Shohei Kosuga
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Research Interests
Shohei Kosuga has a total of 21 co-authors. Here are the top co-authors by number of shared publications:
Osamu Hashimoto
Department of Electrical Engineering and Electronics, College of Science and Engineering, Aoyama Gakuin University 1 , 5-10-1 Fuchinobe, Chuo-ku, Sagamihara, Kanagawa 252-5258, Japan
3 shared publicationsRyosuke Suga
Department of Electrical Engineering and Electronics, College of Science and Engineering, Aoyama Gakuin University 1 , 5-10-1 Fuchinobe, Chuo-ku, Sagamihara, Kanagawa 252-5258, Japan
3 shared publications- Shinji Koh
Department of Electrical Engineering and Electronics, College of Science and Engineering, Aoyama Gakuin University
3 shared publications - Shigeru Kanazawa
NTT Innovative Devices Corporation, Atsugi, Japan
2 shared publications Takahiro Nakamura
NTT Device Innovation Center, NTT Corporation, Atsugi, Japan
2 shared publicationsTakeshi Watanabe
Department of Electrical Engineering and Electronics, College of Science and Engineering, Aoyama Gakuin University 1 , 5-10-1 Fuchinobe, Chuo-ku, Sagamihara, Kanagawa 252-5258, Japan
2 shared publications
Latest Publications
- Open Access
- 4 March 2025
- Published by Institute of Electrical and Electronics Engineers (IEEE) in Journal of Lightwave Technology
- Vol. 43 (13) , 6037-6043
165-GHz Bandwidth, 0.53 A/W Vertical-Illumination Photodiode Enabled by Interference-Based Absorption Enhancement
We present a vertical-illumination InP/InGaAs photodiode (PD) with a monolithically integrated micro-lens having a 165-GHz bandwidth. Interference-based absorption enhancement resulted in a 0.53-A/W responsivity and a record 70-GHz external bandwidth-efficiency product, while maintaining a broader absorption spectral range compared with conventional resonant cavity enhanced PDs. The PD features an electric field confinement by an inverted p-down structure, which results in a low dark current of approximately 1 pA and low manufacturing variability. In addition, an InP microlens is monolithically integrated to increase the effective aperture by up to 20 μm, which improves assembly tolerance.
- 4 March 2025
- Published by Institute of Electrical and Electronics Engineers (IEEE) in Journal of Lightwave Technology
- Vol. 43 (13) , 6037-6043
Open Access165-GHz Bandwidth, 0.53 A/W Vertical-Illumination Photodiode Enabled by Interference-Based Absorption Enhancement
We present a vertical-illumination InP/InGaAs photodiode (PD) with a monolithically integrated micro-lens having a 165-GHz bandwidth. Interference-based absorption enhancement resulted in a 0.53-A/W responsivity and a record 70-GHz external bandwidth-efficiency product, while maintaining a broader absorption spectral range compared with conventional resonant cavity enhanced PDs. The PD features an electric field confinement by an inverted p-down structure, which results in a low dark current of approximately 1 pA and low manufacturing variability. In addition, an InP microlens is monolithically integrated to increase the effective aperture by up to 20 μm, which improves assembly tolerance.
- 27 November 2024
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Photonics Technology Letters
- Vol. 37 (1) , 57-60
A 226.875-Gbit/s/λ Optical Receiver Based on a High-Frequency Integration by Flip-Chip Mounting
A high-speed optical receiver for IM-DD 226.875-Gbit/s/$\lambda $ transmission was designed and fabricated by using high-frequency, integrated flip-chip (FC) mounting. Thanks to the developed FC-mounting technique, the optical receiver exhibited high 3-dB bandwidth and less-fluctuation optical-to-electrical (O/E) frequency response. The fabricated optical receiver demonstrated 3-dB bandwidth of 55.1 GHz with less-fluctuation O/E frequency response up to 50 GHz (i.e., Nyquist frequency under 100-Gbaud operation at 4-PAM modulation frequency). The simulated transmission performance of the optical receiver reveals that its link budget for 226.875-Gbit/s/$\lambda $ transmission is expanded by 3.7 dB by using the developed FC-mounting technique. The fabricated optical receiver also experimentally demonstrated transmission of a 226.875-Gbit/s signal over 20-km SSMF.- 27 November 2024
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Photonics Technology Letters
- Vol. 37 (1) , 57-60
A 226.875-Gbit/s/λ Optical Receiver Based on a High-Frequency Integration by Flip-Chip Mounting
A high-speed optical receiver for IM-DD 226.875-Gbit/s/$\lambda $ transmission was designed and fabricated by using high-frequency, integrated flip-chip (FC) mounting. Thanks to the developed FC-mounting technique, the optical receiver exhibited high 3-dB bandwidth and less-fluctuation optical-to-electrical (O/E) frequency response. The fabricated optical receiver demonstrated 3-dB bandwidth of 55.1 GHz with less-fluctuation O/E frequency response up to 50 GHz (i.e., Nyquist frequency under 100-Gbaud operation at 4-PAM modulation frequency). The simulated transmission performance of the optical receiver reveals that its link budget for 226.875-Gbit/s/$\lambda $ transmission is expanded by 3.7 dB by using the developed FC-mounting technique. The fabricated optical receiver also experimentally demonstrated transmission of a 226.875-Gbit/s signal over 20-km SSMF.- Open Access
- 1 March 2021
- Published by AIP Publishing in AIP Advances
- Vol. 11 (3) , 035136
Optically transparent antenna based on carrier-doped three-layer stacked graphene
We fabricated an optically transparent monopole antenna using graphene film and investigated the feasibility of the film as an electrode material for antennas. A low sheet resistance (80 Ω/sq) was attained by stacking the graphene films and carrier doping with an ionic liquid. The optical transmittance of the carrier-doped three-layer stacked graphene film was greater than 90%, enabling it to be embedded in highly transparent objects without altering their landscape. Using the monopole antenna structure with a metal ground plane, we measured the reflection and radiation characteristics of the graphene monopole antenna, excluding the contribution from the power feeding components. The radiation efficiency of the graphene monopole antenna, which was measured by the Wheeler cap method, was determined to be 52.5% at 9.8 GHz. Through the measurements of the graphene monopole antenna, we demonstrated that the carrier-doped three-layer stacked graphene film can be used as an electrode material for optically transparent antennas.
