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**Numerical Modelling of a High Repetition Rate Fiber Laser, Mode - Locked by **
**External Optical Modulation of a Semiconductor Optical Amplifier **
K. Zoiros, T. Stathopoulos, K. Vlachos, A. Hatziefremidis, T. Houbavlis, T. Papakyriakopoulos and H. Avramopoulos
Department of Electrical and Computer Engineering
Photonics Communications Research Laboratory
9 Iroon Polytechniou Street, 157 73, Zografou, Athens, Greece
Tel : +30 1 772 2076, Fax : +30 1 772 2077, Email : hav@cc.ece.ntua.gr

** **

Abstract

A theoretical study of a high repetition rate laser source based on a novel mode - locking

technique is presented. This technique relies on the fast saturation and recovery of a

semiconductor optical amplifier induced by an external optical pulse and has been used to

obtain 4.3 ps pulses at 20 GHz. A numerical model of the fiber ring laser has been developed

describing the mode - locking process in the laser oscillator and providing solutions for the

steady - state mode - locked pulse profile. The critical parameters of the system are defined and

analyzed and their impact on the formation of the mode - locked pulses is examined. The

comparison between the theoretical results and the experimental data reveals very good

agreement and has allowed the optimization of the performance of the system in terms of these

parameters.

**1. Introduction **

Ultra-high speed multi-access networks are evolving rapidly and are being developed to satisfy

the increasing bandwidth demand due to the massive use of Internet and multimedia. Optical

signal sources capable of generating stable ultra - short pulse trains at high repetition rates and

with a tuning range as wide as possible are key elements for these novel photonic networks that

may combine wavelength division multiplexing (WDM) and optical time domain multiplexing

(OTDM) transmission techniques [1]. Short pulse ultrafast lasers are also necessary for the

performance of ultra - high speed, all - optical logic experiments and the demonstration of all –

optical Boolean functions such as AND and XOR [2], [3]. Active mode - locking is one of the

main methods for the generation of ultra - short transform - limited optical pulses which is

based on the direct modulation of the optical field during each cavity round - trip. At 1.5 μm,

several actively mode - locked fiber lasers employing Er doped fiber as the gain medium and

producing transform - limited picosecond pulses at multi - GHz rates have been demonstrated

[4 - 9]. The majority of these systems uses loss modulation by lithium niobate electro - optic

modulators due to their large electro - optic coefficient and their compact construction on low

loss titanium - indiffused waveguides. Unfortunately, these modulators are highly sensitive to

the polarization state of the input optical field. For this reason, laser sources using lithium

niobate modulators have to be build from polarization preserving fiber pigtailed components

[6], [7] or else suffer from mode - locking loss which limits their operational usability.

Similarly, the use of lightly or moderately doped Er fiber results in long cavities which make

fiber lasers sensitive to small environmental perturbations, such as thermal fluctuations and

acoustic vibration. Although several active stabilization techniques have been developed to

counter the instability of long cavity fiber lasers, these increase the complexity of the system

[8], [9]. In order to solve these problems, semiconductor optical amplifiers (SOAs) have been

deployed in mode - locked laser sources for the generation of short optical pulses at high

repetition rates. The use of an SOA inside the laser cavity is particularly attractive since it can

provide simultaneously gain over a broad spectral range and modulation due to its fast gain

dynamics. Actively mode - locked laser sources with an intracavity SOA have been

demonstrated by several research groups [10 - 15] to generate short optical pulses at various

repetition rates. In these configurations the SOA provides either the necessary gain exceeding

the ring laser cavity loss in combination with an intracavity electroabsorption [10] or

electrooptic modulator [11] or both gain and electrically controlled gain modulation [12 - 15].

