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Dive into the research topics where Takahisa Harayama is active.

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Featured researches published by Takahisa Harayama.


Proceedings of SPIE, the International Society for Optical Engineering | 2007

Experimental investigation of Sagnac beat signals using semiconductor fiber-optic ring laser gyroscope (S-FOG) based on semiconductor optical amplifier (SOA)

Shuichi Tamura; Keizo Inagaki; Hiroyuki Noto; Takahisa Harayama

We are conducting research to confirm the performance of a semiconductor fiber-optic ring laser gyroscope (S-FOG) featuring a semiconductor in its laser cavity. This S-FOG consists of a semiconductor optical amplifier (SOA) as a gain medium, a polarization-maintaining fiber to make a ring cavity, and a directional coupler to take part of the optical power out of the cavity. One of the advantages of the S-FOG is the adaptability of the laser cavity, which allows us to examine many cases of S-FOG applications easily. In the first case, we observed that the S-FOG generated Sagnac beat signals whose peak frequency was proportional to the rotation rate when it rotated. In the second case, we changed the area surrounded by the ring cavity (the fiber) and its perimeter and maintained a near-fixed oscillation wavelength of the ring laser. In this case, all of our experimental results were in good agreement with theoretical calculations, within a few percent. In the third case, we changed the oscillation wavelength and fixed the shape of the ring cavity. In this case, our results were also in good agreement with theoretical calculations. In the fourth case, we examined the Sagnac beat spectrum generated by the S-FOG in detail. The linewidth of the Sagnac beat spectrum increases as the area bounded by the optical path in the ring cavity becomes smaller, or as the length of the cavity becomes shorter. Our experimental results show that the S-FOG works as a gyro and that there exists practical potential for a semiconductor ring laser gyro.


Optical Fiber Sensors (2006), paper ME7 | 2006

Sagnac Beat Signals Observed in Semiconductor Fiber-Optic Ring Laser Gyroscope

Keizo Inagaki; Shuichi Tamura; Hiroyuki Noto; Takahisa Harayama

A semiconductor fiber-optic ring laser gyroscope, which consist of a semiconductor optical amplifier as a gain medium and polarization-maintaining fiber to form a ring resonator, generate Sagnac beat signals demonstrating good agreement with theoretical calculations.


Proceedings of SPIE, the International Society for Optical Engineering | 2008

Improvement of accuracy of angular velocity detection in semiconductor fiber-optic ring laser gyroscope

Tomoki Ishida; Shuichi Tamura; Satoshi Sunada; Keizo Inagaki; Shigeru Saito; Takahisa Harayama

A semiconductor fiber-optic ring laser gyroscope (S-FOG) consists of a semiconductor optical amplifier (SOA) and optical fiber to form a ring cavity. The fiber ring cavity enables larger sizes and smaller scattering, while the SOA gain is shared by the clockwise (CW) and counterclockwise (CCW) propagating modes. When the S-FOG is rotated, a new beat signal called the Sagnac beat frequency is observed. We investigated the effect of the fiber ring cavitys length on detection characteristics. Detection sensitivity was not dependent on the number of laps of fiber ring cavity. However, when the cavity length became longer, the linewidth of Sagnac beat became narrower, and then accuracy of angular velocity detection improved. The relation between the linewidth Δ ν of the Sagnac beat and cavity length P was proved to be Δ ν ≈ P-1.86.


Proceedings of SPIE, the International Society for Optical Engineering | 2008

Earth's rotation rate detection using an extremely large semiconductor fiber optic gyroscope extending over 10,000 m2

Keizo Inagaki; Shuichi Tamura; Tomoko Tanaka; Hiroyuki Noto; Takahisa Harayama

We detect the Earths rotation rate using a semiconductor fiber optic gyroscope (S-FOG), which is an active ring laser gyroscope that consists of a semiconductor optical amplifier (SOA) and a fiber optic ring resonator. Four different optical fiber layouts with different scale factors in rotation rate measurement are configured and measured. Expected Sagnac beat signals proportional to the scale factors are observed. The maximum layout of S-FOG is extended over 10,898 m2, which, to our knowledge, is the largest active ring laser gyroscope ever built.


Archive | 2007

Laser gyro and electronic device using the same

Noriyuki Yokouchi; Junji Yoshida; Takahisa Harayama; Takehiro Fukushima; Akihiko Kasukawa; Shuichi Tamura; Keizou Inagaki; Morito Matsuoka


Archive | 2006

Semiconductor laser gyro

Tomoko Tanaka; Takehiro Fukushima; Keizo Inagaki; Takahisa Harayama


Optical Fiber Sensors (2006), paper TuE63 | 2006

Nonlinear Sagnac effect for ring laser gyroscopes

Takahisa Harayama; Satoshi Sunada; Shuichi Tamura; Keizo Inagaki; Hiroyuki Noto


Archive | 2005

Gyro employing semiconductor laser

Takahisa Harayama; Takehiro Fukushima


Archive | 2005

Semiconductor laser gyroscope

Takehiro Fukushima; Takahisa Harayama; Nobuo Saito; Shuichi Tamura; 卓久 原山; 信雄 斎藤; 修一 田村; 丈浩 福嶋


Laser Science, LS 2013 | 2013

Optics InfoBase Conference Papers

Takehiro Fukushima; Susumu Shinohara; Satoshi Sunada; Takahisa Harayama; Koichiro Sakaguchi; Yasunori Tokuda

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Shuichi Tamura

The Furukawa Electric Co.

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