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Shi Y, Liu X, Ma L, Immonen M, Zhu L, He Z. Optical printed circuit boards with multimode polymer waveguides and pluggable connectors for high-speed optical interconnects. OPTICS EXPRESS 2023; 31:27776-27786. [PMID: 37710845 DOI: 10.1364/oe.497184] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/05/2023] [Accepted: 07/26/2023] [Indexed: 09/16/2023]
Abstract
We demonstrate the development of optical printed circuit boards (OPCBs) containing multimode polymer waveguides and pluggable optical connectors. The basic optical characteristics of the PCB-embedded waveguides, waveguide connectors, and high-speed performance were comprehensively evaluated. The fabricated OPCB comprises eight electrical layers and one optical layer. Waveguides are terminated at both ends with MT/MPO connectors. The optical channels comprising 10 cm-long waveguides embedded in OPCBs with two connectors show an average insertion loss of 6.42 dB. The resulting coupling loss is 0.77 dB per interface, which is very low and to our knowledge is among the lowest reported to date for waveguides embedded in rigid PCBs. 30 Gbps per channel NRZ data transmission was demonstrated with a measured waveguide bandwidth of 23 GHz × m, which gives a possible data traffic of 720 Gb/s for such 24-channel parallel optical link. Our efforts lay the foundation for the further development of OPCBs with higher performance.
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Frequency Response of Thermo-Optic Phase Modulators Based on Fluorinated Polyimide Polymer Waveguide. Polymers (Basel) 2022; 14:polym14112186. [PMID: 35683859 PMCID: PMC9182701 DOI: 10.3390/polym14112186] [Citation(s) in RCA: 2] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/10/2022] [Revised: 05/25/2022] [Accepted: 05/26/2022] [Indexed: 02/04/2023] Open
Abstract
Polymer waveguide phase modulators exhibit stable low-power phase modulation owing to their exceptional thermal confinement and high thermo-optic effect, and thus, have the merit of thermal isolation between channels, which is crucial for an optical phased array (OPA) beam scanner device. In this work, a waveguide phase modulator was designed and fabricated based on a high-refractive-index fluorinated polyimide. The propagation loss of the polyimide waveguide and the temporal response of the phase modulator were characterized. Moreover, the transfer function of the phase modulator including multiple poles and zeros was obtained from the measured frequency response. The polyimide waveguide modulator device demonstrated a fast response time of 117 μs for 1 kHz input signal, however, for 1 mHz step-function input, it exhibited an additional 5% phase change in 5 s.
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Shi Y, Ma L, Zhuang Y, He Z. Investigation on roughness-induced scattering loss of small-core polymer waveguides for single-mode optical interconnect applications. OPTICS EXPRESS 2020; 28:38733-38744. [PMID: 33379436 DOI: 10.1364/oe.410283] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/16/2020] [Accepted: 12/01/2020] [Indexed: 06/12/2023]
Abstract
We investigated the roughness-induced scattering loss (LossR) of small-core polymer waveguides fabricated using the photolithography method, both theoretically and experimentally. The dependence of LossR on the roughness parameter, waveguide dimension, operation wavelength, refractive index difference and distribution, polarization sensitivity, sidewall angle, and bending radius were studied. The surface roughness of both the sidewall and the top/bottom of the fabricated waveguides were measured using laser confocal microscope, and the results showed that the averaged sidewall roughness was approximately 60 nm, which is 3 times that of the top/bottom surface. As a result, the sidewall roughness-induced LossR is 9 times that induced by the top/bottom roughness. The calculated value of LossR agrees well with the measured value. LossR increases rapidly with the decrease in the waveguide width, especially when the waveguide width is reduced below 10 µm, at which the LossR is approximately 0.3 dB/cm. On the other hand, the dependence of LossR on the waveguide height is negligible. Our results provide guidance for developing single-mode polymer waveguides with low loss for optical interconnect applications.
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Abstract
This paper discusses the evolution observed in the field of high performance polymers and tries to forecast the future in different domains. The paper is divided into four sections: 1. From the 1960s to the 21st century. 2. What’s new in chemistry and why? 3. What could be the future for high performance polymers in structural applications, electrical industries, electronic and electro-optical industries, membrane technologies, fuel cell membranes and other fields such as conductive polymers. 4. Concluding remarks.
