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Low-energy single-optical-cycle soliton self-compression in air-silica nanowires

[+] Author Affiliations
Amine Ben Salem, Rim Cherif, Mourad Zghal

University of Carthage, Engineering School of Communication of Tunis (Sup’Com), Cirta’Com Laboratory, Ghazala Technopark, 2083, Ariana, Tunisia

J. Nanophoton. 5(1), 059506 (November 16, 2011). doi:10.1117/1.3662888
History: Received September 16, 2011; Revised October 29, 2011; Accepted October 31, 2011; Published November 16, 2011; Online November 16, 2011
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We investigated and optimized the process of soliton self-compression in few millimeters-long air-silica nanowires. A 100 fs prechirped input pulse was compressed to a 1.4 fs pulse by pumping at very low energy of 2.5 nJ an air-silica nanowire. More than one octave spanning coherent broadband supercontinuum extending from 260 to 1800 nm was generated.

Figures in this Article

Air-silica nanowires with core diameters smaller than the wavelength have attracted considerable interest due to their unique dispersion profiles and nonlinear properties for wide range of applications.12 These nanowires are not only suitable for nanophotonic devices but also enable soliton self-compression (SSC), dispersion compensation, and broadband supercontinuum (SC) generation.34 Much effort has been dedicated in generating pulses in the few-optical-cycle regime which has permitted important achievements in diverse fields such as the study of ultrafast dynamics in matter, high-order harmonic generation, extreme nonlinear optics, and attosecond physics.56 An impressive approach toward the monocycle regime dating back to the 1980s has been used to generate compressed pulses relying on the concept of SSC.7 The introduction of highly nonlinear photonic nanowires with anomalous group velocity dispersion at visible and near-infrared wavelengths has enormously contributed in the study of SSC techniques and the generation of few to single-optical cycles. The results approaching the single-cycle regime have been reported by Foster et al. using tapered air-silica nanowires.8 They experimentally demonstrated the SSC of 70 to 6.8 fs compressed pulse by injecting light into a 2-mm long 980 nm core diameter air-silica nanowire.

In this paper, we demonstrate the generation of a compressed pulse as short as 1.4 fs (ca. 0.52 single-optical-cycle) in a 1.15-mm long 800 nm core-diameter air-silica nanowire acting as a dispersion compensating fiber. Therefore, to the best of our knowledge, this is the shortest pulse and the highest compression ratio ever achieved and reported in air-silica nanowires at a low energy level. First, a full modal analysis of the optical properties of air-silica nanowires including chromatic dispersion, effective mode area, and nonlinear coefficient is presented. Investigation of the evanescent field has been conducted and the cut-off condition of single mode operation in air-silica nanowires is evaluated. Secondly, the optimization of the SSC, by pumping at very low pulse energy of 2.5 nJ, a 100 fs prechirped input pulse in the 800 nm air-silica nanowire is achieved. Moreover, more than one octave spanning coherent SC is generated extending from 260 to 1800 nm.

The optical properties of the air-silica nanowires are calculated using the glass-rod-in-air model.9 With this model, we analyze the confinement of the fundamental mode, the evolution of the dispersion as a function of the wavelength, the effective area, and the nonlinear coefficient. A full vectorial finite element method with dense meshes made up of 104 to 105 is developed to calculate the propagation constant β of the fundamental mode HE11. By expanding the mode-propagation constant β in a Taylor series at a central frequency ω0, the chromatic dispersion can be determined through the group velocity dispersion (GVD) parameter β2 as a function of the wavelength.10 We calculate the chromatic dispersion as a function of the wavelength for different core diameter air-silica nanowires ranging from 400 to 900 nm, as seen in Fig. 1. Good agreement is found with chromatic dispersions calculated in Refs. 4 and 8.

Graphic Jump LocationF1 :

Calculated chromatic dispersion of air-silica nanowires with core diameters ranging from 400 to 900 nm.

