Yakup Midilli
Research Subjects
Yakup Midilli has a total of 27 co-authors. Here are the top co-authors by number of shared publications:
- Ali Karatutlu
Engineering Fundamental Sciences, Sivas University of Science and Technology, Sivas 58000, Turkey
5 shared publications - Bülend Ortaç
National Nanotechnology Research Center (UNAM) and the Institute of Materials Science Nanotechnology, Bilkent University, Ankara, Trkiye
5 shared publications Bülend Ortaç
3 shared publicationsEkin Teslime Balk
UNAM-National Nanotechnology Research Center and Institute of Material Science and Nanotechnology, Bilkent University, 06800 Ankara, Turkey
2 shared publications- Elif Yapar Yildirim
UNAM-National Nanotechnology Research Center and Institute of Material Science and Nanotechnology, Bilkent University, 06800 Ankara, Turkey
2 shared publications A. Aytaç Seymen
1 shared publication
Latest Publications
- 23 September 2024
- Published by Optica Publishing Group in Applied Optics
- Vol. 63 (28) , 7402-7409
Estimation of ground-based atmospheric turbulence strength (C n2) by neural network architecture
Estimating the atmospheric turbulence strength (C n 2) becomes significant in the research field of electromagnetic radiation transmission through the atmosphere, particularly optical waves. As turbulence strength increases, the quality and strength of these optical waves may decrease and cause much trouble as they pass through the atmosphere. Throughout the years, C n 2 has been formulated by different research groups for various geographical locations and seasons using macro-meteorological variables empirically and theoretically. However, since these models are based on the data collected from numerous places and conditions, such as deserts or coastal areas, they do not provide accurate C n 2 predictions for our experimental site, as demonstrated for three well-known models in the paper. In this study, a novel, to our knowledge, artificial neural network (ANN) model named as quadratic Fourier neural network (QFNN) is trained to estimate C n 2 from experimentally measured ground-based atmospheric turbulence strength and macro-meteorological variables during the winter season in a rural area. The trained model gives reliable estimations, achieving a value of R2=0.92 for experimental C n 2 values.
- 23 September 2024
- Published by Optica Publishing Group in Applied Optics
- Vol. 63 (28) , 7402-7409
Estimation of ground-based atmospheric turbulence strength (C n2) by neural network architecture
Estimating the atmospheric turbulence strength (C n 2) becomes significant in the research field of electromagnetic radiation transmission through the atmosphere, particularly optical waves. As turbulence strength increases, the quality and strength of these optical waves may decrease and cause much trouble as they pass through the atmosphere. Throughout the years, C n 2 has been formulated by different research groups for various geographical locations and seasons using macro-meteorological variables empirically and theoretically. However, since these models are based on the data collected from numerous places and conditions, such as deserts or coastal areas, they do not provide accurate C n 2 predictions for our experimental site, as demonstrated for three well-known models in the paper. In this study, a novel, to our knowledge, artificial neural network (ANN) model named as quadratic Fourier neural network (QFNN) is trained to estimate C n 2 from experimentally measured ground-based atmospheric turbulence strength and macro-meteorological variables during the winter season in a rural area. The trained model gives reliable estimations, achieving a value of R2=0.92 for experimental C n 2 values.
