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Journal of Electrical and Computer Engineering
Volume 2012 (2012), Article ID 314872, 6 pages
Research Article

All-Optical Fiber Interferometer-Based Methods for Ultra-Wideband Signal Generation

EMAT Laboratory, Electrical Department, Faculty of Engineering, University of Moncton, 18 Avenue Antonine Maillet, Moncton, NB, Canada E1A 3E9

Received 28 October 2011; Accepted 8 April 2012

Academic Editor: Baoyong Chi

Copyright © 2012 Kais Dridi and Habib Hamam. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.


We report two new, simple, and cost-effective all-optical methods to generate ultra-wideband (UWB) impulse radio signals. The proposed methods are based on fiber-interferometric structures, where an input pulse is split and propagates along the two interferometer arms. The interference of these pulses at the output of the interferometer leads to UWB pulse generation. A theoretical analysis is provided and some relevant simulation results are presented. Large bandwidths are obtained while satisfying the requirements of the Federal Communication Commission (FCC). With these two techniques, UWB pulses can be readily generated and cost-effectively propagated through optical fibers.

1. Introduction

Major advances in wireless communications, networking, radar, imaging, and positioning systems have been made since the fast emergence of ultra-wideband (UWB) technology. UWB radio technology converges towards being a strongest candidate compared to the other existing radio technologies. It has gained ground since the USA FCC’s proposed rulemaking. In its Report and Order (R&O) issued in February 2002, large bandwidth from 3.1 to 10.6 GHz has been unleashed with an isotropic radiated power level of less than −41 dBm/MHz. Besides, this radio technology owns its success due to its intrinsic features and benefits including low power consumption, low complexity, low cost, wide occupied bandwidth, high data rates, immunity to multipath fading, and high security [13].

Unfortunately, shot-range propagation is still considered as a main limitation preventing widespread deployment of such technology: transmitted signals can propagate for distances less than 10 meters as illustrated by Figure 1. To overcome this inherent restriction, solutions based on the integration of optical fibers and UWB radio are promising. The idea is to widen the area of coverage by means of small antennas interconnected by optical fibers. Large surface can hence be divided into small picocells where low-power transmitters are used. A key point in such architecture is the fact that UWB pulses are generated from a central station (CS) and distribute to UWB access points (UWB-AP) through optical fibers as shown in Figure 1. This way saves optoelectronic (O/E) conversions, which limit the bandwidth. In addition, it ensures seamless integration with the high-rate optical networks. Thus, UWB over fiber (UWB-o-F) system can be deployed to achieving high data rate access in an indoor environment.

Figure 1: An UWB-o-F system for high data rate coverage (UWBAP: UWB Access Point).

UWB signals have been generated both electronically [48] and optically [922]. Several approaches have been proposed for optical UWB signal generation. For example, monocycle pulses have been generated using a hybrid system based on a gain switched Fabry-Pérot laser diode (FPLD) and a microwave differentiator [9, 10]. Other techniques were based on cross-phase modulation (XPM) [11] and cross-gain modulation (XGM) [12] in a semiconductor optical amplifier (SOA). Birefringence time delay has been also applied by cascading phase modulator (PM) with a polarization maintaining fiber (PMF) [13]. Generation based on the gain saturation of a dark return-to-zero (RZ) signal in an SOA [14] has been also demonstrated. Moreover, other types of UWB signals (e.g., doublet) have been generated based on a Mach-Zehnder modulator (MZM) biased at a nonlinear region [15], a combination of an optical phase modulator with a dispersive fiber [16], and a special frequency shift keying modulator [17], and a conversion from phase modulation (PM) to intensity modulation (IM) is performed by an optical frequency discriminator-based Fiber Bragg Grating (FBG) [1822]. The aforementioned techniques require a lot of adjustment and control to be able to ensure a relative stable UWB pulse generation. This may lead to complex solutions, which will be costly when implementing. In this paper, we advance two new and simple approaches for monocycle and doublet UWB signal generation in the optical domain.