This paper presents theoretical results obtained from an actively mode - locked fiber ring laser

source that uses a single SOA to provide both gain and gain modulation via cross gain

saturation from an external optical pulse train. This source is very simple to build from

commercially available components and has been shown to be capable of producing nearly

transform - limited 4.3 ps pulses at 10 and 20 GHz over 16 nm tuning range [16]. The novel

configuration results in a stable oscillator since the use of a single active element to provide

both gain and modulation renders the cavity short. Furthermore, the cavity is nearly

polarization insensitive as there is no lithium niobate modulator and the SOA is operated under

heavy saturation providing nearly polarization independent gain. A mathematical model of the

fiber ring laser has been developed describing the mode - locking process in the laser oscillator

and providing solutions for the steady - state mode - locked pulse profile. A complete

investigation on the critical parameters that determine the width, energy and position of the

mode - locked pulse relative to the external pulse has been performed. These parameters include

the small signal gain and carrier lifetime of the SOA, the cavity loss and the pulse energy and

width of the external modulating signal. From the analysis carried out it has been found that the

minimum pulse width is obtained when these parameters are adjusted so that the mode - locked

pulse forms in the middle between two successive external pulses and that this condition

corresponds to the case where the energies of the external and mode - locked pulses are nearly

equal. A rule of thumb has been also derived concerning the relationship between the operating

repetition period and the carrier lifetime of the SOA which is particularly important when the

fiber ring laser source is used for ultra - high speed all - optical applications.

**2. Model for mode - locking using optical gain modulation of a semiconductor optical **
**amplifier **
Mode - locking is a well known technique for the generation of ultra - short pulses and has been studied theoretically by several research groups [17 - 19]. In particular, active mode - locking has received considerable theoretical interest including analytical [20], [21] and numerical treatment [22], [23] for the estimation of mode - locked pulse characteristics. This section presents the numerical model that describes the mode - locking process of the SOA fiber ring cavity. The model follows the unidirectional propagation of the pulse around the cavity as it is shown in the block diagram of Figure 1. The operations considered inside the ring cavity are (a) saturable gain in the semiconductor laser optical amplifier (SOA) by the externally introduced pulse and the circulating mode-locked pulse, (b) bandwidth limitation of the circulating pulse with an optical filter and (c) linear losses that are present in the cavity.

**Spec** **tral**
** Saturable**
**Filtering**
Figure 1. Block diagram of fiber ring laser source used in simulation

The parameters of the model are assumed to take values for which the oscillator operates under

steady - state mode - locked condition. The pulse is therefore assumed to reproduce itself after

one complete circulation around the laser cavity without any changes in the width or the energy,

apart from a small temporal displacement. The other implicit assumptions which have been

made in order to obtain the solutions are as follows: (a) The electric field of the circulating

mode - locked pulse is assumed to be linearly polarized along the SOA axis of peak gain, (b)

Changes in the mode - locked pulse profile due to its transit through each cavity element are

small. As such, Taylor expansions of exponential terms to the first order incur small errors in

the analysis, (c) The pulse energy of the external optical pulse and the circulating mode - locked

pulse is assumed to be low enough compared to the saturation energy of the SOA. As a result of

this, the gain coefficient of the SOA may be expanded up to second order with respect to pulse

energies, (d) The bandwidth of the mode - locked pulse is assumed to be small compared to the

bandwidth of the spectral limiting element in the cavity and Taylor expansion to second order of

the pulse spectrum in the frequency domain is appropriate.

**2.1 Steady - state equations **

The profile of the output pulse after the consecutive transit through the SOA, spectral filtering

and after encountering the cavity linear losses can be expressed as the successive operation of

three operators 1

Oˆ , Oˆ2 and Oˆ3 on the input pulse profile Ein(t)
T is the transit time of the pulse through the SOA, 2
pulse experiences when travelling from the exit of the SOA to the exit of the filter and 3
temporal delay that the pulse experiences to travel from the exit of the filter to the entrance of the SOA. In this expression, 1
Oˆ is defined as the gain operator of the SOA acting on the
, with G(t) being the time - dependent power
ˆ 2 is defined as the time domain transfer operator of the pulse
is related to the full width at half
f , of the filter transfer function by ω
, where L is the power linear loss coefficient of the
system. On the assumption that the profile change per pulse transit is small, the exponential terms in equation (1) may be expanded to first order providing
is the round trip time of the laser cavity, which for simplicity is
assumed to be equal to the repetition period, Text , of the externally introduced pulse train. In order to obtain closure and a steady - state solution for the mode - locked pulse, the mode - locked pulse is assumed to reproduce itself after each complete transit through the SOA, filter and losses. The gain of the SOA is also assumed to recover to the same value before each mode - locked pulse enters it. In order to accommodate small temporal shifts, δT, of the pulse around its peak as a result of the gain saturation in the SOA, the self - reproducing pulse profile principle is applied by requiring that Eout
where we have introduced the normalized parameters
Specifically, g(t) is the gain coefficient of the SOA normalized to the linear loss coefficient and δ is a time delay (or advance) parameter indicating whether the pulse repetition period deviates from the free space round trip time R

