 1612 nm operating wavelengths when the HC-PBGF was used as used as a delay line (green) and when a standard optical fibre that introduced a similar delay was used as a delay line (dashed-red) for comparison. No degradation of the noise performance is seen, showing stable performance of the HC-PBGF based system (which offers a >100-fold reduced temperature sensitivity).
Experimental setup of the OEO. The oscillator cavity consists of the length of HC-PBGF (end face and spectral transmission characteristics shown in inset) placed in a thermally-controlled chamber and with the remaining components (inside the green-dashed-border) being thermally shielded. The blue-dot-bordered part is dedicated to generating a stable 9.972-GHz RF signal reference and using it to measure the OEO frequency drift. WTL: Wavelength-tunable laser; MZM: Mach-Zehnder amplitude modulator, OC: Optical coupler; PC: Polarization controller; OA: Optical Attenuator; PD: Photodiode; RFA: RF amplification; BPF: Band-pass filter, ES: RF splitter; GPS: Global positioning system.
Hollow-core fibres for temperature-insensitive fibre optics and its demonstration in an Optoelectronic oscillator

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.


Radially and azimuthally polarized nanosecond Yb-doped fiber MOPA system incorporating temporal shaping

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.


Wavelength conversion of complex modulation formats in a compact SiGe waveguide

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.


Left: Spectra (a) Before PSA; (b) After PSA; (c) Before amplitude regeneration; (d) After amplitude regeneration. Right: Process resulting in corresponding spectra.
Experimental setup of the regenerator showing the two underlying phase and amplitude regenerative stages.
(a) Spectrum identifying the pump to signal power ratio, P1 : S. (b) Plot of output OSNR of regenerated signal against P1 : S for three different total launch powers into the fibre.
Δϕ, ΔMag and EVM for three different noise scenarios.
(a) Constellation plots; (b) BER curves for the complete system with both sub-systems combined.
Full quadrature regeneration of QPSK signals using sequential phase sensitive amplification and parametric saturation

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.


Schematic of the experimental setup
SHG power and conversion efficiency versus input fundamental power. The inset shows the second harmonic spectrum.
Output Raman spectra from a step-index single mode fiber with lengths of 15 m (a) and 5 m (b). The different colours represent different pump powers launched into the fibers to selectively excite different Stokes lines. Pump power: blue 285 mW; green 685 mW; red 880 mW in (a) and blue 540 mW; green 1.3 W; red 1.5 W in (b).
(a) Output beam profiles from graded-index fiber: pump after 200 m fiber (i); 3rd Stokes after 200 m fiber (ii); 3rd Stokes after 19 m fiber (iii) and (b) Raman spectra of the 19 m graded-index fiber. In (b) the different colours represent different pump powers launched into the fibers to selectively excite different Stokes lines. Pump power: blue 890 mW; green 1.1 W; red 1.5 W.
(a)Output Raman spectra and beam profile of the 15-m PCF and (b) Pulse shapes of pump and Raman Stokes, all pulse amplitudes are normalized and equally offset for better visibility. In (a) the different colours represent different pump powers launched into the fibers to selectively excite different Stokes lines. Pump power: blue 640 mW; green 1.6 W; red 1.9 W.
Raman-shifted wavelength-selectable pulsed fiber laser with high repetition rate and high pulse energy in the visible

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.


Inter-modal four-wave mixing study in a two-mode fiber

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.


(a)–(c) Schematic of the experimental setup for diode-pumped TDFAs working in the 1700–1800 nm region, denoted as TDFA-A/B/C, respectively. Iso., isolator; Cir., circulator; LD, laser diode; WDM, wavelength division multiplexer; TDF, thulium-doped fiber; HDF, holmium-doped fiber. (d) Right axis, absorption of the HDF; left axis, insertion losses of passive components, including a custom-made WDM coupler, an isolator, and a circulator. For comparison, the insertion loss of a first-generation WDM coupler is also shown.
Detailed wideband performance of TDFA-A shown in Fig. 1(a). Wavelength dependence of the small-signal gain ( seed power), saturated gain (0 dBm seed power), and NF for both gain curves. (b) Output spectra over the tested wavelength region for 0 dBm seed power, measured with 0.5 nm spectral resolution.
Gain and NF of TDFA-A/B/C in the 1710–1850 nm region in comparison with those of a previously reported TDFA [9]. Symbols with and without lines correspond to gain and NF results, respectively.
(a) Schematic of the TDFA working in the 1650–1700 nm region. Cir., circulator; WDM, wavelength division multiplexer; TDF, thulium-doped fiber; ASE, amplified spontaneous emission; Iso., isolator; F.L., fiber laser; P.D., power dump; M, Mirror. (b) Left, insertion losses of the circulator and WDMs; right, transmission loss of the ASE filters.
(a) Gain and NF characteristics of the TDFA shown in Fig. 4. (b) Spectra of amplified small signals (0.5 nm spectral resolution).
Exploiting the short wavelength gain of silica-based thulium-doped fiber amplifiers

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.


Citations (75)


... 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]. ...

Reference:

O-band BDFA achieves 24 dB ultra-wideband signal range effective gain clamping with a maximum float of 0.42 dB
O+E-band Transmission over 50-km SMF using A Broadband Bismuth Doped Fibre Amplifier
  • Citing Conference Paper
  • 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]. ...

Interband Short Reach Data Transmission in Ultrawide Bandwidth Hollow Core Fiber

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]. ...

Hollow-core fibres for temperature-insensitive fibre optics and its demonstration in an Optoelectronic oscillator

... 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]. ...

Radially and azimuthally polarized nanosecond Yb-doped fiber MOPA system incorporating temporal shaping

... 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. ...

Wavelength conversion of complex modulation formats in a compact SiGe waveguide

... 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]. ...

Full quadrature regeneration of QPSK signals using sequential phase sensitive amplification and parametric saturation

... 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. ...

Raman-shifted wavelength-selectable pulsed fiber laser with high repetition rate and high pulse energy in the visible

... 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. ...

Inter-modal four-wave mixing study in a two-mode fiber

... 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]. ...

Exploiting the short wavelength gain of silica-based thulium-doped fiber amplifiers

... 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]: ...

Optimisation of amplitude limiters for phase preservation based on the exact solution to degenerate four-wave mixing