2. Development of the Design Methods

In nonlinear (NL) dispersive fibers, propagation of optical pulses is governed by a propagation equation which can be reduced to the nonlinear Schrödinger Equation (NLSE) under certain conditions [23]. The propagation equation can be written as follows:𝑖𝜕𝑢𝜕𝑧+𝑖𝛽1𝜕𝑢𝛼𝜕𝑡+𝑖21𝑢2𝛽2𝜕2𝑢𝜕𝑡2𝑖6𝛽3𝜕3𝑢𝜕𝑡3+𝛾|𝑢|2𝑢=0,(1)

where 𝑢 is the slowly varying amplitude of the incident pulse envelope, 𝛼 is the attenuation coefficient related to fiber losses effects, and 𝛽2 and 𝛽3 are, respectively, the second- and third-order dispersion parameters: the group velocity dispersion (GVD) ([ps2/Km]) and the third-order dispersion (TOD) ([ps3/Km]) parameters. The nonlinear parameter is represented by 𝛾 known as the self-phase modulation (SPM) parameter. 𝛽1 is the first-order dispersion constant or merely the inverse of the group velocity 𝑣𝑔 ([ps/Km]).

Suppose that a related time frame 𝑇 which is measured in a frame of reference moving with the pulse at the group velocity 𝑣𝑔(𝑇=𝜏(z/𝑣g)=t𝛽1z). The 𝛽1 term of (1) can be omitted. Besides, since pulses are significantly larger than 5 picoseconds, TOD as well as nonlinear effects can also be neglected [24]. In a previous work and for another application a more rigorous analysis including TOD was carried out [24]. However in our present application the pulse width is larger than 10 ps, which means that TOD and nonlinear effects have insignificant meaning. By neglecting the TOD (and preserving the non linear parameter 𝛾for the moment) we obtain𝑖𝜕𝑢𝛼𝜕𝑧+𝑖21𝑢2𝛽2𝜕2𝑢𝜕𝑇2+𝛾|𝑢|2𝑢=0.(2)

Let us consider the case where only the dispersion is dominating and the pulse is propagating in a lossless medium (𝛼=0); (2) can be rewritten as𝑖𝜕𝑢=1𝜕𝑧2𝛽2𝜕2𝑢𝜕𝑇2.(3)

Nonlinearity effects can be neglected under the following condition: 𝐿𝑑/𝐿𝑛𝑙1, where 𝐿𝑑 is the dispersion length expressed by 𝑇02/|𝛽2| and 𝐿𝑛𝑙 is the nonlinear length expressed by 1/𝛾𝑃0. 𝑃0 and 𝑇0 are, respectively, the peak power and initial width for the incident pulse. For given values of the fiber parameters 𝛾 and 𝛽2, 𝑃0 should be ≪1. W and 𝑇0 should be in the picoseconds range.

Consider now a normalized amplitude 𝑠(𝑧,𝜏) introduced as follows:𝑢(𝑧,𝜏)=𝑃0exp𝛼𝑧2𝑠(𝑧,𝜏),(4)

where 𝜏is a time scale—normalized to the input pulse width 𝑇0—defined by 𝑇/𝑇0.

Under all the aforementioned conditions, if we define the normalized amplitude 𝑠(𝑧,𝑇) according to (4), 𝑠(𝑧,𝑇) satisfies the following partial differential equation:𝑖𝜕𝑠=1𝜕𝑧2𝛽2𝜕2𝑠𝜕𝑇2.(5)

The expansion of (5) leads to1𝑖(𝑠(𝑧+Δ𝑧,𝑇)𝑠(𝑧,𝑇))=2Δ𝑧𝛽2𝜕2𝑠𝜕𝑇2.(6)

Let us suppose the difference between the two fields 𝑠(𝑧+Δ𝑧,𝑇) and 𝑠(𝑧,𝑇) as an output signal described by the following expression:𝑠1out(𝑧,𝑇)=𝑠(𝑧+Δ𝑧,𝑇)𝑠(𝑧,𝑇).(7)

Expression (7) represents a spatial difference since it is a difference fulfilled in the space (i.e., 𝑧) domain. In addition to this spatial difference, a temporal difference can be achieved as well. This is done by fixing 𝑧 and varying 𝑇 by a certain delay of 𝜏. Hence, another difference results as𝑠2out(𝑧,𝑇)=𝑠(𝑧,𝑇𝜏)𝑠(𝑧,𝑇).(8)

A Fourier domain analysis tells us that𝑠𝑇𝐹1out(𝑧,𝑇)𝛼𝜔2𝑠𝑆(𝑧,𝜔),𝑇𝐹2out(𝑧,𝑇)𝛼𝜔𝑆(𝑧,𝜔).(9)

Going back to time domain, 𝑠1out and 𝑠2out are proportional to the first and second derivatives of the impulse 𝑠 itself:𝑠1out(𝑧,𝑇)𝛼𝑠(2)𝑠(𝑧,𝑇),2out(𝑧,𝑇)𝛼𝑠(1)(𝑧,𝑇).(10)

Two possible schemes can hence be proposed for the generation of UWB signals. In both cases the first and the second derivates of a Gaussian impulse give the monocycle and the doublet pulses, respectively [25, 26].

