发明公开
EP1411339A3 Wavelength dispersion measuring apparatus and polarization dispersion measuring appparatus
审中-公开
设备,用于测量的波长色散和偏振色散测量装置
- 专利标题: Wavelength dispersion measuring apparatus and polarization dispersion measuring appparatus
- 专利标题(中): 设备,用于测量的波长色散和偏振色散测量装置
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申请号: EP04001628.9申请日: 1999-02-17
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公开(公告)号: EP1411339A3公开(公告)日: 2004-05-12
- 发明人: Otani, Akihito , Otsubo, Toshinobu , Takara, Hidehiko , Kawanishi, Satoki , Yamabayashi, Yoshiaki
- 申请人: Anritus Corporation , Nippon Telegraph and Telephone Corporation
- 申请人地址: 1800, Onna Atsugi-shi, Kanagawa-ken JP
- 专利权人: Anritus Corporation,Nippon Telegraph and Telephone Corporation
- 当前专利权人: Anritus Corporation,Nippon Telegraph and Telephone Corporation
- 当前专利权人地址: 1800, Onna Atsugi-shi, Kanagawa-ken JP
- 代理机构: Meissner, Bolte & Partner
- 优先权: JP3909998 19980220
- 主分类号: G01J9/02
- IPC分类号: G01J9/02 ; G01M11/00
摘要:
A first tunable wavelength pulse light source (22) is driven by a reference signal to emit a first optical pulse. An optical demultiplexer (24) demultiplexes a first optical pulse emitted from the first pulse light source (22) into a reference optical pulse and an incident optical pulse to be sent into an object to be measured. An optical multiplexer (26) multiplexes the reference optical pulse and an outgoing optical pulse passing through the object to output multiplexed light. A second pulse light source (23) generates a second optical pulse which is synchronous with the first optical pulse and delays a predetermined time for each period of the first optical pulse. A sampling unit (27, 27a, 27b) receives the multiplexed light and the second optical pulse to obtain an optical pulse train signal proportional to the intensity of the multiplexed light obtained in synchronism with the second optical pulse. From the optical pulse train signal from the sampling unit (27, 27a, 27b), a signal processor (37) obtains an envelope formed by peaks of individual optical pulses forming the optical pulse train. The wavelength dispersion of the object is obtained by measuring the delay time of the outgoing optical pulse passing through the object on the basis of intervals between the peaks of the envelope.
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