M.E. Marhic's research while affiliated with Swansea University and other places
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Publications (177)
A semi-classical model is proposed theoretically and demonstrated experimentally on the optical receiver sensitivity enhancement by single-band (signal or idler) and dual-band (signal and idler) fiber optical parametric amplifier (FOPA). The sensitivity enhancement by single-band is determined by the gain of FOPA and the transmission loss of signal...
Four-wave mixing between two initial closely-spaced pumps can generate mixing tones which deplete the initial pumps, and reduce total stimulated Brillouin scattering compared to a single pump. We present theoretical and experimental results confirming this reduction. This mechanism explains why it is actually possible to obtain large gains in some...
A fiber optical parametric amplifier followed by a conventional amplifier can help reduce internal nonlinear crosstalk, while exhibiting a low noise figure. We review this concept and present our recent experimental results validating it.
A continuous-wave fiber optical parametric oscillator with a ring cavity containing a highly nonlinear fiber and two cascaded narrowband filters is demonstrated. We report a 3-dB laser linewidth of less than 400 kHz at 1549 nm with single longitudinal mode operation. Wavelength stability of the laser is <±100 MHz, governed mainly by the narrowband...
We demonstrate reduction of four-wave mixing crosstalk using hybrid optical parametric amplifier with erbium-doped fiber amplifier. Crosstalk reduction of more than 13 dB has been achieved while providing 20-dB gain. Noise figures of different amplifier configurations are compared. Bit error rate measurements confirm the hybrid configuration introd...
Two sets of formulas are derived for the field-quadrature and photon-number fluctuations (variances and correlations) produced by parametric amplifiers and frequency convertors that are driven by pulsed pumps and act on pulsed signals. The first set is based on the Green functions for the underlying parametric processes, whereas the second is based...
The quantum-limited noise figure (NF) for a general combination of linear optical elements is obtained in a compact form. The entries in this expression are obtained from the classical input–output transmission coefficient of the signal, and of the various transmission coefficients from the noise inputs to the output. The same result is also obtain...
A phase-sensitive amplifier followed by a phase-insensitive one can have a noise figure well below 3dB. This can be used for reducing the detrimental nonlinear effects occurring in fiber optical parametric amplifiers for optical communication.
Fiber optical parametric amplifiers (OPAs) are based on a highly-efficient four-wavemixing process. Their capability to give very high gain and large bandwidths has made them an attractive candidate for numerous applications. One of them is continuous-wave(CW) fiber optical parametric oscillators (OPOs) using them as a gain medium. In this chapter...
A microdielectric resonator antenna of dimensions (100 × 100 × 500 m) is designed for biosensing applications. The antenna is terminated with a thin layer of gold on the top and bottom of the microstructure for achieving a high Q . On top of the antenna is the sensing region (100 μm<sup>3</sup>), which loads the antenna depending on the type of mat...
We investigate to what extent the unique features of OPAs (large bandwidths, 0 dB noise figure, phase conjugation, signal regeneration) can be combined and exploited in future long-haul communication networks. Network PMD can complicate the use of phase-sensitive amplification.
We review our investigations on bismuth-oxide fiber as an amplifying medium for parametric amplifiers with continuous-wave pumping. The results lead to new applications in demultiplexing, which are discussed.
We report reduction of cross gain modulation to less than 1 dB by using gain clamping
in a fiber optical parametric amplifier. Power penalties were improved from 2.5 dB to 0.5 dB.
We report on a CW fiber OPO whose output wavelength can be tuned over the 1463-1674 nm range. Over 1 W of output power can be extracted at long wavelengths. The signal 3-dB signal linewidth is about 0.08 nm.
We report high-capacity (> 1 Tb/s) amplification by a fiber optical parametric amplifier in different roles displaying compatibility and versatility in future WDM networks with phase-shift keying modulation format.
The burst-mode amplification performance of a fibre optical parametric amplifier (FOPA) is experimentally investigated. Compared to an EDFA, no serious transient effect was observed for amplified optical packets even with a low traffic granularity, due to the fast response of the FOPA.
We have achieved a four-wave mixing process in a high-finesse highly nonlinear fiber Fabry–Perot resonator, where the amplified signal and idler were enhanced in transmission by 6 dB and 10 dB respectively comparing with those in a single fiber. We used a 6 m long low-loss Fabry–Perot resonator with two high-reflectivity fiber Bragg gratings writte...