2.1. Space-Based UWB Pulse Generation

Figure 2 shows us a clear insight on how a physical implementation for UWB impulses generation would be: an interferometer system having two arms with different lengths 𝑧 and 𝑧+Δ𝑧. The 𝜋-shift element induces a negative impulse.

Figure 2: Possible doublet pulse generation scheme.

In the following analysis, we used the expressions of 𝑠1 and 𝑠2 that can be deduced from the solution of (5) in two different ways:𝑠1=𝑇(𝑧,𝑇)=𝑠(𝑧,𝑇)0𝑇0𝑖𝛽2,1𝑧1/2𝑇exp22𝑇02𝑖𝛽2,1𝑧,𝑠(11)2=𝑇(𝑧,𝑇)=𝑠(𝑧+Δ𝑧,𝑇)0𝑇0𝑖𝛽2,1(𝑧+Δ𝑧)1/2𝑇×exp22𝑇02𝑖𝛽2,1.(𝑧+Δ𝑧)(12)

𝛽2 in (5) is 𝛽2,1.

Equation (12) contains a virtual GVD parameter 𝛽2,2, which is different from the first one (𝛽2,1):𝛽2,2=𝛽2,1𝑧+Δ𝑧𝑧.(13)

So, instead of adding a short fiber-length (Δ𝑧) to the second arm, we can choose a fiber arm as long as the first arm but with a different dispersion parameter as depicted in Figure 3.

Figure 3: Length-dispersion equivalence.

Expression (12) becomes𝑠2=𝑇(𝑧,𝑇)=𝑠(𝑧+Δ𝑧,𝑇)0𝑇0𝑖𝛽2,2𝑧1/2𝑇exp22𝑇02𝑖𝛽2,2𝑧.(14)

For a fixed first arm length 𝑧=𝐿, 𝛽2,2is constant. As a special case, if we fix 𝑧to 𝐿𝑑, which is the dispersion length over which the effects of dispersion become more important (introduced in Section 2), the following relationship will have an important consideration in our simulation:𝛽2,2=𝛽2,1𝐿+Δ𝑧𝐿.(15)

2.2. Time-Delayed UWB Generation

Figure 4 depicts another possible interferometer-based system, which is composed of two optical fiber arms with different lengths, two optical 3-dB couplers, and a 𝜋-phase shifting device. The delay loop element assures a delay 𝜏 between the two arms. Fourier transform of the expression (8) leads to𝑆out𝑒(𝑧,𝜔)=𝑖𝜔𝜏𝑆1(𝑧,𝜔),(16)

Figure 4: Time delay interferometer (OC: Optical Coupler).

where 𝑆 and 𝑆out are, respectively, the Fourier transforms of both the injected and the output pulses. The decomposition of (16) into Taylor basis would lead to (up to the first order)𝑆out(𝑧,𝜔)𝑖𝜔𝜏𝑆(𝑧,𝜔).(17)

From (17) we can make out that the output spectrum is identical to the initial spectrum modulated by a linear function of the frequency. Let us replace 𝑆(𝑧,𝜔) by the following analytical expression:𝑖𝛽𝑆(𝑧,𝜔)=𝑆(0,𝜔)exp22𝜔2𝑧,(18)

where 𝑆(0,𝜔) can be calculated as [18]𝑆(0,𝜔)=2𝜋𝑇0𝜔exp2𝑇022.(19)

Hence, by combining (18) and (19), the spectrum of the output signal becomes𝑆out(𝑧,𝜔)=2𝜋𝑇0𝑒𝑖𝜔𝜏𝑖𝛽1exp22𝜔2𝑧𝜔×exp2𝑇022.(20)

Since the initial spectrum 𝑆(0,𝜔) is as large as that of the propagated signal 𝑆(𝑧,𝜔), the bandwidth of the output signal (the extent of 𝑆out(𝑧,𝜔)) does not depend on 𝑧.