By reducing the nanowire's core diameter, the region of the anomalous GVD exhibited between two zero dispersion wavelengths can be shifted toward the blue wavelength region. This property is a result from the dominance of the waveguide dispersion over the material dispersion (bulk silica) for air-silica nanowires. With the appropriate choice of the core size, the overall GVD can be highly engineered and the second zero dispersion wavelength can be positioned near the pump wavelength to yield anomalous, normal, or zero GVD. We notice that the largest region of the anomalous GVD centered around a pump wavelength of λp = 800 nm and accompanied with low third-order dispersion (β3) is found for the 800 nm core-diameter air-silica nanowire (β2 = −9.12×10−2 ps2 m−1 and β3 = −5.28×10−6 ps3 m−1). This property is primordial to achieve efficient SSC which results from the interplay between the dispersion and the self-phase modulation effects. This fact is due to exotic dispersion profiles and high nonlinearities provided by air-silica nanowires. Thus, the 800 nm core-diameter air-silica nanowire is selected to optimize the SSC at λp = 800 nm.

By calculating the longitudinal component of the Poynting vector Sz for the sub-wavelength nanowire structures, a significant fraction of the power is found to reside in the evanescent field. This evanescent field interacts directly with the cladding (air)-glass interfaces. The calculation of the Poynting vector shows that when the optical wavelength λ is larger than the nanowire's core diameter d, the evanescent field starts to dominate and its fractional power increases. Although the modeling has been conducted for a fixed λ and varying d, one could assume that the behavior of the evanescent field and its fractional power remain the same as long as the ratio d/λ does not change. This is justified by the small changes Δn/n ≈ 0.02 of the refractive index of silica glass in a large wavelength range between 400 and 1800 nm. To obtain straightforward information about the power distribution in the radial direction, we evaluate the fractional power ηEF outside the core which is given in Ref. 9.

Figure 2 shows the fraction of power of the fundamental mode propagating outside the core as a function of the normalized diameter d/λ. We notice that by increasing d/λ, the evanescent field decreases until reaching a value of 9% for a ratio d/λ = 1 and almost 1% for a ratio of d/λ = 2. Therefore, with a careful design of air-silica nanowire with a core diameter d < 0.25λ, more than 98% of the light can propagate outside the core. The evanescent field surrounding the nanowire and the strong radial confinement of the light make air-silica nanowires well-suited for an efficient and controlled interaction of guided light with matter and perfect devices for sensing applications.11 Like conventional optical fibers, air-silica nanowires experience single-mode (HE11) guiding for V < 2.405.9 The dashed line in Fig. 2 indicates the cut-off condition for single mode operation. We clearly see that only the fundamental mode propagates when d < 0.71λ (i.e., V < 2.405). At this cut-off condition, the fractional power inside the core is equal to 80% of the total propagating light. For instance, at λp = 800 nm, the critical core diameter for single mode operation is dSM = 568 nm. Since the air-silica nanowire exhibits a significant fraction of the power propagating outside the core, an accurate estimation of the nonlinear coefficient γ is needed.12 Figure 2 depicts the effective mode area Aeff = 2πn2/(λpγ) and γ calculated at λp = 800 nm for air-silica nanowires with core diameters ranging from 200 to 1000 nm. It illustrates that the mode confinement determined by the effective mode area becomes stronger when reducing the core diameter of the air-silica nanowire. This behavior evolves linearly and reaches a minimum effective mode area (maximum nonlinear coefficient) value for a core diameter of about 550 nm. A high nonlinear coefficient of 507 W−1 km−1 is calculated for the 800 nm air-silica nanowire by using n2 = 2.6×10−20 m2 W−1.10

Graphic Jump LocationF2 :

(a) Fractional power ηEF outside the core as a function of the normalized diameter d/λ. (b) Effective mode area (Aeff) and nonlinear coefficient (γ) of air-silica nanowires for different core diameters at λp = 800 nm.

The investigation of the nonlinear propagation is based on the resolution of the generalized nonlinear Schrödinger equation (GNLSE) which takes into account the contribution of linear and nonlinear effects and describes the temporal and the longitudinal dependence of the pulse envelope A(z,t).10 The resolution of the GNLSE is performed using the symmetrized split step Fourier method.13 We set the loss coefficient to 1 dBm−1 (Ref. 4) and used an accurate model including the full dispersion profile. We consider the propagation of an N’th order soliton having the envelope field expression

A(0,t)=P0sech(t/T0)exp(iC·t2/2T02)
, where P0 is the peak power and T0 is the input soliton duration defined as TFWHM /1.763. TFWHM is the input pulse full width at half maximum (FWHM) duration. C is the chirp parameter controlling the initial chirp.10

Our numerical study shows that input pulses with durations shorter than 100 fs with few nanojoule energy requires an optimal nanowire length considerably shorter than 1 mm, which immediately poses a practical problem since it is difficult to obtain such short fiber lengths. However, enlarging the initial pulse duration at the same low input energy allows the increase of the nanowire length so that 100 fs input pulse is found to overcome this difficulty. Air-silica nanowires’ lengths on the order of 1 mm are then required, which can be easily fabricated as demonstrated in Ref. 8. Thus, in our calculations, the input pulse duration is taken as TFWHM = 100 fs.