We report less than 1-dB cross-talk penalty for 26 DWDM channels modulated at 43.7 Gb/s RZ-DPSK when amplified by a fiber optical parametric amplifier showing compatibility with high-capacity (> 1 Tb/s) communication systems.
We have experimentally shown that gain clamping is required in fiber optical parametric amplifiers. By using optical gain clamping (OGC), we have reduced gain variation to 1 dB, for signal input variation of 12 dB.
We report operation of a continuous-wave one-pump fibre OPA with net gain between 1447 nm and 1717 nm. We used a 114 m long step-index highly-nonlinear fibre, and 5 W of pump power.
Optical demultiplexing for a 40 Gbit/s RZ-DPSK OTDM signal using a fibre optical parametric amplifier with a sinusoidal-clock-modulated pump is experimentally demonstrated. Less than 1.3 dB power penalty and around 30 dB gain are obtained for all four demultiplexed channels. Superior performance is obtained for the demultiplexed tributaries in RZ-D...
We report operation of a continuous-wave one-pump fiber OPA with net gain between 1460 nm and 1690 nm. We used a 50 m long step-index highly-nonlinear fiber, and 5 W of pump power.
We used the sub-nanometer bandwidth of a bismuth-oxide fiber OPA for demultiplexing 10 Gb/s channels 100 GHz apart with penalty <2 dB. We obtained -20 dB of crosstalk, with 2.5 W of CW pump power.
We show that the set of two coupled differential equations governing a four-wave mixing (FWM) component and its associated idler in a one-pump fiber optical parametric amplifier are the same as for standard parametric amplification, but with additional source terms arising from FWM between already-calculated waves. We show how to solve this new set...
We improve the accuracy of numerical simulations for short fiber optical parametric amplifiers (OPAs). Instead of using the usual coarse-step method, we adopt a model for birefringence and dispersion which uses fine-step variations of the parameters. We also improve the split-step Fourier method by exactly treating the nonlinear ellipse rotation te...
The exact solution of the two coupled differential equations governing a FWM component and its associated idler in a one-pump fiber OPA consist of a sum of exponentials. First- and second-order crosstalk terms scale like the corresponding powers of the signal power.
We show that the ratio of fiber loss to fiber nonlinearity is an important parameter for the design of pump resonators for fiber OPAs. Silica-based HNLF have advantages over other nonlinear fibers for making such resonators, and can exhibit power enhancement ratios of over 100.
We investigated the gain of two-pump fiber-optic parametric amplifiers (OPAs) when the signal is close to one pump. We considered all eight types of OPAs introduced in [
J. Opt. Soc. Am. B
20, 2425 (2003)
], and we extended the analysis of that paper from a four- to a six-wave model. We started from six coupled-wave equations and derived exact exp...
We obtained 6 dB gain with a one-pump fiber OPA using a 3-m long Bi-HNLF fiber. Pump power was 30.2 dBm. SBS suppression required 300 MHz PRBS phase modulation.
We report on the amplification of 12 × 10 Gb/s wavelength-division-multiplexed signals by a double-pumped fiber optic parametric amplifier (2P-FOPA). A gain of 10 dB is obtained using a 4.3 km-long conventional dispersion shifted fiber (DSF) as nonlinear medium. Our spectra show negligible generation of spurious FWM products, and we attribute this...
In recent years, impressive performance of fiber optical parametric amplifiers (OPAs) have been demonstrated in different respects. We describe these recent advances and discuss some of the challenges should be addressed before OPAs can be practical.
We propose a novel metro-access integrated network that integrates hybrid TDM/WDM optical access networks into MAN, such that the capacity upgrade in both networks can be achieved simultaneously. By interconnecting multiple access ring networks, MARIN provides alternative paths for MAN traffic to be routed on it with high aggregated throughput. Thu...
We improve the accuracy of the split-step Fourier method by exactly treating nonlinear ellipse rotation terms. Results obtained this way for two-pump OPAs are significantly different from those obtained by neglecting ellipse rotation terms 2006 Optical Society of America OCIS codes: (060.2320) Fiber optics amplifiers and oscillators; (190.4370) N...
A fibre optical parametric ampifier operating in the small-signal gain regime can exhibit the same gain when amplifying in either direction. This is true even in the presence of random dispersion and birefringence variations along the fibre.