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Affiliation(s)
- B Sillion
- CNRS-SCA, BP 22, 69390 Vernaison, France and Sociétée Fraņcaise de Chimie, 250, Rue St Jacques, 75005 Paris, France
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Wei S, Zhenyu Z, Qiwei P, Qingtian G, Lina Y, Changshui F, Dong X, Hongzhen W, Jinzhong Y. Nonlinear Optical Properties and Chromophore Electrostatic Interactions for the Poly(ether ketone) Guest−Host Polymer Films. Macromolecules 2001. [DOI: 10.1021/ma001737b] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/29/2022]
Affiliation(s)
- Shi Wei
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China; Department of Chemistry, Shandong University, Jinan 250100, P. R. China; Institute of Optoelectronics, Department of Physics, Shandong University, Jinan 250100, P. R. China; and Semiconductor Institute Region of State Key Laboratory on Integrated Optoelectronics, Chinese Academy of Science, Beijing 100083, P. R. China
| | - Zhang Zhenyu
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China; Department of Chemistry, Shandong University, Jinan 250100, P. R. China; Institute of Optoelectronics, Department of Physics, Shandong University, Jinan 250100, P. R. China; and Semiconductor Institute Region of State Key Laboratory on Integrated Optoelectronics, Chinese Academy of Science, Beijing 100083, P. R. China
| | - Pan Qiwei
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China; Department of Chemistry, Shandong University, Jinan 250100, P. R. China; Institute of Optoelectronics, Department of Physics, Shandong University, Jinan 250100, P. R. China; and Semiconductor Institute Region of State Key Laboratory on Integrated Optoelectronics, Chinese Academy of Science, Beijing 100083, P. R. China
| | - Gu Qingtian
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China; Department of Chemistry, Shandong University, Jinan 250100, P. R. China; Institute of Optoelectronics, Department of Physics, Shandong University, Jinan 250100, P. R. China; and Semiconductor Institute Region of State Key Laboratory on Integrated Optoelectronics, Chinese Academy of Science, Beijing 100083, P. R. China
| | - Ye Lina
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China; Department of Chemistry, Shandong University, Jinan 250100, P. R. China; Institute of Optoelectronics, Department of Physics, Shandong University, Jinan 250100, P. R. China; and Semiconductor Institute Region of State Key Laboratory on Integrated Optoelectronics, Chinese Academy of Science, Beijing 100083, P. R. China
| | - Fang Changshui
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China; Department of Chemistry, Shandong University, Jinan 250100, P. R. China; Institute of Optoelectronics, Department of Physics, Shandong University, Jinan 250100, P. R. China; and Semiconductor Institute Region of State Key Laboratory on Integrated Optoelectronics, Chinese Academy of Science, Beijing 100083, P. R. China
| | - Xu Dong
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China; Department of Chemistry, Shandong University, Jinan 250100, P. R. China; Institute of Optoelectronics, Department of Physics, Shandong University, Jinan 250100, P. R. China; and Semiconductor Institute Region of State Key Laboratory on Integrated Optoelectronics, Chinese Academy of Science, Beijing 100083, P. R. China
| | - Wei Hongzhen
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China; Department of Chemistry, Shandong University, Jinan 250100, P. R. China; Institute of Optoelectronics, Department of Physics, Shandong University, Jinan 250100, P. R. China; and Semiconductor Institute Region of State Key Laboratory on Integrated Optoelectronics, Chinese Academy of Science, Beijing 100083, P. R. China
| | - Yu Jinzhong
- State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, P. R. China; Department of Chemistry, Shandong University, Jinan 250100, P. R. China; Institute of Optoelectronics, Department of Physics, Shandong University, Jinan 250100, P. R. China; and Semiconductor Institute Region of State Key Laboratory on Integrated Optoelectronics, Chinese Academy of Science, Beijing 100083, P. R. China
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Matsuura T, Kobayashi J, Ando S, Maruno T, Sasaki S, Yamamoto F. Heat-resistant flexible-film optical waveguides from fluorinated polyimides. APPLIED OPTICS 1999; 38:966-971. [PMID: 18305699 DOI: 10.1364/ao.38.000966] [Citation(s) in RCA: 12] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/26/2023]
Abstract
Heat-resistant flexible-film optical waveguides were fabricated from fluorinated polyimides. These waveguides operated in single mode and had low optical loss (0.3 dB/cm) at a wavelength of 1.3 microm for TE and TM polarizations. They also had good flexibility: The optical loss did not significantly change above a minimum radius of curvature of less than 20 mm. The birefringence of 9 x 10(-5) between the TE and TM polarizations is 2 orders of magnitude smaller than that for a waveguide upon a substrate. Moreover, these waveguides had high thermal stability and moisture resistance: The optical loss and single-mode behavior changed little after heating the waveguides at 420 degrees C for 1 h or after their exposure to 85% relative humidity at 85 degrees C for more than 350 h.
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Affiliation(s)
- T Matsuura
- NTT, 3-9-11 Midori-cho, Musashino-shi, Tokyo 180-8585, Japan
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