Download Tunable delay slow-light in an active fiber Bragg grating

Tunable delay slow-light in an active fiber Bragg
grating
Kai Qian, Li Zhan*, Honggen Li, Xiao Hu, Junsong Peng, Liang Zhang, Yuxing Xia
Department of Physics, State Key Lab of Advanced Optical Communication Systems and Networks, Shanghai Jiao
Tong University, Shanghai, 200240, China
*[email protected]
Abstract: We proposed and experimentally demonstrated an extremely
simple and feasible slow-light technique to achieve tunable optical delay by
using the Er/Yb codoped fiber Bragg grating (FBG). The signal light
experiences strong dispersion when it is launched into the reflection edge of
FBG, and the group delay value is determined by the signal wavelength and
the pump power. In the experiment, a controllable delay of 0.9 ns can be
obtained through changing the 980nm pump power. The group velocity can
be slowed down to 5.6 × 107 m/s, which is 19% of the speed of light in free
space. It provides a very simple approach to control the light group delay,
which is likely to have important implications for practical applications.
©2009 Optical Society of America
OCIS codes: (060.3735) fiber Bragg gratings; (260.2030) Dispersion; (060.2310) fiber optics;
(999.9999) slow light.
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1. Introduction
Controlling the group velocity of light has been attracting more interests owing to its potential
application as tunable optical buffer in all-optical router commutation and optical computing.
Thus, the techniques of tunable slow-light have been widely studied, such as
electromagnetically induced transparency (EIT) [1], coherent population oscillation (CPO) [2–
5], coupled resonator induced transparency (CRIT) [6], stimulated Raman scattering (SRS)
[7], fiber optical parametric amplifier (OPA) [8] and hybrid approach employing wavelength
conversion with the linear dispersion [9,10]. Stimulated Brillouin scattering (SBS) slow light
has attracted much attention because it can generate large delays at any wavelength and only
requires low-power pump [11–14]. However, its narrow bandwidth does not allow delaying
the narrow pulses [15], and thus SBS slow-light usually requires a relatively complicated
system to improve the operating bandwidth [15–17].
FBGs have been applied as key fiber components in many fields such as dispersion
compensators, wavelength converters and phase conjugators for their versatility and unique
filtering capabilities [18]. In 2005, D. Janner, etc. reported the group velocity reduction by
using Moiré fiber gratings [19]. The delay can be tuned when the signal wavelength shifts the
center of the transmission band. However, the practical systems don’t allow changing the
signal wavelength. In 2006, J. T. Mok, etc. reported the slow light properties of gap solitons in
an apodized FBG [20]. Using a high power signal, the optical nonlinearity induces an index
change of FBG. Thus, the delay can be modified by varying the signal power. In addition, the
dispersion effect can be eliminated through the soliton formation. However, this approach
requires very high power signal (~2 kW), which limits its practical implications.
In this paper, a simple technique to obtain tunable delay is experimentally demonstrated by
utilizing an active FBG written on Er/Yb codoped fiber. Since the reflection phase of FBG
tends to vary rapidly near the band edges, the delay nearby becomes appreciable [21]. The
time delay from the FBG reflection varies with the reflection spectrum shift when changing
the pump power. In the experiment, we obtain a tunable delay of 0.9 ns for a 200 MHz signal
with changing the 980nm pump powers. This scheme is very simple, and cost-effective. It
may have important implications in the practical systems, such as data synchronization and
optical phase array antenna [22–24].
2. Theory
The characteristics of FBG can be calculated using the coupled mode theory [21,25]. The
reflection coefficient can be written as
ρ=
#117459 - $15.00 USD
(C) 2009 OSA
−κ sinh( κ 2 − σˆ 2 L)
σ sinh( κ 2 − σˆ 2 L) + i κ 2 − σˆ 2 cosh( κ 2 − σˆ 2 L)
,
(1)
Received 21 Sep 2009; revised 30 Oct 2009; accepted 3 Nov 2009; published 19 Nov 2009
23 November 2009 / Vol. 17, No. 24 / OPTICS EXPRESS 22218
where κ = π n1 λ is the coupling coefficient, n1 the spatial modulation amplitude, and λ the
wavelength, σˆ is the AC coupling coefficient and σˆ = δ + iα , α is the gain (or loss)
1 1 
constant, δ = 2π neff  −
 is the detuning to the Bragg wavelength λD = 2neff Λ , Λ is the
 λ λD 
period, neff is the effective index, and L is the FGB length. The group delay reflected by the
FBG is
τ =−
λ 2 dϕ
,
2π c d λ
(2)
where ϕ is the phase of the reflection coefficient and can be expressed as
 κ 2 − σˆ 2

coth( κ 2 − σˆ 2 L)  .
