Arturo Alberto Castillo-Guzmán

Dr. Arturo Alberto Castillo-Guzmán

Physical-Mathematical Sciences Research Center (CICFIM), Nuevo Leon Autonomus University (UANL), 64455 San Nicolás de los Garza, Mexico
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Research Focus & Metrics

Academic Career Length

21Years (2006-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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25 January 2010 in Optics Letters
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Journal Article
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JAJ. E. Antonio-Lopez
J. E. Antonio-Lopez
Arturo Alberto Castillo-GuzmánArturo Alberto Castillo-Guzmán
Arturo Alberto Castillo-Guzmán
DMDaniel May-Arrioja
Daniel May-Arrioja
RSR. Selvas-Aguilar
R. Selvas-Aguilar
PLP. LiKamWa
P. LiKamWa
We report on a wavelength-tunable filter based on multimode interference (MMI) effects. A typical MMI filter consists of a multimode fiber (MMF) spliced between two single-mode fibers (SMF). The peak wavelength response of the filter exhibits a linear dependence when the length of the MMF is modified. Therefore a capillary tube filled with refractive-index-matching liquid is used to effectively increase the length of the MMF, and thus wavelength tuning is achieved. Using this filter a ring-based tunable erbium-doped fiber laser is demonstrated with a tunability of 30 nm, covering the full C-band.

4 January 2010 in Optics Express
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Journal Article
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Arturo Alberto Castillo-GuzmánArturo Alberto Castillo-Guzmán
Arturo Alberto Castillo-Guzmán
JAJ. E. Antonio-Lopez
J. E. Antonio-Lopez
RSR. Selvas-Aguilar
R. Selvas-Aguilar
DMD. A. May-Arrioja
D. A. May-Arrioja
JAJulian Moises EstudIllo Ayala
Julian Moises EstudIllo Ayala
PLP. LiKamWa
P. LiKamWa
A widely tunable erbium-doped all-fiber laser has been demonstrated. The tunable mechanism is based on a novel tunable filter using multimode interference effects (MMI). The tunable MMI filter was applied to fabricate a tunable erbium-doped fiber laser via a standard ring cavity. A tuning range of 60 nm was obtained, ranging from 1549 nm to 1609 nm, with a signal to noise ratio of 40 dB. The tunable MMI filter mechanism is very simple and inexpensive, but also quite efficient as a wavelength tunable filter.

7 March 2021 in Sensors
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Jose R. Guzman-SepulvedaJose R. Guzman-Sepulveda
Jose R. Guzman-Sepulveda
RGRafael Guzman-Cabrera
Rafael Guzman-Cabrera
Arturo Alberto Castillo-GuzmánArturo Alberto Castillo-Guzmán
Arturo Alberto Castillo-Guzmán
We review fiber-based multimode interference (MMI) devices with a particular focus on optical fiber-based sensing applications. The present review complements a recently published, extensive review where the sensing of conventional physical variables such as refractive index, temperature, displacement, and strain was covered. This review focuses on MMI fiber sensors for nonconventional physical variables, including mechanical, electromagnetic, chemical, and optical, covering around fifteen years of work in the field. Finally, by the end of this paper, we also review some new trends of MMI-based schemes based on polymer fibers, for wavelength-locking applications, for retrieving the thermo-optic coefficient of liquid samples, and for measuring the dynamics of complex fluids.

10 June 2016 in Sensors
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Journal Article
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EMEduardo Huerta Mascotte
Eduardo Huerta Mascotte
JSJuan Sierra
Juan Sierra
Ruth Ivonne Mata-ChavezRuth Ivonne Mata-Chavez
Ruth Ivonne Mata-Chavez
DJD. Jauregui-Vazquez
D. Jauregui-Vazquez
Arturo Alberto Castillo-GuzmánArturo Alberto Castillo-Guzmán
Arturo Alberto Castillo-Guzmán
RRRoberto Rojas-Laguna
Roberto Rojas-Laguna
In this paper, an all-fiber Mach-Zehnder interferometer (MZI) based on a non-zero dispersion-shifted fiber (NZ-DSF) is presented. The MZI was implemented by core-offset fusion splicing one section of a NZ-DSF fiber between two pieces of single mode fibers (SMFs). Here, the NZ-DSF core and cladding were used as the arms of the MZI, while the core-offset sections acted as optical fiber couplers. Thus, a MZI interference spectrum with a fringe contrast (FC) of about 20 dB was observed. Moreover, its response spectrum was experimentally characterized to the torsion parameter and a sensitivity of 0.070 nm/° was achieved. Finally, these MZIs can be implemented in a compact size and low cost.

1 November 2013 in Optics Communications
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Journal Article
Closed access
DJD. Jauregui-Vazquez
D. Jauregui-Vazquez
JAJulian Moises EstudIllo Ayala
Julian Moises EstudIllo Ayala
Arturo Alberto Castillo-GuzmánArturo Alberto Castillo-Guzmán
Arturo Alberto Castillo-Guzmán
RRR. Rojas-Laguna
R. Rojas-Laguna
RSR. Selvas-Aguilar
R. Selvas-Aguilar
AFA. Flores-Balderas
A. Flores-Balderas

2 June 2017 in Sensors
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Journal Article
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GSGuillermo Salceda-Delgado
Guillermo Salceda-Delgado
AMAlejandro Martinez-Rios
Alejandro Martinez-Rios
RSRomeo Selvas-Aguilar
Romeo Selvas-Aguilar
RTRicardo Ivan Alvarez Tamayo
Ricardo Ivan Alvarez Tamayo
Arturo Alberto Castillo-GuzmánArturo Alberto Castillo-Guzmán
Arturo Alberto Castillo-Guzmán
LEL. F. Enriquez-Gomez
L. F. Enriquez-Gomez
A compact, highly sensitive optical fiber displacement and curvature radius sensor is presented. The device consists of an adiabatic bi-conical fused fiber taper spliced to a single-mode fiber (SMF) segment with a flat face end. The bi-conical taper structure acts as a modal coupling device between core and cladding modes for the SMF segment. When the bi-conical taper is bent by an axial displacement, the symmetrical bi-conical shape of the tapered structure is stressed, causing a change in the refractive index profile which becomes asymmetric. As a result, the taper adiabaticity is lost, and interference between modes appears. As the bending increases, a small change in the fringe visibility and a wavelength shift on the periodical reflection spectrum of the in-fiber interferometer is produced. The displacement sensitivity and the spectral periodicity of the device can be adjusted by the proper selection of the SMF length. Sensitivities from around 1.93 to 3.4 nm/mm were obtained for SMF length between 7.5 and 12.5 cm. Both sensor interrogations, wavelength shift and visibility contrast, can be used to measure displacement and curvature radius magnitudes.