- 1 March 2021
- Published by AIP Publishing in AIP Advances
- Vol. 11 (3) , 035136
Open AccessOptically transparent antenna based on carrier-doped three-layer stacked graphene
We fabricated an optically transparent monopole antenna using graphene film and investigated the feasibility of the film as an electrode material for antennas. A low sheet resistance (80 Ω/sq) was attained by stacking the graphene films and carrier doping with an ionic liquid. The optical transmittance of the carrier-doped three-layer stacked graphene film was greater than 90%, enabling it to be embedded in highly transparent objects without altering their landscape. Using the monopole antenna structure with a metal ground plane, we measured the reflection and radiation characteristics of the graphene monopole antenna, excluding the contribution from the power feeding components. The radiation efficiency of the graphene monopole antenna, which was measured by the Wheeler cap method, was determined to be 52.5% at 9.8 GHz. Through the measurements of the graphene monopole antenna, we demonstrated that the carrier-doped three-layer stacked graphene film can be used as an electrode material for optically transparent antennas.
- Open Access
- 15 November 2020
- Published by Wiley in Engineering Reports
- Vol. 3 (5)
Characterization of contact properties at interface between metal and graphene up to 15 GHz
The contact properties between metal and monolayer chemical vapor deposition (CVD) graphene were investigated. Coplanar waveguides (CPWs) composed of CVD graphene‐based signal lines and Au‐based ground lines were fabricated. The S‐parameters of the CPWs were experimentally measured from 1 to 15 GHz. The contact properties were analyzed using a lumped component‐based equivalent circuit model, which consists of the experimentally determined parallel contact resistance and the parallel contact capacitance. The calculated S‐parameters of the model roughly agreed with the measured ones, which indicated that the model was suitable for analyzing the contact properties between metal and graphene up to 15 GHz. Because the impedance of the contact capacitance (4.8 × 10−3 Ω) was four orders of magnitude lower than that of the contact resistance (50 Ω) at 15 GHz, the current flow was more capacitive and efficient than that in the DC band. The ratio of power consumption and power storage in the microwave band to the total power consumption in the DC band decreased with increasing frequency and increasing contact capacitance. Therefore, higher contact capacitance is preferable in designing microwave devices with a metal/graphene‐based feeding structure, such as antennas and transmission lines.
- 15 November 2020
- Published by Wiley in Engineering Reports
- Vol. 3 (5)
Open AccessCharacterization of contact properties at interface between metal and graphene up to 15 GHz
The contact properties between metal and monolayer chemical vapor deposition (CVD) graphene were investigated. Coplanar waveguides (CPWs) composed of CVD graphene‐based signal lines and Au‐based ground lines were fabricated. The S‐parameters of the CPWs were experimentally measured from 1 to 15 GHz. The contact properties were analyzed using a lumped component‐based equivalent circuit model, which consists of the experimentally determined parallel contact resistance and the parallel contact capacitance. The calculated S‐parameters of the model roughly agreed with the measured ones, which indicated that the model was suitable for analyzing the contact properties between metal and graphene up to 15 GHz. Because the impedance of the contact capacitance (4.8 × 10−3 Ω) was four orders of magnitude lower than that of the contact resistance (50 Ω) at 15 GHz, the current flow was more capacitive and efficient than that in the DC band. The ratio of power consumption and power storage in the microwave band to the total power consumption in the DC band decreased with increasing frequency and increasing contact capacitance. Therefore, higher contact capacitance is preferable in designing microwave devices with a metal/graphene‐based feeding structure, such as antennas and transmission lines.
- 30 October 2018
- Published by Wiley in Microwave and Optical Technology Letters
- Vol. 60 (12) , 2992-2998
Radiation properties of graphene‐based optically transparent dipole antenna
The radiation properties of a graphene‐based optically transparent half‐wavelength dipole antenna in microwave bands was investigated. The resonance frequencies of a reference Au antenna and a graphene antenna having the same antenna structures were 9.5 and 21.6 GHz, respectively, owing to the difference in conductivity. Despite the low conductivity of graphene, the gain of the graphene antenna was 1 dB higher than that of the Au antenna. We also showed the feasibility of using graphene‐based optically transparent antenna through the measurements of transmission characteristics between two graphene antenna.
- 30 October 2018
- Published by Wiley in Microwave and Optical Technology Letters
- Vol. 60 (12) , 2992-2998
Radiation properties of graphene‐based optically transparent dipole antenna
The radiation properties of a graphene‐based optically transparent half‐wavelength dipole antenna in microwave bands was investigated. The resonance frequencies of a reference Au antenna and a graphene antenna having the same antenna structures were 9.5 and 21.6 GHz, respectively, owing to the difference in conductivity. Despite the low conductivity of graphene, the gain of the graphene antenna was 1 dB higher than that of the Au antenna. We also showed the feasibility of using graphene‐based optically transparent antenna through the measurements of transmission characteristics between two graphene antenna.