In the two proposed systems, a 𝜋 phase device must be inserted in one arm to implement the negative impulse function. The 𝜋-phase shift element design is not considered in our work; however, it can be implemented such as in [27] or [28].

3. Simulation Results

As a quick proof of concept, we have carried out simulations using the Photonic Transmission Design System (PTDS) simulator produced by Virtual Photonics Inc, known as VPISystems nowadays [29]. It is based on the Ptolemy open-source software [30]. Figure 5 describes a range of parameters that have been manipulated in the purpose of ensuring high-quality monocycle and doublet impulses. The injected impulse is characterized by its initial power (𝑃0) and its full width at half maximum (FWHM). The optical couplers control the amount of power through the interferometer by adjusting the coupling ratios CR1 and CR2. 𝑙1, 𝑙2, 𝛽2,1, and 𝛽2,2are the lengths and GVD parameters of the two optical fiber arms, respectively. The semiconductor optical amplifier (SOA) gives a little amplification for the obtained impulse. In these simulations, it has been controlled through its injection current 𝐼𝑐. A photodetector performs a conversion from the optical to the electrical domain.

Figure 5: UWB pulse generation schema.
3.1. For the Space Approach

In this approach, the interferometer arms’ lengths are chosen equal to 720 m (Figure 5) but with different dispersion parameters −7.34 ps2/km and −5.75 ps2/km. A Gaussian pulse, with an FHWM of 62.5 ps, is injected via the first optical coupler which has a coupling ration CR1 equal to 0.3. A Gaussian doublet has been generated and amplified with an SOA (biased at 150 mA). Table 1 summarizes the interferometer’s parameters used for the doublet generation. A UWB doublet signal has been obtained with an FWHM of about 48.45 ps, as shown in Figure 6, with 10.7 GHz bandwidth (from 2.7 to 13.4 GHz) measured at −10 dB.

Table 1: Doublet generation’s parameters.
Figure 6: The generated doublet (a) and its spectrum (b).
3.2. For the Time-Delay Approach

A 2 mW Gaussian pulse is launched to the interferometer system with an FWHM of about 47 ps (Figure 5). The arms’ lengths are fixed to 720 m and 520 m with the same dispersion parameter of −22 ps²/km. The coupling ratios of the input and output couplers of our system are equal to 0.5 (See Table 2 for the interferometer’s parameters). At the output of the second coupler, the optical monocycle pulse is amplified by a semiconductor optical amplifier (SOA) biased at 120 mA. Table 2 summarized the interferometer’s parameters used for monocycle generation. After the photodetector, the resulted monocycle (Figure 7) measures an upper FWHM of about 40.625 ps and a lower FWHM of about 57.813 ps. It offers a −10 dB bandwidth of about 10.3 GHz from 2.3 to 12.6 GHz (Figure 7). The obtained spectrum respects well the requirements of the FCC spectral mask.

Table 2: Monocycle generation’s parameters.
Figure 7: The generated monocycle (a) and its spectrum (b).

Both symmetry of the monocycle and the bandwidth of its spectrum can be adjusted by tuning the injection current in the SOA. The higher this current is, the more the symmetric pulse is ensured.

The time-delay approach offers a relatively broader spectrum than that obtained with the space approach. On the other hand, from a practical point of view, the latter approach not only requires different and nonstandard dispersion parameters in both arms of the proposed system, but also imposes the use of fiber optic couplers with specific coupling ratios. Conversely, the former approach requires only standard fiber arms (e.g., a standard Corning SMF-28) with 50% fiber optic couplers. The time-delay approach is thus more simple and cost-effective solution for experimental investigation, albeit it shows comparative results with the other method.

4. Conclusion

New all-optical UWB pulses generation methods have been demonstrated and approved by simulations. While the first one is based on time-delay approach to generate monocycle pulse, the second approach has a spatial perspective where the chromatic dispersion is exploited to generate doublet pulse. Both methods use an interferometric architecture incorporating a 𝜋-device shift. Interesting bandwidths have been obtained meeting the FCC requirements. With these methods, not only can UWB pulses be generated optically but also their propagation over optical networks is simply assured. Experimental assessment would be a key point as a future work.


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