Şemsettin Altındal
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Şemsettin Altındal has a total of 44 co-authors. Here are the top co-authors by number of shared publications:
- Yashar Azizian-Kalandaragh
Department of Photonics, Faculty of Applied Sciences, Gazi University, Ankara, Türkiye
6 shared publications - Suleyman Ozcelik
Photonics Application and Research Center, Gazi University, Ankara, Turkey
3 shared publications - Ahmet Gümüş
Ondokuz Mayıs University
2 shared publications - Ali Barkhordari
Faculty of Physics Shahid Bahonar University of Kerman Kerman 76131 Iran
2 shared publications - Dilber Esra Yıldız
Hitit University
2 shared publications - Ekmel Ozbay
Bilkent University
2 shared publications
Latest Publications
- 28 October 2025
- Published by Springer Nature in Journal of Materials Science: Materials in Electronics
- Vol. 36 (30) , 1-14
Assessment of wide frequency range admittance properties of Au/(ZnO:CeO2:PVP)/n-Si Schottky diodes
- 28 October 2025
- Published by Springer Nature in Journal of Materials Science: Materials in Electronics
- Vol. 36 (30) , 1-14
Assessment of wide frequency range admittance properties of Au/(ZnO:CeO2:PVP)/n-Si Schottky diodes
- 1 August 2024
- Published by IOP Publishing in Physica Scripta
- Vol. 99 (9) , 095504
A comparative study of the Au/n-Si (MS) and Au/(ZnO:CeO2:PVP)/n-Si (MPS) Schottky structures by using current/voltage characteristics in dark and under illumination
In the present study, both metal/semiconductor (MS) and metal/polymer/semiconductor (MPS) Schottky Diodes (SDs) were grown onto the same n-Si wafer to compare their electrical and optical characteristics. Firstly, ZnO and CeO2 nanostructures were synthesized by ultrasonic-assisted method (UAM), and structurally characterized by utilizing x-ray diffraction (XRD), Ultraviolet-visible spectroscopy (UV–vis), and Fourier-Transform-IR (FTIR) methods. The mean submicron crystallite sizes were estimated to be below 11.39 nm for CeO2 and 54.37 nm for ZnO nanostructures through the Debye–Scherrer method. The optical bandgap was calculated as 3.84 eV for CeO2 and 3.88 eV for ZnO nanostructures via Tauc plot. Electrical parameters such as reverse-saturation current (Io), ideality-factor (n), zero-bias barrier height (ΦBo), and rectification-ratio (RR) were found as 0.596 μA, 5.45, 0.64 eV, 2.74 × 105 in dark and 5.54 μA, 5.88, 0.59 eV, 8.60 × 103 under illumination for the MS SD and 0.027 μA, 4.36, 0.72 eV, 1.85 × 107 in dark and 0.714 μA, 5.18, 0.64 eV, 7.61 × 104 under illumination for the MPS SD, respectively. The energy-dependent profile of surface-states was obtained via the Card-Rhoderick method, by considering ΦB(V) and n. RR of the MPS SD is almost sixty-seven times the RR of the MS SD in the dark. The sensitivity of the MPS SD (=710) is nineteen and five-tenths the sensitivity of the MS SD (=36.4), so the MPS SD is considerably more sensitive to illumination. These results indicate that the (ZnO:CeO2:PVP) organic interlayer significantly improves the performance of the MS SD.
- 1 August 2024
- Published by IOP Publishing in Physica Scripta
- Vol. 99 (9) , 095504
A comparative study of the Au/n-Si (MS) and Au/(ZnO:CeO2:PVP)/n-Si (MPS) Schottky structures by using current/voltage characteristics in dark and under illumination
In the present study, both metal/semiconductor (MS) and metal/polymer/semiconductor (MPS) Schottky Diodes (SDs) were grown onto the same n-Si wafer to compare their electrical and optical characteristics. Firstly, ZnO and CeO2 nanostructures were synthesized by ultrasonic-assisted method (UAM), and structurally characterized by utilizing x-ray diffraction (XRD), Ultraviolet-visible spectroscopy (UV–vis), and Fourier-Transform-IR (FTIR) methods. The mean submicron crystallite sizes were estimated to be below 11.39 nm for CeO2 and 54.37 nm for ZnO nanostructures through the Debye–Scherrer method. The optical bandgap was calculated as 3.84 eV for CeO2 and 3.88 eV for ZnO nanostructures via Tauc plot. Electrical parameters such as reverse-saturation current (Io), ideality-factor (n), zero-bias barrier height (ΦBo), and rectification-ratio (RR) were found as 0.596 μA, 5.45, 0.64 eV, 2.74 × 105 in dark and 5.54 μA, 5.88, 0.59 eV, 8.60 × 103 under illumination for the MS SD and 0.027 μA, 4.36, 0.72 eV, 1.85 × 107 in dark and 0.714 μA, 5.18, 0.64 eV, 7.61 × 104 under illumination for the MPS SD, respectively. The energy-dependent profile of surface-states was obtained via the Card-Rhoderick method, by considering ΦB(V) and n. RR of the MPS SD is almost sixty-seven times the RR of the MS SD in the dark. The sensitivity of the MPS SD (=710) is nineteen and five-tenths the sensitivity of the MS SD (=36.4), so the MPS SD is considerably more sensitive to illumination. These results indicate that the (ZnO:CeO2:PVP) organic interlayer significantly improves the performance of the MS SD.
