Highlights


Accurate determination of Poisson’s ratio in optical fibers using
Forward Stimulated Brillouin Scattering (FSBS)


FSBS enables a high accuracy measurement of Poisson’s ratio (ν) of optical fibers and its temperature dependence (Opt. Express 30, 442295, 2022). Our approach is based on an all-optical pump and probe technique used for the excitation and characterization of both, radial and torsional-radial acoustic resonances of optical fibers (Opt. Lett. 45, 5331-5334, 2020). Following this approach, the determination of Poisson’s ratio does not require the measurement of any physical length, but only frequency measurements. The dependence of fiber Poisson’s ratio with temperature is also determined experimentally.
*Our article in Optics Express has been highlighted as an Editor's Pick.*

Record accuracy measurement of phase and group refractive indices of optical fibers


Weak fiber Bragg gratings enable high accuracy measurement of the absolute modal refraction index of the fundamental mode in single-mode fibers. We also demonstrate a new method to measure the group index, and report on the thermo-optic and the strain-optic coefficients as a function of the wavelength (Appl. Opt. 60, 2824-2832, 2021. Several standard optical fibers were characterized: Corning SMF28 telecom fiber, Fibercore HB1250 polarization maintaining fiber and Fibecore M5 erbium doped fiber. *Aplied Optics' Editors have chosen this paper to be highlighted as an Editor's Pick.*


Novel concept for in-fiber biosensors: Bio-Bragg Gratings


We present the design, fabrication, and proof of concept of a novel biosensor based on a bio-Bragg-grating (BBG) that is imprinted on the surface of a microfiber. Our approach combines the ability to pattern a periodic network of bioreceptors on the surface of a microfiber, with the sensing capacity of microfibers due to its enhanced evanescent optical field. The bioreceptors (BSA, in our case) are placed in a periodic fashion onto the fiber surface by microcontact printing. The interaction between the fundamental optical mode of the microfiber and this incipient BBG leads to a weak reflection peak in the optical response of the device.


The biosensing transduction principle relies on the fact that, if the specific target (IgGs in this case) is present in the external medium, it will bind to the bioreceptors that conform the BBG, increasing its reflectivity. As a result, it will be possible to quantify the concentration of specific IgGs by measuring such reflectivity. Tunability of the BBG response, wavelength multiplexation, and minimized non-specific binding signal contributions are demonstrated.


This work has been published in Biosensors and Bioelectronics (Biosensors & Bioelectronics, Vol. 176, art. 112916, (2021)), and was registered as a national patent (ES2749689 / G01N21/17).

Broadband tuning of polarization modulation (PMI) in photonic crystal fibers (PCF)


Wideband tuning of strong bands generated through polarization modulation instability (PMI) in photonic crystal fibers (PCF) is achieved via thermal tuning of fiber’s chromatic dispersion and birefringence, using PCFs infiltrated with ethanol and pumped at 1064 nm (Optics Letters 45, 4891-4894, 2020). In a previous article, we demonstrated tunable PMI in all-normal dispersion (AND-i) photonic crystal fibers, in which scalar four wave mixing (FWM) was forbidden (IEEE Photonics Journal 11, art. 7104108, 2019).

Direct measurement of the ratio between chromatic dispersion and the nonlinear coefficient


The fundamentals of our measuring method is based on a conservation law of the nonlinear Schrödinger equation, so it is not limited to specific ranges of chromatic dispersion and nonlinear coefficient values, in contrast to previous approaches. Measuring the increments of intensity autocorrelation at zero time delay (which provides -Δρloss), and the square of the rms spectral width (Δμ2) at different powers, for a given fiber length, one obtains directly the ratio between chromatic dispersion and the nonlinear coefficient (β2/γ). (Optics Letters 45, 4432-4435, 2020) *Optics Letters' Editors have chosen this paper to be highlighted as an Editor's Pick.*

Measurement of the strain-optic coefficients of PMMA from 800 to 2000 nm


PMMA Pockels' coefficients exhibit negligible dispersion and anisotropy in the wavelength range [800, 2000] nm:

p11 = 0.298 ± 0.010        p12 = 0.294 ± 0.010

The strain-optic coefficients were measured using a technique based on the excitation of azimuthal whispering gallery modes resonances in thin PMMA cylinders (OSA Continuum 3, 441-446, 2020). The technique was previously demonstrated using silica fibers (Optics Letters 41, 2934-2937, 2016).

Polarization modulation instability (PMI) in all-normal dispersion (ANDi) photonic crystal fibers (PCF)


PMI enables a controlled generation of new frequencies in ANDi fibers, in which scalar four wave mixing (FWM) is forbidden. Several ANDi - PCF were designed and fabricated at the LFO facilities. A detailed experimental and theoretical characterization of PMI in these ANDi - PCF was carried out (IEEE Photonics Journal 11, art. 7104108, 2019). This work is part of a project focused on the development of new tunable light sources based on FWM in nonlinear PCF with special dispersion properties.

20 W Yb fiber laser: random noise pulsed regime


We show that the laser output obeys the photon statistics inherent to narrowband amplified spontaneous emission and that the noise pulsing is properly addressed in terms of probability density and autocorrelation functions. Our novel approach reveals, in particular, that the regime’s coherence time dramatically shortens, from few ns to tens ps, with increasing laser power (Scientific Reports 9, art. 13073, 2019)

Special Fiber Gratings


Recent advances in fiber grating fabrication: (Left) Single-mode Bragg gratings in tapered few-mode and multimode fibers (Optics Letters 44, 4024-4027, 2019), and (Right) long period gratings with subnanometric linewidths (Optics Letters 42, 1265-1268, 2017). These fabrication improvements have pushed forward some applications in photonic fractional signal processing (Progress in Optics 63, 93-178, 2018).