- 14 August 2022
- Published by Springer Nature in Applied Physics B
- Vol. 128 (9) , 1-10
Effects of gamma radiation on Yb-doped Al–P–silicate optical fibers
- 14 August 2022
- Published by Springer Nature in Applied Physics B
- Vol. 128 (9) , 1-10
Effects of gamma radiation on Yb-doped Al–P–silicate optical fibers
- 7 July 2020
- Published by American Chemical Society (ACS) in ACS Applied Polymer Materials
- Vol. 2 (9) , 3840-3849
Cucurbit[7]uril-Capped Hybrid Conjugated Oligomer-Gold Nanoparticles for Combined Photodynamic-Photothermal Therapy and Cellular Imaging
- 7 July 2020
- Published by American Chemical Society (ACS) in ACS Applied Polymer Materials
- Vol. 2 (9) , 3840-3849
Cucurbit[7]uril-Capped Hybrid Conjugated Oligomer-Gold Nanoparticles for Combined Photodynamic-Photothermal Therapy and Cellular Imaging
- 29 January 2020
- Published by Institute of Electrical and Electronics Engineers (IEEE) in Journal of Lightwave Technology
- Vol. 38 (7) , 1915-1920
Demonstration of an All-Fiber Ultra-Low Numerical Aperture Ytterbium-Doped Large Mode Area Fiber in a Master Oscillator Power Amplifier Configuration Above 1 kW Power Level
We demonstrate an all-fiber ultra-low numerical aperture high power fiber laser system operating in the continuous-wave regime at a central wavelength of 1080 nm. A special ytterbium-doped fiber preform has been designed and fabricated by using modified chemical vapor deposition technique with the deposition percentages of 0.03mol% of $\text{Yb}_{2} \text{O}_{3}$ , 1.8mol% of $\text{Al}_{2}\text{O}_{3}$ , and 2.1mol% of $\text{P}_{2}\text{O}_{5}$ . Then it has been drawn to obtain an active fiber having core/cladding diameters of 26 μm/410 μm respectively. The numerical aperture of the fiber has been first predicted as 0.034 from refractive index profile of the preform. Afterward, this number has been verified with a simple test setup by altering the bending diameter of the fiber and the excitation conditions of it. To test the high power performance, a laser system has been constructed in a master oscillator power amplifier configuration, and ∼ 80 W seed signal power is amplified to 1.05 kW. The quality of the laser output beam has been measured in terms of $\text{M}^2$ value along both x and y coordinates as 1.11 and 1.16 respectively.- 29 January 2020
- Published by Institute of Electrical and Electronics Engineers (IEEE) in Journal of Lightwave Technology
- Vol. 38 (7) , 1915-1920
Demonstration of an All-Fiber Ultra-Low Numerical Aperture Ytterbium-Doped Large Mode Area Fiber in a Master Oscillator Power Amplifier Configuration Above 1 kW Power Level
We demonstrate an all-fiber ultra-low numerical aperture high power fiber laser system operating in the continuous-wave regime at a central wavelength of 1080 nm. A special ytterbium-doped fiber preform has been designed and fabricated by using modified chemical vapor deposition technique with the deposition percentages of 0.03mol% of $\text{Yb}_{2} \text{O}_{3}$ , 1.8mol% of $\text{Al}_{2}\text{O}_{3}$ , and 2.1mol% of $\text{P}_{2}\text{O}_{5}$ . Then it has been drawn to obtain an active fiber having core/cladding diameters of 26 μm/410 μm respectively. The numerical aperture of the fiber has been first predicted as 0.034 from refractive index profile of the preform. Afterward, this number has been verified with a simple test setup by altering the bending diameter of the fiber and the excitation conditions of it. To test the high power performance, a laser system has been constructed in a master oscillator power amplifier configuration, and ∼ 80 W seed signal power is amplified to 1.05 kW. The quality of the laser output beam has been measured in terms of $\text{M}^2$ value along both x and y coordinates as 1.11 and 1.16 respectively.- 1 October 2019
- Published by Elsevier in Optics and Lasers in Engineering
- Vol. 121, 54-60
Performance evaluation of fiber-based ballistic composites against laser threats
- 1 October 2019
- Published by Elsevier in Optics and Lasers in Engineering
- Vol. 121, 54-60
Performance evaluation of fiber-based ballistic composites against laser threats
- 29 August 2019
- Published by Optica Publishing Group in Applied Optics
- Vol. 58 (25) , 6926-6933
Combined method for the fabrication of high-power cladding light stripper using a buffered oxide etchant
Cladding light strippers (CLSs) are vital and one of the critical components for high-power fiber laser applications. In this study, we show the first studies of the formation mechanisms and optimum conditions of a CLS device using a buffered oxide etchant by a combined method of stain (wet) etching and vapor-phase etching. This high-power CLS was shown to result in a stripping performance of at the launched power of 333 W (pump limited). The thermal imaging demonstrates that the maximum temperature reached when operating the device at maximum launched power was . The atomic force microscopy (AFM) results show that the combined method yields crystal-like structures with the height in microscales, whereas other conventional methods give only nanoscale roughness. The method also preserves the diameter of the CLS device close to the bare fiber with about 10 μm tapering leads to a high surface area to strip unwanted light, which is good for heat dissipation. The combined method possesses the outcome of two methods, including both the crystal-like structures and nanosized hillocks, resulting in high-power stripping performance and robustness.- 29 August 2019
- Published by Optica Publishing Group in Applied Optics
- Vol. 58 (25) , 6926-6933
Combined method for the fabrication of high-power cladding light stripper using a buffered oxide etchant