The 1620-1700 nm region of the optical spectrum is important as it contains numerous molecular resonance lines of chemical species. We have investigated, theoretically and experimentally, the possibility of designing an efficient tunable wavelength converter (WC) based on a fiber OPA, to generate high-power in that range, by mixing radiation genera...
We propose and demonstrate a polarization independent two-pump fiber OPA based on polarization diversity. We achieve less than 0.4-dB PDG for 15.5-dB gain when the input signal polarization is swept over the Poincare sphere.
We show that the signal quality degradation of WDM channels in a two-pump optical parametric amplifier (OPA) is dominated by the cross-gain modulation (XGM) and we demonstrated experimentally that it can be improved significantly by a two-orthogonal-pump OPA (2OP-OPA).
Fiber optical parametric amplifiers (OPAs) are nonlinear devices based
on the third-order nonlinear susceptibility of glass fibers. They
require one or two pumps, located near the fiber zero-dispersion
wavelength, and phase matching between the waves must occur. Injecting a
signal at the input results in amplified signal and a new wavelength,
the i...
We show that with a two-orthogonal-pump OPA (2OP-OPA), the WDM signal quality is improved by up to 4-dB compared to a two-parallel-pump OPA (2PP-OPA) with the same signal gain.
The gain spectrum of a fiber optical parametric amplifier (OPA) can be controlled by imposing a temperature distribution along the fiber, which modulates the local fiber zero-dispersion wavelength lambda0, and hence the parametric gain coefficient. We present simulations and experimental verification for various binary temperature distributions. Th...
We propose and demonstrate a novel multiple wavelength converter with gain based on a pulsed-pump fiber optical parametric device. Penalties ranging from 0.26 to 1.24 dB for ±k ×100 GHz (k= 1,2,3,4) wavelength conversion were measured.
Fiber optical parametric amplifiers (OPAs) are based on the third-order nonlinear susceptibility of glass fibers. If two strong pumps and a weak signal are fed into a fiber, an idler is generated. Signal and idler can grow together if pump power is high enough, and phase matching occurs. Gain in excess of 60 dB has been obtained. Fiber OPAs can exh...
Fiber optical parametric amplifiers (OPAs) are based on the third-order nonlinear susceptibility of glass fibers. If two strong pumps and a weak signal are fed into a fiber, an idler is generated. Signal and idler can grow together if pump power is high enough, and phase matching occurs. In recent years, impressive performance has been demonstrated...
By suitably choosing the fiber properties, and by tuning the pump wavelength near the fiber zero-dispersion wavelength, one can in principle generate a wide variety of one-pump fiber optical parametric amplifier gain spectra. These can range from a very wide single region to two symmetric narrow gain regions far away from the pump. We have experime...
Upconversion pumping in the 1400 nm-range gives thulium-doped fiber amplifier (TDFA) a dynamic range of 15 dB, and transient power excursion much lower than conventional erbium-doped fiber amplifier during dynamic wavelength add-drop. Hence, it is promising for bursty traffic applications.
System performance of 40 Gb/s transmission over short-reach, commercial-grade 62.5 μm multimode fiber using readily available single-mode transceivers is highly sensitive to launch polarization. Return-to-zero transmission experienced 3-dB power penalty, while nonreturn-to-zero suffered link outage.
By averaging the OPA equations for fibers with random birefringence, we show that the gain coefficient with orthogonal pumps is significantly larger than would be expected in nonbirefringent fibers. This is verified by experiments.
The large homogeneous bandwidth of a thulium-doped fibre amplifier makes it suitable for optical gain clamping. This has been demonstrated experimentally. Gain variation of 1.2 dB for 15 dB input dynamic range has been achieved, with less than 1 dB gain ripple over 20 nm, and no noise figure degradation, while pumped at 1050 nm.
Pump to signal RIN transfer in fiber OPAs is investigated theoretically and experimentally. For a 20 dB gain, signal RIN is larger than pump RIN by a factor ranging from 2 to 14.
© 2003 Optical Society of America
© 2003 Optical Society of America
We propose and demonstrate a novel scheme to achieve low polarization dependent gain (PDG) forward-pumped Raman amplification via polarization sweeping at 10 GHz. This scheme employs the asymmetry of electro-optic coefficients of LiNbO3 crystals to sweep the pump SOP at 10 GHz across the Poincare sphere.
We present a method using two parallel fiber optical parametric amplifiers (OPAs) and two interleavers, which allow one to either amplify or spectrally invert a broad spectrum. This permits the utilization of the full bandwidth of OPAs and wavelength converters.