- Open Access
- 23 April 2024
- Published by IOP Publishing in Physica Scripta
- Vol. 99 (5) , 055967
Electrical and dielectric behaviors of Al/SiO2-surfactant/n-Si schottky structure in wide range of voltage and frequency
SiO2 surfactant insulator into Al/n-Si metal-semiconductor (MS) structure was fabricated into Al/SiO2-surfactant/n-Si metal–insulator–semiconductor (MIS) structure and its effect on the electrical properties of the final structure was investigated. The SiO2-surfactant layer is coated on the n-Si wafer by the spin coating technique. The I-V data is used to calculate the fundamental electrical parameters of this MIS structure. The density distribution of the surface states (Nss) is computed depending on the energy at forward potential. The current conduction mechanisms (CCMs) in the MIS structure are examined at the reverse and forward biases applied. To get more accurate and reliable results, the profiles of I-V and C/(G/ω)-V are measured at a wide range of bias voltage (0.25V-4V) and frequency (1kHz-1MHz), respectively. The performance of the MIS is significant due to the basic values of electrical parameters (n, I0, Rs, Rsh, Nss, ΦB0, and Rectifying Ration (RR)) and dielectric parameters (ε′, ε″, tan δ, M′, M″, Rs, and σ) compared with the MS structure. The other electrical parameters (ND, WD, Em, ΦΒ) are extracted from the slope and intercept of the reverse bias C−2-V plot as a function of frequency. Furthermore, the profile of voltage-dependent Rs and Nss was determined using different methods from I-V and C/G-V data and examined comparatively with each other. The changes in impedance properties with frequency and voltage of the MIS are discussed in detail.
- 23 April 2024
- Published by IOP Publishing in Physica Scripta
- Vol. 99 (5) , 055967
Open AccessElectrical and dielectric behaviors of Al/SiO2-surfactant/n-Si schottky structure in wide range of voltage and frequency
SiO2 surfactant insulator into Al/n-Si metal-semiconductor (MS) structure was fabricated into Al/SiO2-surfactant/n-Si metal–insulator–semiconductor (MIS) structure and its effect on the electrical properties of the final structure was investigated. The SiO2-surfactant layer is coated on the n-Si wafer by the spin coating technique. The I-V data is used to calculate the fundamental electrical parameters of this MIS structure. The density distribution of the surface states (Nss) is computed depending on the energy at forward potential. The current conduction mechanisms (CCMs) in the MIS structure are examined at the reverse and forward biases applied. To get more accurate and reliable results, the profiles of I-V and C/(G/ω)-V are measured at a wide range of bias voltage (0.25V-4V) and frequency (1kHz-1MHz), respectively. The performance of the MIS is significant due to the basic values of electrical parameters (n, I0, Rs, Rsh, Nss, ΦB0, and Rectifying Ration (RR)) and dielectric parameters (ε′, ε″, tan δ, M′, M″, Rs, and σ) compared with the MS structure. The other electrical parameters (ND, WD, Em, ΦΒ) are extracted from the slope and intercept of the reverse bias C−2-V plot as a function of frequency. Furthermore, the profile of voltage-dependent Rs and Nss was determined using different methods from I-V and C/G-V data and examined comparatively with each other. The changes in impedance properties with frequency and voltage of the MIS are discussed in detail.
- Open Access
- 16 March 2023
- Published by American Chemical Society (ACS) in ACS Applied Electronic Materials
- Vol. 5 (3) , 1804-1811
Negative Capacitance Behavior at Low Frequencies of Nitrogen-Doped Polyethylenimine-Functionalized Graphene Quantum Dots-Based Structure
- 16 March 2023
- Published by American Chemical Society (ACS) in ACS Applied Electronic Materials
- Vol. 5 (3) , 1804-1811
Open AccessNegative Capacitance Behavior at Low Frequencies of Nitrogen-Doped Polyethylenimine-Functionalized Graphene Quantum Dots-Based Structure
- 23 June 2022
- Published by IOP Publishing in Semiconductor Science and Technology
- Vol. 37 (8) , 085008
DC and RF performance of lateral AlGaN/GaN FinFET with ultrathin gate dielectric
In this study, an enhancement-mode (E-mode) GaN high electron mobility transistor (HEMT) with lateral tri-gate structure field effect transistor (FinFET) is proposed. To passivate the fin width, while keeping the normally-off performance of the FinFET intact, an ultrathin aluminium-oxide/sapphire (Al2O3) gate dielectric is proposed (in a basic single-finger 0.125 mm device). Later, the DC and radio frequency (RF) performances of the proposed FinFET designs (with optimized fin width and Al2O3 thickness) are compared with that of conventional planar HEMT. DC and RF measurements are performed using power transistors in ten-fingers configuration, with a total gate periphery of 2.5 mm. The effect of Fin structure and Al2O3 thickness on the electrical performance of HEMTs, including threshold voltage (V th) shift, transconductance (g m) linearity, small-signal gain, cut off frequency (f t), output power (P out), and power-added efficiency (PAE) are investigated. Based on our findings, FinFET configuration imposes normally-off functionality with a V th = 0 .2 V, while the planar architecture has a V th = − 3 .7 V. Originating from passivation property of the alumina layer, the FinFET design exhibits two orders of magnitude smaller drain and gate leakage currents compared to the planar case. Moreover, large signal RF measurements reveals an improved P out density by over 50% compared to planar device, attributed to reduced thermal resistance in FinFETs stemming from additional lateral heat spreading of sidewall gates. Owing to its superior DC and RF performance, the proposed FinFET design with ultrathin gate dielectric could bear the potential of reliable operating for microwave power applications, by further scaling of the gate length.