In order to characterize the efficiency of the SSC, three parameters are introduced and denoted: 1. zopt is the optimal length at which a maximum compressed pulse can be extracted with highest output preserved soliton pulse shape. 2. Fc = TFWHM/Tcomp is the compression factor defined as the ratio of the FWHM pulse durations at the input (TFWHM) and the output of the nanowire (Tcomp). 3. Qc = Pcomp/(P0Fc) is the quality factor defined as the ratio of the peak power (Pcomp) of the compressed pulse with the input peak power P0 and Fc. We start our analysis with the optimization of laser-pulse parameters (i.e., pulse duration, pulse shape, and chirp) on SSC and the spectral properties of the generated SC. We first examine the effect of the chirp on the compression factor. To this end, we simulate an initial nonchirped hyperbolic-secant pulse and vary the input pulse energy. A maximum compressed pulse with duration of 1.53 fs in a 1.15 mm nanowire length is found with an input energy of 2.5 nJ. Then, we vary the input chirp C and we analyze the nonlinear evolution aiming to extract the optimal chirp value giving the maximum compressed pulse.

Figure 3 shows the effect of the variation of the chirp on the duration of the final compressed pulse Tcomp. We find that positive chirp degrades the temporal compression while negative chirp enhances the SSC. The optimal chirp value of C = −0.2 is found to maximize the temporal compression. In conclusion, we find that a very low input energy of 2.5 nJ prechirped input hyperbolic-secant pulse at a pump wavelength of 800 nm gives an optimum temporal compressed pulse. Figure 3 shows the result of the optimization of the temporal evolution of the chirped hyperbolic-secant pulse with C = −0.2 as a function of the propagation distance. We extract a maximum compressed pulse as short as 1.4 fs generated after 1.15-mm long 800 nm core-diameter air-silica nanowire corresponding to the excitation of an input soliton order N = 19.8. This interaction corresponds to a very high compression factor Fc = 71.43 and a quality factor Qc = 0.13. We notice that by overpassing the optimal propagation distance (zopt = 1.15 mm), the temporal pulse profile presents a remarkable increasing multipeak and broadened structure due to soliton fission induced by Raman scattering and high-order dispersions. The main aim of the analysis presented in this section is to understand the spatiotemporal dynamics behind the supercontinuum SSC to few-cycle durations.

Graphic Jump LocationF3 :

(a) Effect of the initial chirp on the compression efficiency. (b) Temporal evolution of 100 fs prechirped input as a function of the propagation distance at λp = 800 nm.

Figure 4 shows the spectral evolution of 100 fs input pulse with 2.5 nJ input energy in the 800 nm core-diameter air-silica nanowire as a function of the propagation distance until the optimal SSC is achieved. The analysis of the coherence properties of the generated SC with adding one photon per mode noise with a random phase14 shows from an ensemble average of 60 independent simulations that the generated SC is perfectly coherent over the entire generated bandwidth [see Fig. 4]. The corresponding spectrogram representations are shown at each of the propagation distances in Fig. 4. Broadband SC from ultraviolet to mid-infrared regions extending from 260 to 1800 nm is generated.

Graphic Jump LocationF4 :

(a) Spectral evolution of 100 fs input pulse with 2.5 nJ input as a function of the propagation distance z. (b) Degree of coherence of the generated SC. (c) Spectrogram representation of the pulse at each propagation distance.

These features reflect the growth of the symmetrical broadening when the propagation distance increases to 1 mm. This confirms that the effect of self-phase modulation is the predominant effect given such broadening. However, an asymmetric spectral profile starts to appear toward infrared wavelengths and is observed at the optimal length. This is justified by the fact that the compressed pulse undergoes soliton fission caused by the Raman effect but with very low intensity [as seen in Fig. 3] so that Raman solitons are generated and the SC is redshifted. Although very small pulse fluctuations and peaks appear around the highest peak of the compressed pulse, the extraction of the optimal compressed pulse is still valid since a large intensity gap is depicted between the highest and smallest peaks. Comparable broadband compressible SC was theoretically generated in the 800 nm nanowire by Foster et al. ,8 but in a very short nanowire length of 650 μm which can be considered as a practical problem to obtain such a short fiber length. Thus, the idea of enlarging the initial pulse to 100 fs is proposed with an implemented prechirping technique and generating efficient compressible SC to a single-cycle pulse is achieved.