σˆ


ϕ = −a tan 
(3)
Fig. 1. Calculated reflection spectrum (solid line) and group delay (dash dot line) in FBG.
We calculated the reflection spectrum and the group delay of a 3.5-cm-long FBG with the
Bragg wavelength of 1545.611 nm and the spatial modulation amplitude of 0.53 × 10 −4 . As
shown in Fig. 1, the group delay becomes appreciable near the edges of the reflection band.
Since the core refractive index of the active fiber varies with the pump power [26], the
reflectivity spectrum may be changed if varying the pump power. Thus, for a signal with the
central wavelength near the band edges of the FBG, an appreciable tunable optical delay can
be obtained with different pump powers. Although the same effect can be obtained by thermal
or mechanical means, these approaches are not compatible with practical systems for their
long response time. This optical approach is considered owing to the short response time of
optical signal processing.
3. Experiments and results
Figure 2 shows the experimental setup to achieve the tunable slow-light in the active FBG.
The continuous light from a tunable laser source is modulated by an electro-optic modulator to
produce the signal of 200 MHz sinusoidal pulse train, whose average power is 3mW. A ~3.5cm FBG written on 2-m-long Er/Yb codoped fiber is pumped by a 980 nm laser diode. The
pulse train is reflected by the FBG and output from the port 3 of the circulator. The tunable
delay of the probe pulse reflected by the FBG is measured by a high-speed oscilloscope after
opto-electrical conversion.
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Received 21 Sep 2009; revised 30 Oct 2009; accepted 3 Nov 2009; published 19 Nov 2009
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Fig. 2. Experimental setup: TLS, tunable laser source; PC, polarization controller; EOM,
electrooptic modulator; WDM, 980 nm/ 1550 nm wavelength division multiplexer.
Fig. 3. Measured reflection spectra of the FBG at different pump powers.
In the active fiber, the core refractive index changes as a consequence of the variation of
the pump power [26]. The Bragg wavelength of a FBG is linearly proportional to the effective
index, which is approximately equal to the core refractive index in the uniform FBG. Figure 3
shows the measured reflection spectra of the FBG with different pump powers. When the
pump power increases from 0 mW to 160 mW, the reflection spectrum shift is about 0.01 nm.
The estimated core index change ∆n is ~ 9.4 × 10−6 . The threshold of active fiber relies on the
active fiber length. When the pump power is close to the threshold, the index variation is
relatively sensitive [26]. In fact, the threshold pump power is only several milliwatts for this
about 3.5-cm-long active FBG. Thus, several milliwatts pump power is adequate to control the
signal. However, 2-m-long Er/Yb codoped fiber used here enhance the threshold to several
tens of milliwatts. The long active fiber used here contributes to the improvement of the
output power and the signal quality.
Figure 4 shows the traces of the signal pulses for different wavelengths. From Fig. 4(a),
without pumping, when the signal wavelength is tuned to the reflection edges of the FBG,
1545.622 and 1545.698 nm respectively, about 0.3 ns delay for both situations can be obtained
compared to the case of the Bragg wavelength of 1545.660 nm. As shown in Fig. 4(b), when
the pump power is 160 mW, the wavelength of the reflection edges is 1545.635 and 1545.711
nm respectively. The Bragg wavelength is 1545.673 nm. About 0.013 nm reflection spectrum
shift can be observed. In addition, under zero pump power, the signal reflected from the FBG
band edges experiences large distortion because the power is too low to detect, which is
shown in Fig. 4(a). When the pump power is 160 mW, the relatively high signal power can be
obtained. The signal distortion can be optimized.