The solution of this steady - state equation for the recirculating mode - locked pulse requires the

calculation of the time dependent normalized gain coefficient g(t). For this purpose, we consider

in 2.2 the gain dynamics of the SOA during its gain saturation and recovery periods. In the

analysis that follows, the external pulses are temporally separated from the mode - locked pulses

by an unknown parameter, Ts , that is assumed to be large compared to the width of the two

pulses. Physically, this means that the external pulse energy does not play any direct role in

saturating the gain of the SOA during the presence of the mode - locked pulse and therefore

need not be taken into account in equation (3) explicitly. The effect of the saturation of the SOA

by the external pulses is however taken into account in calculating the input gain parameter at

the entrance point of the mode - locked pulses as will be described in 2.4.

**2.2 Semiconductor optical amplifier gain dynamics **

The ordinary differential equation that governs the temporal saturation for each point in the pulse is [24]
is the integrated small signal gain normalized to the cavity linear
losses and Jsat = ωoΑ/σ is the saturation energy of the amplifier. The parameters tcar , εο , A, Γ, σ, ωo , o
I are the carrier lifetime, the dielectric constant in vacuum, the cross section
area of the active region, the confinement factor, the transition cross section, the photon energy

and the carrier density and injection current required for transparency, respectively.

**2.3. Gain saturation by a short optical pulse **

Equation (4) can be now used to obtain the gain saturation of the SOA for a short optical pulse,

on the assumption that the width of the pulse is much smaller than the carrier lifetime of the

amplifier [24]. This in practice means that the optical pulse is so short that the gain has no time

to recover during its duration and the first term in the right hand side of equation (4) can be thus

neglected. Assuming also for simplicity that around the peak of the mode - locked pulse g(t) is

close to 1 so that the exponential term may be expanded to first order, the resulting normalized

time dependent gain g(t) is

gin is the gain before the arrival of the recirculating mode - locked optical pulses and
is the instantaneous energy of the mode - locked pulses entering
the SOA. The exponential of (5) may be expanded, according to the assumptions already stated, into second order Taylor series and substituting in (3) yields
The solution of this equation requires the knowledge of p
recovery analysis that follows.

**2.4. Gain recovery **

After the saturation of the SOA according to (5), the gain recovers due to the injection of carriers by the injection current. The gain recovery can be calculated, assuming that the stimulated recombination term (second term) in the right hand side of (4) can be neglected, from
where gf is the gain of the saturated SOA immediately after the transit of a pulse through given by
g and Jtotal are the SOA gain and pulse energy immediately before the pulse
entrance into the SOA. Given that two different sets of pulses transit the SOA at different times, i.e. the external and mode - locked pulses, the recovery of the SOA must be accounted separately for these sets of pulses. For this reason, in
takes the values Jp and Jext for the mode - locked and external pulses, respectively. In order to obtain the steady - state condition for the laser oscillator, the gain of the SOA is assumed to recover always to the same level p
external pulses enter it, respectively. As the mode - locked pulse forms at time Ts after the external pulse has entered the SOA, its gain has had Ts T time to recover to the value p
before the arrival of the mode - locked pulse, where ΔΤ
text being the width of the external pulse. Similarly, the external pulse experiences a gain equal
in which has recovered from the saturated value g after the mode - locked pulse exits the
time has elapsed. The equation of the recovery of the SOA is thus
split in two equations which describe the SOA recovery after the transition of the external and mode - locked pulses, respectively. Equations (7) and (8) yield
gin is eliminated and an expression is obtained which involves only
are the normalized to the SOA saturation energy energies of the
mode - locked and external pulses respectively, A