Soliton self-compression has been investigated in an 800 nm air-silica nanowire. A 1.4 fs compressed pulse starting from 100 fs is obtained at a very low input pulse energy of 2.5 nJ in only a 1.15-mm long nanowire. Thus, a very high compression factor of 71.43 is achieved. The generation of more than one octave spanning coherent SC from UV to near-IR is shown. Air-silica nanowires are found to be very promising for designing white light coherent sources and suitable waveguides for dispersion compensation and high SSC which opens new horizon toward extreme nonlinear optics and attosecond physics.

We acknowledge partial support of “Institut Télécom” through the “Futur et Ruptures” PhD thesis of A. Ben Salem. We thank John Dudley from Institut Femto-ST, University of Franche-Comté, Besançon, France for collaboration and useful scientific discussions.

Tong  L. M., , Gattass  R. R., , Ashcom  J. B., , He  S. L., , Lou  J. Y., , Shen  M. Y., , Maxwell  I., , and Mazur  E., “ Subwavelength-diameter silica wires for low-loss optical wave guiding. ,” Nature. 426, , 816–819  ((2003)).
Foster  M., , Turner  C., , Lipson  M., , and Gaeta  A. L., “ Nonlinear optics in photonic nanowires. ,” Opt. Express. 16, , 1300–1320  ((2008)).
Gattass  R. R., , Svacha  G. T., , Tong  L. M., , and Mazur  E., “ Supercontinuum generation in submicrometer diameter silica fibers. ,” Opt. Express. 14, , 9408–9414  ((2006)).
Leon-Saval  S. G., , Birks  T. A., , Wadsworth  W. J., , Russell  P. S. J., , and Mason  M. W., “ Supercontinuum generation in submicron fibre waveguides. ,” Opt. Express. 12, , 2864–2869  ((2004)).
Brabec  T., and Krausz  F., “ Intense few-cycle laser fields: Frontiers of nonlinear optics. ,” Rev. Mod. Phys.. 72, , 545–591  ((2000)).
Kartner  F. X., Ed.,  Few-Cycle Laser Pulse Generation and Its Applications. ,  Springer Verlag ,  Berlin, Germany  ((2004)).
Mollenauer  L. F., , Stolen  R. H., , Gordon  J. P., , and Tomlinson  W. J., “ Extreme picosecond pulse narrowing by means of soliton effect in single-mode optical fibers. ,” Opt. Lett.. 8, , 289–291  ((1983)).
Foster  M., , Gaeta  A. L., , Caoand  Q., , and Trebino  R., “ Soliton-effect compression of supercontinuum to few-cycle durations in photonic nanowires. ,” Opt. Express. 13, , 6848–6855  ((2005)).
Tong  L., , Lou  J., , and Mazur  E., “ Single-mode guiding properties of subwavelength-diameter silica and silicon wire waveguides. ,” Opt. Express. 12, , 1025–1035  ((2004)).
Agrawal  G. P.,  Nonlinear Fiber Optics. , 4th Ed.,  Academic, Elsevier ,  San Diego, USA  ((2006)).
Brambilla  G., “ Optical fibre nanotaper sensors. ,” Opt. Fiber Tech.. 16, , 331–342  ((2010)).
Foster  M. A., , Moll  K. D., , and Gaeta  A. L., “ Optimal waveguide dimensions for nonlinear interactions. ,” Opt. Express. 12, , 2880–2887  ((2004)).
Cherif  R., , Zghal  M., , Tartara  L., , Degiorgio  V., “ Single-sided supercontinuum generation in a photonic crystal fiber by selective excitation of the third-order mode. ,” Proc. SPIE. 6990, , 69900O  ((2008)).
Dudley  J. M., and Coen  S., “ Coherence properties of supercontinuum spectra generated in photonic crystal fiber and tapered optical fiber. ,” Opt. Lett.. 27, , 1180–1182  ((2002)).
© 2011 Society of Photo-Optical Instrumentation Engineers (SPIE)

Citation

Amine Ben Salem ; Rim Cherif and Mourad Zghal
"Low-energy single-optical-cycle soliton self-compression in air-silica nanowires", J. Nanophoton. 5(1), 059506 (November 16, 2011). ; http://dx.doi.org/10.1117/1.3662888


Figures

Graphic Jump LocationF1 :

Calculated chromatic dispersion of air-silica nanowires with core diameters ranging from 400 to 900 nm.