We review the characteristics of fiber optical parametric amplifiers, and some of their potential applications. We describe recent developments, and discuss some of the challenges that remain to be addressed before they can be used in optical communication systems.
A fibre optical parametric amplifier with orthogonal circularly-polarised pumps requires only half the pump power of an amplifier with linearly-polarised pumps to achieve a given gain. The gain is also independent of the polarisation of the input signal.
We demonstrated a pulsed-pump fiber optical parametric amplifier followed by a narrow optical filter for transparent signal amplification. Wide gain-bandwidth of 85 nm, large gain of 43 dB, and clear eye-opening were demonstrated for 10 Gb/s-NRZ signals by a 20 GHz asynchronous pulsed pump.
It is shown that, as a first approximation, chromatic dispersion in demultiplexers based on arrayed waveguide gratings (AWGs) is proportional to the local spatial curvature of the wavefronts of the field at the output of the input guide, whose image shifts across the output guide as frequency changes. More accurate results can be obtained by convol...
We demonstrate experimentally a technique to cancel the spectrum broadening in a fiber optical parametric wavelength converter (WC) by using two pumps phase-modulated 180deg out of phase, one of them being obtained by four-wave mixing in an auxiliary fiber. The resulting WC spectrum is comparable to that of the input signal
We report continuous-wave operation of singly resonant fiber optical parametric oscillators. In a cavity formed by 100 m of highly nonlinear fiber and two fiber Bragg gratings, the pump power threshold was 240 mW; the output wavelength could be tuned over 80 nm by tuning of the pump. We also obtained an internal conversion efficiency of 30%, compar...
With a suitable arrangement of two pumps and two signals with
respect to the zero-dispersion wavelength of a fiber, simultaneous
wavelength exchange between two signals can be realized by four-wave
mixing in the fiber. We have demonstrated near-complete wavelength
exchange between two signals at 1573.4 and 1579.9 nm with two 0.25-W
pumps in a 1-km-...
We investigate, theoretically and experimentally, a novel scheme to suppress the crosstalk between wavelengths in wavelength-division-multiplexing (WDM) analog fiber systems. The idea is based on the fact that crosstalk (due to stimulated Raman scattering and cross-phase modulation combined with group velocity dispersion), is caused by the intensit...
We reported on the fast transient response of EDTFAs. The transient time of EDTFAs can be one-ninth as short as that of the EDSFAs with similar gain shape in L-band. We also demonstrated optically gain-clamped EDTFAs and showed that the power excursion due to SHB is comparable to or smaller than that in EDSFAs. The relaxation oscillation frequencie...
Summary form only given. Because wavelength exchange (WE) makes use of four-wave mixing (FWM) between two pumps and two signals, the states of polarization (SOP) of pumps and signals strongly affect its operation characteristics. In this paper, we explore the influence of the SOP of pumps and signals in WE, and show that WE with orthogonal pumps gi...
We have demonstrated polarization-independent operation of a CW fiber optical parametric amplifier using two orthogonal pumps, with 15 dB of gain over a 20 nm bandwidth. This method is compatible with two-pump dithering to avoid idler broadening, and provides a flat-gain spectrum. Another advantage of using this method, compared with a polarization...
We have demonstrated a novel wavelength conversion scheme based on XGM in fiber OPA. The scheme enables the tunable wavelength conversion with a simple configuration, and it is free from linewidth broadening caused by the phase modulation of OPA pump. The signal at 1554 nm was converted anywhere into a 13 nm wavelength range, in either the C band (...
We demonstrate theoretically and experimentally that gain saturation in a fiber optical parametric amplifier (OPA) can be used to efficiently cancel the second-order distortion generated in an analog fiber link by SPM and GVD. We demonstrated reduction of CSO distortion by 12 dB
We designed highly-nonlinear tellurite fibers with zero-dispersion near 1550 nm and the nonlinear coefficient gamma over 200 km<sup>-1 </sup>-W-1 using various structures including tapered fibers and photonic crystal structures. Applications to fiber optical parametric amplifiers (OPAs) are discussed
Summary form only given. We propose a full-vectorial algorithm, which solves the wave equations exactly, without the assumption of de-coupling of the two transverse fields. The algorithm based on Hermite-Gaussian function expansions is efficient because only relatively few terms are necessary to obtain good results. Our algorithm simplifies the ref...