**2.5 Solution **

In order to obtain a steady - state solution for the mode - locked pulse profile in terms of its

width and energy, the mode - locked pulses are assumed to be squared hyperbolic secant in

shape with total energy Jp so that the electric field is given by

p is related to the full width at half maximum, FWHM
Squaring (12) and integrating over the time dependent variable we obtain
Substituting (12) and (13) and equating the coefficients of the same order terms in (6), the following equations are derived
Equations (11), (14), (15) and (16) form a set of nonlinear equations with unknowns t p , Uo ,

(11), (17), (18) and (19) form the final set of equations for the calculation of t pΔωc .

**3. **
**Results of the self - consistent model and discussion **
**3.1 Calculation of **FWHM

U is performed by setting equation (11) equal to (17) and
substituting the known values of the period and pulse width of the external pulse train, the SOA carrier lifetime and the cavity loss. The derived equation in x is however transcendental and requires numerical solution. In order to solve the transcendental equation and find the unknown x, the parameters α and Ts are scanned in accordance with the experimental conditions for a given value of the normalized small signal gain, ss
g , which is the only independent variable of
the nonlinear system of equations. The unknown x is also scanned within a range whose lower limit is determined by the fact that the normalized energy of the mode - locked pulses must be always less than the normalized energy of the external pulses. Note that due to the form of the transcendental equation, the same combinations of the values of o
multiple solutions of x. The selection of the single x solution and the elimination of the others is performed by choosing the value that corresponds to the smallest pulse width. Therefore, by solving the system for minimum pulse width, the optimum value of Ts and α is obtained for the given ss
g . The value of x that corresponds to this set of ss
g , α and Ts is then replaced in (19) to
calculate t pΔωc and the desired value of FWHM

**3.2 Simulation results and discussion **

Simulation results were obtained for repetition frequencies at 10 GHz and 20 GHz in order to

compare them to the experimental ones. The parameters used for the simulations were chosen to

agree with the values in the experimental configuration [16]. Specifically, the width of the

external pulses was 8 ps, the cavity loss was 15 dB and the full width at half maximum of the

spectral limiting filter was 5 nm for both frequencies. The small signal power gain coefficient

that was used in the calculation of the normalized to the loss small signal gain, gss could take

values in the range 19.2 - 25.2 dB, in accordance to the gain characteristic of the SOA. The

values also of the carrier lifetime were selected to be 100 ps at 10 GHz and 70 ps at 20 GHz in

order to match the theoretical and experimental data provided for the 500 μm SOA that was

used in the experiment. The decrease of the carrier lifetime at the higher repetition frequency is