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Received 21 Sep 2009; revised 30 Oct 2009; accepted 3 Nov 2009; published 19 Nov 2009
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Fig. 4. Delayed pulse obtained by varying the signal wavelength when pump power is (a) 0
mW (b) 160 mW.
Fig. 5. Observation of delay or advancement with different pump powers when the signal
wavelength is at 1545.704 nm.
Figure 5 shows the signal traces under different pump powers when the signal wavelength
is set at 1545.704 nm. This wavelength is on the first right side lobe of the FBG reflection
band when zero pump power. When the pump power increases to 100 mW, about 0.5 ns delay
is obtained. The delay decreases gradually when the pump power increases from 100 mW to
130 mW. The pulses experience 0.4 ns advancement when the pump power is 160 mW. In
short, when the pump power increases from 100 mW to 160 mW, up to 0.9 ns controllable
delay has been obtained. From the parameters mentioned above, the group velocity can be
estimated about 5.6 × 107 m/s, which is about 19 percent of the speed of light in free space.
Figure 6 shows the theoretical simulation for this process. We assume the delay spectrum
shift is proportional to the pump power. The assumption is reasonable for the pump power is
close to the threshold. The signal wavelength is set near the first right side lobe of the
reflection spectrum. The calculated delay value varies with pump power. It increases from
0.17ns to 0.42ns when pump power rises from 0 mW to 100 mW, but declines to 0.25ns when
pump power continues to rise from 100 mW to 130 mW and to 0.16ns when pump power
from 130 mW to 160 mW.
The above theory, in which the reflection spectrum shift owing to the pump variation is
considered as the only factor to influence the delay, can explain the variation tendency of
delay; especially why the maximum delay occurs when the pump power is ~100 mW. The
discrepancy between the theory and the experiment is probably due to the shape changing of
the reflection spectrum line in the active FBG.
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Received 21 Sep 2009; revised 30 Oct 2009; accepted 3 Nov 2009; published 19 Nov 2009
23 November 2009 / Vol. 17, No. 24 / OPTICS EXPRESS 22221
Fig. 6. Calculated delay spectrum shift for the FBG with different 980 nm pump powers. The
inset illustrates the details of the delay varying with the reflection spectrum shift.
Compared with other approaches, this slow-light approach has many advantages. First,
only a 980 nm pump and an active FBG are used to generate tunable delay. It is an extremely
simple and very feasible slow light technology to achieve tunable delay. Besides, the delay
value and the signal bandwidth rely on the characteristics of FBG. For example, shorter FBG
length leads to broader bandwidth and smaller delay value. Actually, there is a trade off
between the group delay and the signal bandwidth [27], but this should be further improved
through optimizing the FBG parameters. The fractional delay is 18% in our experiments. Note
that the delay here doesn’t depend on the bit rate of the signal. The larger fractional delay may
be obtained using the higher bit rate signal. On the other hand, larger fractional delay can be
obtained by cascading the grating in a serial manner. In addition, the signal is amplified in the
active fibers, which provides a lossless or even gain slow-light approach.
4. Conclusion
We have experimentally demonstrated a very simple tunable delay slow-light scheme. Up to
0.9 ns delay is achieved by using a cheap and accessible and controllable active FBG by
varying the pump power. The group delay generated by the FBG reflection becomes
appreciable near the band edges of the reflection spectrum, and the reflection spectrum of the
active FBG shifts with the pump power. We believe that this simple, feasible, cost-effective
slow light approach will have a great future in developing optical data synchronization and
optical phase array antenna.
Acknowledgements
The authors acknowledge the support from the National Natural Science Foundation of China
of Grant 10874118, the key project of the Ministry of Education of China of Grant 109061,
and the “SMC Young Star” Scientist Program of Shanghai Jiao Tong University.
#117459 - $15.00 USD
(C) 2009 OSA
Received 21 Sep 2009; revised 30 Oct 2009; accepted 3 Nov 2009; published 19 Nov 2009
23 November 2009 / Vol. 17, No. 24 / OPTICS EXPRESS 22222