CW-to-pulse conversion using temporal Talbot array illuminators.

We report on the linear conversion of continuous-wave (CW) laser light to optical pulses using temporal Talbot array illuminators (TAIs) with fractional orders 1/q(q≤10), implemented by use of multilevel PM and dispersive propagation in a chirped fiber Bragg grating. The generated, sub-nanosecond optical pulse trains have repetition rates in the gigahertz range and show the presence of satellite pulses originated by the finite electrical modulation bandwidth (7.5 GHz). Though this fact impacts the resulting extinction ratio, an experimental comparison with time and Fresnel lenses indicates that temporal TAIs represent compact systems with high light gathering efficiency (>87%) at moderate values of compression (q≤8), which can be tailored in repetition rate, gain, or width, through the fractional Talbot order for its use in pulse compression systems fed by CW light.

[1]  C. Fernández-Pousa,et al.  On the structure of quadratic Gauss sums in the Talbot effect. , 2016, Journal of the Optical Society of America. A, Optics, image science, and vision.

[2]  José Azaña,et al.  Linear optical pulse compression based on temporal zone plates. , 2013, Optics express.

[3]  J R Leger,et al.  Efficient array illuminator using binary-optics phase plates at fractional-Talbot planes. , 1990, Optics letters.

[4]  Daniel R. Grischkowsky,et al.  Temporal compression of light , 1978 .

[5]  John E. Bjorkholm,et al.  Conversion of cw light into a train of subnanosecond pulses using frequency modulation and the dispersion of a near‐resonant atomic vapor , 1975 .

[6]  S. Kawanishi,et al.  Optical pulse generator using phase modulator and linearly chirped fiber Bragg gratings , 2005, IEEE Photonics Technology Letters.

[7]  Joseph M. Lukens,et al.  A temporal cloak at telecommunication data rate , 2013, Nature.

[8]  José Azaña,et al.  On the generality of the Talbot condition for inducing self-imaging effects on periodic objects. , 2016, Optics letters.

[9]  M. V. Berry,et al.  Integer, fractional and fractal Talbot effects , 1996 .

[10]  A. Gaeta,et al.  Demonstration of temporal cloaking , 2011, Nature.

[11]  Tadasi Sueta,et al.  Optical pulse compression using high-frequency electrooptic phase modulation , 1988 .

[12]  J. Capmany,et al.  Return-to-Zero Pulse Generators Using Overdriven Amplitude Modulators at One Fourth of the Data Rate , 2007, IEEE Photonics Technology Letters.

[13]  J. Azaña,et al.  Noiseless intensity amplification of repetitive signals by coherent addition using the temporal Talbot effect , 2014, Nature Communications.

[14]  Shuqin Lou,et al.  Novel Temporal Zone Plate Designs With Improved Energy Efficiency and Noise Performance , 2014, Journal of Lightwave Technology.

[15]  B. Kolner Space-time duality and the theory of temporal imaging , 1994 .

[16]  Michal Lipson,et al.  Optical time lens based on four-wave mixing on a silicon chip. , 2008, Optics letters.

[17]  P. C. Chui,et al.  Comparison of state-of-art phase modulators and parametric mixers in time-lens applications under different repetition rates. , 2013, Applied optics.