We have obtained analytical expressions for the two-orthogonal-pump optical parametric amplifier (OPA). Our experiments demonstrate good agreement with theory. A perpendicular OPA requires higher pump power than a parallel OPA to achieve the same parametric gain. We also investigated the bandwidths of the two configurations, and proposed a techniqu...
We have demonstrated optical single sideband (OSSB) transmission with standard fibre Bragg grating (FBG). No RF analog circuit is necessary. FBG not only suppress the sideband but also can compensate for chromatic dispersion of the link. The higher data rate is, the better SBSR will be. Therefore, this technique will be ideal for OC768 and beyond....
In summary, we have demonstrated, for the first time to our knowledge, a gain-clamped discrete Raman amplifier in the S-band. The device achieves peak net gain over 22 dB, and a gain variation of only 0.3 dB for signal input power ranging from -20 dBm to 2.7 dBm. Unlike conventional gain-clamping designs, an extinction ratio between signal and lasi...
Theory shows that near-complete pump depletion can be obtained in uniform fiber-optic parametric amplifiers (OPA's) for a particular phase-matching condition. We have demonstrated 92% pump depletion in a cw fiber OPA, with a 200-mW pump at 1560 nm in an 11-km-long dispersion-shifted fiber.
We demonstrate a new S-band nonlinear fibre amplifier, with over 18 dB gain, and S-band wavelength converter, with over 20 nm bandwidth, obtained by combination of Raman gain and optical parametric amplification.
A new all-optical 3R regeneration technique using
injection-locking in a gain-switched DFB-LD is proposed. The operation
of the technique is confirmed numerically and experimentally. Both
simulation and experimental results show that the degraded RZ pulses are
reshaped, retimed, and regenerated by injection-locking, into short
pulses generated by g...
Theory shows that with a suitable choice of the wavelengths of two pumps, and two signals about the zero-dispersion wavelength of a fiber, simultaneous unit conversion efficiency from one signal to the other, and vice versa, can be obtained. We have demonstrated near-complete wavelength exchange between two signal wavelengths, with two 200 mW pumps...
By using complementary modulation of two closely-spaced optical carriers, nonlinear crosstalk on other carriers in WDM analog fiber communication systems can be greatly reduced. We have obtained up to 30 dB reduction at low modulation frequencies, where crosstalk is most severe.
Summary form only given. Devices based on the nonlinear optical susceptibilities χ(2) or χ(3) can be used for performing important functions such as amplification or wavelength conversion. Typically one uses a strong pump, and injects a weaker signal into the device, thereby generating at the output an amplified signal, and a strong idler. In a wel...
Distributed Raman amplification is used to reduce the optical
power launched into the transmission fibre of an analogue communication
system. This reduces all impairments caused by fibre nonlinearities. The
authors have experimentally demonstrated 8-15 dB nonlinear crosstalk
reduction in an analogue wavelength division multiplexed (WDM) system
We fabricated an optimized discrete Raman amplifier with
dispersion compensating fibre (DCF) and evaluated its nonlinearities.
XPM is larger than in a comparable EDFA. By simulations, we revealed
methods to reduce XPM substantially, which is beneficial for wideband
WDM systems
Models are presented which show that, for WDM systems, XPM and FWM
in EDFAs can be far larger for tellurite than for silica (tens of dB
larger for RWM), because tellurite is highly nonlinear. Experimental
results for XPM are presented
© 1999 Optical Society of America
We study in detail the two types of nonlinear crosstalk which
cause severe problems in WDM AM CATV systems. They are respectively due
to stimulated Raman scattering (SRS), and cross-phase modulation (XPM)
interacting with group-velocity dispersion
Nonlinear cross talk and stimulated Brillouin scattering (SBS)
reduction are demonstrated in an analog wavelength-division multiplexing
(WDM) optical communication system using optical carrier suppression.
Cross talk reduction by 20 dB over 2 GHz is achieved. SBS is negligible
without employing any frequency or phase dithering
We demonstrate an optical fibre parametric amplifier concept by measuring the parametric gain on three different combination of fibers including nonlinear fibre and dispersion shifted fibre
Degenerate four-wave mixing (DFWM) in optical fibres can be used to obtain gain and to generate squeezed states, by utilizing a balanced Mach-Zehnder fibre interferometer (MZFI) with two non-linear arms, which behaves as a degenerate parametric amplifier. In a classical derivation for the optical gain; pump depletion and propagation loss are consid...
