(19)
(11) EP 1 806 557 A8

(12) CORRECTED EUROPEAN PATENT APPLICATION
Note: Bibliography reflects the latest situation

(15) Correction information:
Corrected version no 1 (W1 A2)

(48) Corrigendum issued on:
09.06.2010 Bulletin 2010/23

(88) Date of publication A3:
31.03.2010 Bulletin 2010/13

(43) Date of publication:
11.07.2007 Bulletin 2007/28

(21) Application number: 07003547.2

(22) Date of filing: 25.01.2002
(51) International Patent Classification (IPC): 
G01B 9/00(2006.01)
G02B 6/34(2006.01)
G02B 6/12(2006.01)
G02F 1/225(2006.01)
(84) Designated Contracting States:
DE FR GB

(30) Priority: 26.01.2001 JP 2001017943

(62) Application number of the earlier application in accordance with Art. 76 EPC:
02250526.7 / 1227297

(71) Applicant: NIPPON TELEGRAPH AND TELEPHONE CORPORATION
Tokyo, 100-8116 (JP)

(72) Inventors:
  • Goh, Takashi NTT Intellectual Property Center
    Musashino-shi Tokyo 180-8585 (JP)
  • Abe, Makoto NTT Intellectual Property Center
    Musashino-shi Tokyo 180-8585 (JP)
  • Inoue, Yasuyuki NTT Intellectual Property Center
    Musashino-shi Tokyo 180-8585 (JP)
  • Okuno, Masayuki NTT Intellectual Property Center
    Musashino-shi Tokyo 180-8585 (JP)
  • Saida, Takashi NTT Intellectual Property Center
    Musashino-shi Tokyo 180-8585 (JP)

(74) Representative: Roberts, Gwilym Vaughan et al
Kilburn & Strode LLP 20 Red Lion Street
London WC1R 4PJ
London WC1R 4PJ (GB)

 
Remarks:
This application was filed on 21 - 02 - 2007 as a divisional application to the application mentioned under INID code 62.
 


(54) Interferometer and its fabrication method


(57) An interferometer includes a waveguide core (2), and thin film heaters (4a, 4b) with widths W1 and W2. The thin film heaters are mounted directly above the waveguide core, and operate as two types of different annealing regions. The annealing, which is carried out by supplying current to the thin film heaters (4a,4b), can alter the quality of the cladding (3), and change the stress applied on the waveguide core (2), thereby making it possible to control the polarization dependency. Thus changing the width of the thin film heaters (4a, 4b) and/or the amount of the supply current thereto enables the permanent control of the effective refractive index (birefringence index) independently in the transverse electric polarization mode and the transverse magnetic polarization mode. This enables the transverse electric polarization mode to be adjusted to a phase difference of λ/2, and the transverse magnetic polarization mode to a phase difference of zero.