- 23 June 2022
- Published by IOP Publishing in Semiconductor Science and Technology
- Vol. 37 (8) , 085008
DC and RF performance of lateral AlGaN/GaN FinFET with ultrathin gate dielectric
In this study, an enhancement-mode (E-mode) GaN high electron mobility transistor (HEMT) with lateral tri-gate structure field effect transistor (FinFET) is proposed. To passivate the fin width, while keeping the normally-off performance of the FinFET intact, an ultrathin aluminium-oxide/sapphire (Al2O3) gate dielectric is proposed (in a basic single-finger 0.125 mm device). Later, the DC and radio frequency (RF) performances of the proposed FinFET designs (with optimized fin width and Al2O3 thickness) are compared with that of conventional planar HEMT. DC and RF measurements are performed using power transistors in ten-fingers configuration, with a total gate periphery of 2.5 mm. The effect of Fin structure and Al2O3 thickness on the electrical performance of HEMTs, including threshold voltage (V th) shift, transconductance (g m) linearity, small-signal gain, cut off frequency (f t), output power (P out), and power-added efficiency (PAE) are investigated. Based on our findings, FinFET configuration imposes normally-off functionality with a V th = 0 .2 V, while the planar architecture has a V th = − 3 .7 V. Originating from passivation property of the alumina layer, the FinFET design exhibits two orders of magnitude smaller drain and gate leakage currents compared to the planar case. Moreover, large signal RF measurements reveals an improved P out density by over 50% compared to planar device, attributed to reduced thermal resistance in FinFETs stemming from additional lateral heat spreading of sidewall gates. Owing to its superior DC and RF performance, the proposed FinFET design with ultrathin gate dielectric could bear the potential of reliable operating for microwave power applications, by further scaling of the gate length.
- 24 January 2021
- Published by Springer Nature in Journal of Materials Science: Materials in Electronics
- Vol. 32 (3) , 3451-3459
Electrical characterization of Au/n-Si (MS) diode with and without graphene-polyvinylpyrrolidone (Gr-PVP) interface layer
- 24 January 2021
- Published by Springer Nature in Journal of Materials Science: Materials in Electronics
- Vol. 32 (3) , 3451-3459
Electrical characterization of Au/n-Si (MS) diode with and without graphene-polyvinylpyrrolidone (Gr-PVP) interface layer
- 1 September 2019
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- p. X-017-017
Utilization of Al2O3/PVP nanocomposite as an interfacial layer for Schottky structures
The objective of this study is to investigate the effect of (Al 2 O 3- PVP) on the electrical characteristics in Al/p-Si (MS) and Al/(Al 2 O 3 -PVP)/p-Si (MPS) structures. At the first stage of this study, the preparation mechanism of A 2 O 3 nanostructures and its structural and morphological properties have been reported. Finally, the fabricated Schottky structures on the base of (Al 2 O 3 -PVP) nanocomposites have been reported. The forward and reverse bias I-V measurements at room temperature were also have been investigated and compared with each other to see the effect of organic interfacial layer on the main electrical characteristics.
- 1 September 2019
- Published by Institute of Electrical and Electronics Engineers (IEEE)
- p. X-017-017
Utilization of Al2O3/PVP nanocomposite as an interfacial layer for Schottky structures
The objective of this study is to investigate the effect of (Al 2 O 3- PVP) on the electrical characteristics in Al/p-Si (MS) and Al/(Al 2 O 3 -PVP)/p-Si (MPS) structures. At the first stage of this study, the preparation mechanism of A 2 O 3 nanostructures and its structural and morphological properties have been reported. Finally, the fabricated Schottky structures on the base of (Al 2 O 3 -PVP) nanocomposites have been reported. The forward and reverse bias I-V measurements at room temperature were also have been investigated and compared with each other to see the effect of organic interfacial layer on the main electrical characteristics.