Crosstalk reduction is demonstrated in a WDM analogue optical
communication system using optical carrier suppression. A crosstalk
reduction by 20 dB over 2 GHz is achieved while maintaining the same
received RF power
When designing optical modulators it is generally desired to
obtain a linear relationship between the applied voltage V and the
output light intensity I, or output field E. Using the Mach-Zehnder
interferometer as a basic component, designs have been found which are
free from harmonic distortion up to the fifth order. We introduce a
novel interfero...
The 1-pump fiber optical parametric amplifier (OPA) with dispersion and loss, but no pump depletion, has recently been characterized by a 2×2 transfer matrix, with each term expressed in terms of four Hankel functions, H<sub>iu</sub> of imaginary order iu. Unfortunately, these functions are not commonly available in mathematical packages such as Ma...
We have introduced the possibility of synthesizing WDM routers
based on N X N hierarchic star couplers. We have examined how the
required phase shifts can be introduced by means of path length
differences, and studied in detail the crosstalk introduced by the
frequency dependence of these phases. We have found that crosstalk
levels are moderate, ev...
We have demonstrated a fiber optical parametric amplifier (OPA)
utilizing a highly nonlinear fiber, which allowed us to obtain
substantial gain with only a 20-m length, over a 24-nm bandwidth, even
though the pump was 49 nm from λ<sub>0</sub>. The availability of
such fibers should greatly facilitate the development of fiber OPAs for
applications s...
Stimulated Raman scattering (SRS) cross talk has been identified
as a major obstacle to the implementation of analog wavelength-division
multiplexing (WDM) optical communication systems. Here we report, for
the first time to our knowledge, a SRS crosstalk reduction obtained by a
cancellation technique. The experimental setup is shown. An optical
ca...
We compare techniques using two fibers connected either in series or in parallel for cancelling cross talk that is due to stimulated Raman scattering in wavelength-division-multiplexed systems. Theory shows that such cross talk can be completely eliminated by a series arrangement in lossy dispersionless fibers by means of midway amplification and s...
We describe, for the first time to our knowledge, experimental demonstration of a pulsed optical parametric amplifier (OPA) with 12 dB maximum gain and a CW OPA with 1.5 dB maximum gain. For the pulsed OPA demonstration, the pumps consisted of a DFB laser at 1555 nm and a tunable external-cavity laser (ECL) operating at 1533.2 nm. For the CW OPA, a...
We have shown that SRS crosstalk in WDM systems can be reduced in
the presence of dispersion by a factor of the order of the Raman gain G,
by either a series or parallel arrangement. In the absence of
dispersion, perfect cancellation can be obtained in the series
arrangement, but not in the parallel one. The parallel arrangement may
be more practic...
Here we report the operation of a fiber optical parametric amplifier (OPA) with sufficient gain to overcome fiber loss, exhibiting net signal gain G, and conversion efficiency G<sub>1</sub> of the order of 5 dB. We present performance results for amplification and wavelength conversion of IMDD and FSK signals
The authors have measured a signal gain of 5 dB and idler
conversion efficiency of 4 dB in a CW fibre optical parametric
amplifier. The broadening of the idler spectrum resulting from pump
dithering used to suppress SBS is observed, and a means to eliminate it
is proposed
By a suitable choice of the wavelengths of two pumps and one signal about the zero-dispersion wavelength of a fiber, it is possible to generate mainly one four-wave-mixing product (idler) whose spectrum is a translated version of that of the signal; no spectral inversion or phase conjugation is involved. Unit conversion efficiency can in principle...
We have shown that the propagation constant mismatch Λβ for a 2-pump fiber OPA can be well approximated by a fourth-order Chebyshev polynomial, by adjusting ω<sub>c</sub>, near ω<sub>0</sub>, and the pump spacing. Very low gain ripple can be obtained over tens of nanometer. This level of performance is not available with any other type of optical a...
Theory predicts that a two-pump fiber optical parametric amplifier or wavelength converter operated near the fiber zero-dispersion wavelength can exhibit a gain spectrum approximated by a Chebyshev polynomial of order 8. Under realistic conditions of pump spacing and fiber dispersion, very low-gain ripple can be obtained over a large bandwidth. For...