Graphic Jump LocationF2 :

(a) Fractional power ηEF outside the core as a function of the normalized diameter d/λ. (b) Effective mode area (Aeff) and nonlinear coefficient (γ) of air-silica nanowires for different core diameters at λp = 800 nm.

Graphic Jump LocationF3 :

(a) Effect of the initial chirp on the compression efficiency. (b) Temporal evolution of 100 fs prechirped input as a function of the propagation distance at λp = 800 nm.

Graphic Jump LocationF4 :

(a) Spectral evolution of 100 fs input pulse with 2.5 nJ input as a function of the propagation distance z. (b) Degree of coherence of the generated SC. (c) Spectrogram representation of the pulse at each propagation distance.

Tables

References

Tong  L. M., , Gattass  R. R., , Ashcom  J. B., , He  S. L., , Lou  J. Y., , Shen  M. Y., , Maxwell  I., , and Mazur  E., “ Subwavelength-diameter silica wires for low-loss optical wave guiding. ,” Nature. 426, , 816–819  ((2003)).
Foster  M., , Turner  C., , Lipson  M., , and Gaeta  A. L., “ Nonlinear optics in photonic nanowires. ,” Opt. Express. 16, , 1300–1320  ((2008)).
Gattass  R. R., , Svacha  G. T., , Tong  L. M., , and Mazur  E., “ Supercontinuum generation in submicrometer diameter silica fibers. ,” Opt. Express. 14, , 9408–9414  ((2006)).
Leon-Saval  S. G., , Birks  T. A., , Wadsworth  W. J., , Russell  P. S. J., , and Mason  M. W., “ Supercontinuum generation in submicron fibre waveguides. ,” Opt. Express. 12, , 2864–2869  ((2004)).
Brabec  T., and Krausz  F., “ Intense few-cycle laser fields: Frontiers of nonlinear optics. ,” Rev. Mod. Phys.. 72, , 545–591  ((2000)).
Kartner  F. X., Ed.,  Few-Cycle Laser Pulse Generation and Its Applications. ,  Springer Verlag ,  Berlin, Germany  ((2004)).
Mollenauer  L. F., , Stolen  R. H., , Gordon  J. P., , and Tomlinson  W. J., “ Extreme picosecond pulse narrowing by means of soliton effect in single-mode optical fibers. ,” Opt. Lett.. 8, , 289–291  ((1983)).
Foster  M., , Gaeta  A. L., , Caoand  Q., , and Trebino  R., “ Soliton-effect compression of supercontinuum to few-cycle durations in photonic nanowires. ,” Opt. Express. 13, , 6848–6855  ((2005)).
Tong  L., , Lou  J., , and Mazur  E., “ Single-mode guiding properties of subwavelength-diameter silica and silicon wire waveguides. ,” Opt. Express. 12, , 1025–1035  ((2004)).
Agrawal  G. P.,  Nonlinear Fiber Optics. , 4th Ed.,  Academic, Elsevier ,  San Diego, USA  ((2006)).
Brambilla  G., “ Optical fibre nanotaper sensors. ,” Opt. Fiber Tech.. 16, , 331–342  ((2010)).
Foster  M. A., , Moll  K. D., , and Gaeta  A. L., “ Optimal waveguide dimensions for nonlinear interactions. ,” Opt. Express. 12, , 2880–2887  ((2004)).
Cherif  R., , Zghal  M., , Tartara  L., , Degiorgio  V., “ Single-sided supercontinuum generation in a photonic crystal fiber by selective excitation of the third-order mode. ,” Proc. SPIE. 6990, , 69900O  ((2008)).
Dudley  J. M., and Coen  S., “ Coherence properties of supercontinuum spectra generated in photonic crystal fiber and tapered optical fiber. ,” Opt. Lett.. 27, , 1180–1182  ((2002)).

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