a result of the higher current at which the SOA has to be driven [25], [26] to account for twice the number of pulses entering the amplifier. The carrier lifetime is a particularly important parameter because it defines the range of repetition frequencies at which the ring laser may be operated for a given SOA, as it will be discussed with the simulation results at 20 GHz. Figure 2 (a) shows the variation of the pulse width, FWHM
the mode - locked pulse as well as of the required external pulse energy, α, against the normalized small signal gain coefficient, gss , at 10 GHz. This figure shows that as the normalized small signal gain increases, the energy of the mode - locked pulse also increases saturating the SOA more strongly and leading to pulse narrowing. Similarly, the energy of the external pulse must also be increased to preserve the condition of shortest pulse from the oscillator. The width of the shortest mode - locked pulse decreases up to a minimum value as the normalized gain increases. The minimum pulse width was obtained for 1.53 normalized small signal gain and was 4.5 ps assuming a filter bandwidth of 5 nm in the experimental system. The value of the mode - locked pulse energy, Uo , is either slightly less than or nearly equal to that of the external pulse, α. At the point of minimum pulse width, o
0.45 and nearly equals α which is 0.46. The SOA is already heavily saturated at the same point and a further increase in the gain beyond this point requires a further increase in the energy of the external pulse, which does not allow an increase in the energy of the mode - locked pulse and results in an increase of its pulse width. Figure 2 (b) illustrates the variation of the temporal separation, Ts , between the mode - locked and external pulses and for convenience the pulse width, FWHM
versus the normalized small signal gain, gss , at 10 GHz. This figure shows that provided the conditions for best pulse width are maintained, the mode - locked pulse forms at 48 ps, approximately half way between two successive external pulses, despite large variations in gss . As the small signal gain increases, the mode - locked pulse moves away from the half way point and closer to the leading of the external pulses. This is due to the fact that as the small signal gain increases, the gain recovers above the losses in the cavity earlier, forcing the mode - locked pulse to move forward. However, the excess gain increases very gradually so that the mode - locked pulse moves very slowly towards the leading of the two consecutive external pulses. From the observation and analysis of Figures 2 (a) and (b) it can be deduced that two conditions must be fulfilled in order to obtain mode - locked pulses with the minimum possible width. The first is that the normalized energies of the mode - locked and external pulses must be nearly equal. This condition alone is not sufficient since there is a large set of parameter values for which the normalized energies are equal but the pulse width is not globally minimum as seen in Figure 2 (b). This leads to the second condition which states that the mode - locked pulse must form nearly equidistantly between consecutive external pulses. When both conditions hold, the fiber ring laser system generates the shortest pulses. Figure 2 (c) displays the variation of the time delay, Ts , between the mode - locked and external pulses against the energy of the external pulse normalized to the saturation energy of the SOA. The results shown are for operation of the laser at 10 GHz with the normalized small signal gain set at 1.53. The figure shows that as the energy of the external pulse increases, the mode - locked pulse becomes increasingly delayed with respect to the leading of the two successive external pulses. This is a consequence of the deeper saturation into which the SOA is brought by the external pulse as its energy increases, which in turn requires a longer recovery time for the gain of the SOA to overcome the cavity losses and allow the mode - locked pulse to form. In the same figure the variation of the pulse width against the normalized external pulse energy has been plotted. As seen, the pulse width
reaches a minimum value for α = 0.46 and forms roughly half way between two consecutive external pulses. Further increase of the external pulse energy beyond this point delays the formation of the mode - locked pulse further and results in its broadening. Figure 2. 10 GHz sim
g . (b) Variation of the time separation between the m
between the mode - locked and external pulses,
The model was next used to evaluate the performance of the laser system as the repetition frequency of the external pulse train was increased to 20 GHz. In order to examine the behaviour of the model, initially the same values for the physical parameters were used as in the case for 10 GHz operation. This time, however, the width of the mode - locked pulses was longer than that of the external pulses. Note that an increase in the repetition rate of the oscillator restricts the range of values that Ts may take, so that there is no overlap between the external and mode - locked pulses. The parameter that most critically determines the quality of mode - locking, however, is the carrier lifetime of the SOA. If the recovery time is far too short for a given repetition period, the gain of the SOA recovers too fast so that the mode - locked pulse forms early behind the external pulse. This allows excess gain to build at its trailing edge, resulting in longer mode - locked pulses. On the contrary, if the recovery time is far too long, the mode - locked pulse trails too far behind the external pulse and has insufficient energy to strongly modulate the gain of the SOA, being therefore long again. In order to obtain a rule of thumb for the carrier lifetime, the theory of standard mode - locking is considered which stipulates that mode - locked pulses form in a laser cavity if the normalized gain function g(t) is greater than 1 just as the pulse forms. In all other instances, that is ahead and behind the pulse, g(t) must be smaller than 1. In this sense and so as to ensure pulse formation, the carrier lifetime must be selected so that gp 1
. Applying first and second order Taylor expansion
approximations in (5) and (11), these inequalities hold simultaneously if
which sets a lower and an upper limit for the amplifier carrier lifetime with respect to the repetition period and the width of the external pulse. This condition implies that for the mode - locked pulses to form, the carrier lifetime of the SOA must decrease as the operating frequency of the ring laser increases. The inverse relationship between the carrier lifetime and the operating frequency may be explained if the roles of the frequency and small signal gain in the mode - locking process are considered. Specifically, an increase of the operating frequency requires an increase of the small signal gain in order to compensate the decrease in energy of the mode - locked pulses due to the larger number of pulses entering the amplifier per unit time. Experimentally, an increase of the small signal gain of the SOA is achieved with a higher drive current which also results in a decrease of its carrier lifetime [25], [26]. Following the preceding analysis, the carrier lifetime used in the 20 GHz simulation was set to 70 ps. Figure 3 (a) depicts the variation of the pulse width and the normalized energy of the mode - locked and external pulses as the normalized small signal gain coefficient is varied at 20 GHz. The behaviour of the oscillator is very similar to that presented in Figure 2 (a) for the 10 GHz
case. The minimum pulse width obtained was 3.9 ps for an increased normalized small signal gain of 1.83. Despite the increase in the small signal gain, the energies of the mode - locked and external pulses were lower than the 10 GHz case, due to the heavy saturation of the SOA, but were again nearly equal at the point of minimum pulse width ( o
the same value of small signal gain as for the 10 GHz operation is used, the mode - locked pulses are longer, 7 ps, with lower energy, o
Figure 3 (b) shows the variation of the time separation between the mode - locked and external pulses, Ts , versus ss
g . The pulse width of the mode - locked pulses is also included so as to
compare with the results from Figure 2 (b). The variation of the position of the mode - locked pulse at 20 GHz has similar behaviour as at 10 GHz, that is, as the small signal gain increases, the mode - locked pulse moves forward towards the leading external pulse. The minimum pulse width is obtained for Ts = 25 ps, half way between two consecutive external pulses.
Figure 3. 20 GHz simulation. (a) Variation of the mode - locked pulse width, FWHM, the normalized energy of the mode - locked, o
U , and external pulses, α, versus the normalized
g . (b) Variation of the time separation between the mode - locked and
external pulses, Ts , versus the normalized small signal gain, ss
In order to assess the ability of the model for quantitative prediction, the parameter values from the experimental set up were substituted in equations (11), (14), (15) and (16). At 10 GHz, with an experimental value for ss
g 1.53 and using a filter of 5 nm spectral bandwidth and external
modulating pulses of 8 ps width, the model predicts mode - locked pulses of 4.5 ps duration

