Ulises Alcántara-Bautista

Mr. Ulises Alcántara-Bautista

orcid

Research Focus & Metrics

Academic Career Length

5Years (2022-Present)

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

Representative Publications

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2 September 2023 in Optics & Laser Technology
Verified
Journal Article
Closed access
UAUlises Alcántara-Bautista
Ulises Alcántara-Bautista
MDManuel Duran-Sanchez
Manuel Duran-Sanchez
EEEdwin Addiel Espinosa-De-La-Cruz
Edwin Addiel Espinosa-De-La-Cruz
IAIvan Armas-Rivera
Ivan Armas-Rivera
MBMiguel Bello-Jiménez
Miguel Bello-Jiménez
BIBaldemar Ibarra-Escamilla
Baldemar Ibarra-Escamilla

8 March 2023 in IEEE Photonics Technology Letters
Verified
Journal Article
Closed access
EEEdwin Espinosa
Edwin Espinosa
MDManuel Duran-Sanchez
Manuel Duran-Sanchez
OPOLIVIER JEAN MICHEL POTTIEZ
OLIVIER JEAN MICHEL POTTIEZ
UAUlises Alcántara-Bautista
Ulises Alcántara-Bautista
JAJared Alaniz-Baylón
Jared Alaniz-Baylón
BIBaldemar Ibarra-Escamilla
Baldemar Ibarra-Escamilla
A supercontinuum source based on a self-Q-switched Er/Yb-codoped fiber laser has been experimentally demonstrated. At different pump powers, starting at a moderate value of 1.1 W, self-Q-switched pulses with a broad flat spectrum of ~ 560 nm width spanning over the range ~1600 – 2160 nm at −5 dB level (considering the Raman peak) are obtained. Such wide spectrum can be achieved directly at the output of the fiber laser resonator, making the structure compact and robust. With a maximum pump power of 4.9 W, the repetition rate, average output power, peak power and pulse energy are approximately 14.7 kHz, 465 mW, 66 kW and $31~\mu \text{J}$ , respectively. This compact SC laser configuration has the merits of simple cavity design, low cost and good robustness, which provide a SC source that can be easily applied to numerous areas, such as spectroscopy, optical communications, metrology and biomedical applications.

12 November 2025 in Optical Fiber Technology
Verified
Journal Article
Open access
EEEdwin Espinosa
Edwin Espinosa
MDManuel Durán-Sánchez
Manuel Durán-Sánchez
UAUlises Alcántara-Bautista
Ulises Alcántara-Bautista
ARAlejandro Reyes-Mora
Alejandro Reyes-Mora
AIAdalid Ibarra
Adalid Ibarra
BIBaldemar Ibarra-Escamilla
Baldemar Ibarra-Escamilla

28 July 2025 in Journal of Optics
Verified
Journal Article
Closed access
EEEdwin Espinosa
Edwin Espinosa
MDManuel Duran-Sanchez
Manuel Duran-Sanchez
UAUlises Alcántara-Bautista
Ulises Alcántara-Bautista
ARAlejandro Reyes-Mora
Alejandro Reyes-Mora
AIAdalid Ibarra
Adalid Ibarra
BIBaldemar Ibarra-Escamilla
Baldemar Ibarra-Escamilla
The first demonstration of noise-like rectangular pulses (NLRPs) with a record pulse energy of 5.2 µJ and a peak power of 160 W at 1565 nm is presented. This is achieved through a linear-cavity fiber laser system with a power-symmetric nonlinear optical loop mirror as the mode locking element. Stable and highly energetic pulses are generated by extending the cavity length and carefully choosing the coupling ratio of the fiber loop mirror. The laser self-starts at a pump threshold of 1.12 W, and as the pump power increases to 10.5 W, the pulse duration extends from 2.2 to 32.2 ns, while the average output power increases from 0.14 to 2 W, yielding a high slope efficiency of 19.1%. Operating at a fundamental repetition rate of 392 kHz, this laser system delivers the highest reported pulse energy and peak power for NLRPs at a wavelength of 1565 nm in a linear cavity. Its cost-effectiveness, stability, and high performance make it a promising tool for applications such as LIDAR, supercontinuum generation, laser materials processing, and nonlinear spectroscopy.

21 June 2025 in Micromachines
Verified
Journal Article
Open access
PDF file
ARAlejandro Reyes-Mora
Alejandro Reyes-Mora
MDManuel Duran-Sanchez
Manuel Duran-Sanchez
EEEdwin Espinosa
Edwin Espinosa
UAUlises Alcántara-Bautista
Ulises Alcántara-Bautista
AIAdalid Ibarra
Adalid Ibarra
BIBaldemar Ibarra-Escamilla
Baldemar Ibarra-Escamilla
In this work, we report the formation of multiple mode-locking states in an Erbium/Ytterbium co-doped fiber laser, such as domain-wall (DW) dark pulses, high-order dark harmonic pulses, dissipative soliton resonance (DSR) pulses, and dual-wavelength h-shaped pulses. By increasing the pump power and adjusting the quarter-wave retarder (QWR) plates, we experimentally achieve 310th-order harmonic dark pulses. DSR pulses emerge at a pump power of 1.01 W and remain stable up to 9.07 W, reaching a maximum pulse width of 676 ns and a pulse energy of 1.608 µJ, while Dual-wavelength h-shaped pulses have a threshold of 1.42 W and maintain stability up to 9.07 W. Using a monochromator, we confirm that these h-shaped pulses result from the superposition of a soliton-like pulse and a DSR-like pulse, emitting at different wavelengths but locked in time. The fundamental repetition rate for dark pulsing, DSR, and h-shaped pulses is 321.34 kHz. This study provides new insights into complex pulse dynamics in fiber lasers and demonstrates the versatile emission regimes achievable through precise pump and polarization control.

8 May 2025 in Fibers
Verified
Journal Article
Open access
PDF file
EEEdwin Espinosa
Edwin Espinosa
MDManuel Duran-Sanchez
Manuel Duran-Sanchez
UAUlises Alcántara-Bautista
Ulises Alcántara-Bautista
ARAlejandro Reyes-Mora
Alejandro Reyes-Mora
AIAdalid Ibarra-Garrido
Adalid Ibarra-Garrido
BIBaldemar Ibarra-Escamilla
Baldemar Ibarra-Escamilla
A passively Q-switched Thulium-doped fiber laser based on glycerin as the saturable absorber is experimentally demonstrated for the first time. The saturable absorber consists of two FC/PC connectors aligned within a mechanical fiber-fiber coupler, with the intervening gap filled with glycerin. Such a saturable absorber is integrated into a compact ring cavity, enabling passive Q-switched laser operation. Starting at a minimum pump power of 1.7 W, Q-switched pulses with a central wavelength of 1946 nm are obtained. At the maximum pump power of 2.4 W, the laser generates pulses with a duration of approximately 2 µs, a repetition rate of 26.7 kHz, and a pulse energy of 1.08 µJ. To the best of our knowledge, this is the first demonstration of passively Q-switched laser operation utilizing a glycerin-based saturable absorber for generating pulsed emission at the 2-µm wavelength region. This breakthrough represents a significant advancement in fiber laser technology, introducing a novel and efficient approach to pulse generation.