Cladding light strippers (CLSs) are vital and one of the critical components for high-power fiber laser applications. In this study, we show the first studies of the formation mechanisms and optimum conditions of a CLS device using a buffered oxide etchant by a combined method of stain (wet) etching and vapor-phase etching. This high-power CLS was shown to result in a stripping performance of at the launched power of 333 W (pump limited). The thermal imaging demonstrates that the maximum temperature reached when operating the device at maximum launched power was . The atomic force microscopy (AFM) results show that the combined method yields crystal-like structures with the height in microscales, whereas other conventional methods give only nanoscale roughness. The method also preserves the diameter of the CLS device close to the bare fiber with about 10 μm tapering leads to a high surface area to strip unwanted light, which is good for heat dissipation. The combined method possesses the outcome of two methods, including both the crystal-like structures and nanosized hillocks, resulting in high-power stripping performance and robustness.- Open Access
- 1 June 2019
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- Vol. 8616, 1
A Combinatorial Buffered Oxide Etching Method for High-Power Cladding Light Stripper
High-power fiber lasers have been applied in many areas due to their advantages such as high beam quality, compact structure, flexibility and high efficiency. However, the absorption of the pump light is limited and a residual pumped light keeps propagating in the cladding. This residual pumped light affects the beam quality and can damage the whole system. Therefore, an efficient removal of excess high-power cladding light is critical for the safe operation of the high-power fiber lasers and high beam quality [1]. Adding a new structure to the cladding of the fiber leading to interrupt total internal reflection in the clad and scatter away the unwanted pump light is the generalized approach for a cladding light stripper (CLS) device fabrication. Also, it is important to scatter all the unwanted light uniformly along the CLS. Etching the fiber for surface damage and recoating the fiber [2] are two general methods for stripping the cladding light [3–5].
- 1 June 2019
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- Vol. 8616, 1
Open AccessA Combinatorial Buffered Oxide Etching Method for High-Power Cladding Light Stripper
High-power fiber lasers have been applied in many areas due to their advantages such as high beam quality, compact structure, flexibility and high efficiency. However, the absorption of the pump light is limited and a residual pumped light keeps propagating in the cladding. This residual pumped light affects the beam quality and can damage the whole system. Therefore, an efficient removal of excess high-power cladding light is critical for the safe operation of the high-power fiber lasers and high beam quality [1]. Adding a new structure to the cladding of the fiber leading to interrupt total internal reflection in the clad and scatter away the unwanted pump light is the generalized approach for a cladding light stripper (CLS) device fabrication. Also, it is important to scatter all the unwanted light uniformly along the CLS. Etching the fiber for surface damage and recoating the fiber [2] are two general methods for stripping the cladding light [3–5].
- 30 August 2017
- Published by Optica Publishing Group in Applied Optics
- Vol. 56 (25) , 7225-7229
1018 nm Yb-doped high-power fiber laser pumped by broadband pump sources around 915 nm with output power above 100 W
We demonstrate a 1018 nm ytterbium-doped all-fiber laser pumped by tunable pump sources operating in the broad absorption spectrum around 915 nm. In the experiment, two different pump diodes were tested to pump over a wide spectrum ranging from 904 to 924 nm by altering the cooling temperature of the pump diodes. Across this so-called pump wavelength regime having a 20 nm wavelength span, the amplified stimulated emission (ASE) suppression of the resulting laser was generally around 35 dB, showing good suppression ratio. Comparisons to the conventional 976 nm-pumped 1018 nm ytterbium-doped fiber laser were also addressed in this study. Finally, we have tested this system for high power experimentation and obtained 67% maximum optical-to-optical efficiency at an approximately 110 W output power level. To the best of our knowledge, this is the first 1018 nm ytterbium-doped all-fiber laser pumped by tunable pump sources around 915 nm reported in detail.
- 30 August 2017
- Published by Optica Publishing Group in Applied Optics
- Vol. 56 (25) , 7225-7229
1018 nm Yb-doped high-power fiber laser pumped by broadband pump sources around 915 nm with output power above 100 W
We demonstrate a 1018 nm ytterbium-doped all-fiber laser pumped by tunable pump sources operating in the broad absorption spectrum around 915 nm. In the experiment, two different pump diodes were tested to pump over a wide spectrum ranging from 904 to 924 nm by altering the cooling temperature of the pump diodes. Across this so-called pump wavelength regime having a 20 nm wavelength span, the amplified stimulated emission (ASE) suppression of the resulting laser was generally around 35 dB, showing good suppression ratio. Comparisons to the conventional 976 nm-pumped 1018 nm ytterbium-doped fiber laser were also addressed in this study. Finally, we have tested this system for high power experimentation and obtained 67% maximum optical-to-optical efficiency at an approximately 110 W output power level. To the best of our knowledge, this is the first 1018 nm ytterbium-doped all-fiber laser pumped by tunable pump sources around 915 nm reported in detail.