with normalized energy 0.45 and external pulses with normalized energy 0.46. In this instance

the mode - locked pulse forms 48 ps behind the external pulse. At 20 GHz, for an increased

normalized gain of 1.78, the model predicts mode - locked pulses of 4.5 ps duration and 0.34

normalized energy forming 26 ps behind the external pulses of 0.35 normalized energy.

Experimentally, the shortest pulse train had 4.3 ps duration and formed 49 ps behind the

external pulses at 10 GHz. At 20 GHz, the corresponding values were again 4.3 ps and 24 ps

delay behind the external pulses. The agreement thus between the experimental and the

theoretical values for the pulse width and the relative delay is exceptionally good given the

simplicity of the model and suggests its robustness to the approximations that necessarily had to

be made.

**4. Conclusion **

We have presented a theoretical study of the performance of a high repetition rate laser source

that exploits the fast saturation of an intracavity semiconductor optical amplifier, forming the

gain element in its cavity, from an external optical pulse to generate ultrashort pulses. A

complete and computationally simple numerical model has been developed to provide solutions

for the steady - state mode - locked pulse profile in terms of the critical parameters of the

system. The results indicate that the minimum pulse width is obtained when these parameters

are adjusted so that the mode - locked pulse forms in the middle between two successive

external pulses and that this condition corresponds to the case where the energies of the external

and mode - locked pulses are nearly equal. A practical rule of thumb has been also derived

concerning the optimum combination of the SOA carrier lifetime and the repetition frequency

that is required for the novel ring laser to be used as a high repetition rate source for

transmission or optical logic experiments. The comparison of the experimental and theoretical

results has revealed an excellent agreement between them and has helped to provide a thorough

explanation of the mode - locking process.

** **

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