Citations
... The optical receiver consist of a telescopic system having a primary and secondary mirror, a block of beam splitter, a spherical aberration from chromatic components and diaphragm placed along an optical axis of the optical receiver. The chromatic component is used to demultiplex the wavelength channels of the input optical beam of the receiver in such a way that channels are focused at different focal planes on the optical axis of the receivers [6,13]. ...
... Optical gain clamping (OGC) has been shown to offer a number of attractive features for improving the performance of EDFAs [6] and Raman amplifiers [7] in dynamic wavelength division-multiplexed (WDM) networks, but is relatively unexplored in FOPAs. Previously, a gain-clamped FOPA (GC-FOPA) was shown theoretically to improve performance for optical packet transmission in FOPAs [8, 9] and gain clamping for a single signal channel was experimentally investigated in [10]. Here, we experimentally investigate the practical viability of using OGC in a dynamic network environment and find only moderate practical benefit in terms in reducing the impact of bit-level XGS but may provide application for static gain control schemes. ...
... Fiber dispersion-induced power fading can be eliminated by using an OSSB signal [21]. Several techniques for implementing an OSSB signal have already been proposed, such as using optical filtering to remove one of the first-order sidebands of DSB signals [22][23][24], dual-drive Mach-Zehnder modulator (DDMZM) [25,26], dual-parallel MZM (DPMZM) [27][28][29], hybrid structure composed of a cascade of an amplitude modulator (AM) and a PM [30,31] and based on a polarization modulator (PolM) [32]. ...
Reference: Bias-free OSSB modulator with tunable OCSR
... Note that the fast response time of the FWM process, which makes FOPAs useful for many important applications, also helps transferring noise from the pumps to the signal efficiently. Several groups have suggested that the noise associated with the pumps is one of the dominant sources of signal SNR degradation [8], [77]- [79], [88]- [91]. Section 5.2 extends the earlier works to the case of dual-pump FOPAs and shows that the group-velocity difference between the signal and pumps has to be taken into account to determine the noise transfer correctly [92]. ...
... In order to address this crosstalk problem, we recently proposed using a hybrid amplifier formed by a fiber OPA with moderate gain, followed by a (non-fiber-OPA) PIA, as a novel and effective means for reducing the FWM crosstalk [16]. This is based on the fact that FWM between signals occurs primarily where signals are the strongest, i.e. near the amplifier output; hence using an amplifier less prone to FWM as a booster will reduce FWM crosstalk (for the same overall gain). ...
... Yam et.al used a pair of band-pass wavelength division multiplexers (WDMs) at the input and output of the RFA. The pass and reflected bands of the WDMS are carefully selected so that the signals and lasing output do not reside in the same band [3]. Bolognini et al. achieved gain-clamping through an optical feedback made of a combination of circulator at the input and a coupler at the output, which generates a counter-propagating laser by filtering a small ASE fraction; a variable optical attenuator (VOA) is used to clamp the gain at different values depending on the span loss which must be compensated by the RFA gain [4]. ...
... Cascade systems are widely used in various electrical and electronics engineering domains such as telecommunications and signal processing [1][2][3][4][5][6][7], circuits [8][9][10][11][12][13][14][15][16], networks and systems [17][18][19][20], solid-state devices [21][22][23][24][25][26][27][28][29], and so on. To extract the actual signal component at the output of these systems, it is critical to calculate its total noise factor (F T ). ...
Reference: Correction to Friis Noise Factors
... where V J 1 J 2 (κ j , κ j ; t, t 0 ) = V J 1 J 2 ;j,j (t, t 0 )/∆κ, (334) W J 1 J 2 (κ j , κ j ; t, t 0 ) = W J 1 J 2 ;j,j (t, t 0 )/∆κ. We note that similar input-output relations were also derived in [72,[97][98][99], albeit with different labels. ...
... Although the FOPAs have their inherent advantage of wide gain bandwidth and are flexible in choosing the gain region via varying pump wavelengths, they offer a low gain, particularly if the number of channels is large. To increase the gain, hybrid FOPAs have been proposed [5][6][7]. A hybrid of FOPA with an erbium-doped fibre amplifier (EDFA) reduces the FWM crosstalk and leads to good gains [7]. ...
... In Ref. [16], a CW single-longitude-mode FOPO was reported, including a saturable-absorber-based Sagnac loop and an erbium-doped fiber. The filters used in the reported CW FOPOs typically have, however, high insertion losses-in the range of 3-5 dB [14][15][16][17][18][19]. These lead to high cavity losses and limitations to further improvement of FOPO performance. ...