Phase Difference Control between Adjacent Optical Pulses by Means of Stabilization of Delayed Interferometer and Its Application to an OTDM
Multiplier for RZ Optical Clock
Hiroyuki TODA and Junichi MIYASHITA
(Received January 22, 2009)
Phase difference between adjacent optical pulses is stabilized by means of stabilization of a delayed interferometer (DI), which can be considered as an optical time-division multiplexed (OTDM) multiplexer. A continuous wave (CW) tunable laser, where the wavelength is different from that of the optical pulse, was used to stabilize the DI. We have confirmed that the phase difference of more than 8 was controlled using a piezo-electric transducer and a lock-in amplifier by tuning the CW laser wavelength. Moreover, we investigated an optical clock quadruple multiplier by serially concatenating the OTDM multiplexer. In 40GHz optical clock generation experiment, we have observed the temporal waveforms and optical spectra when in-phase and out-of phase optical clocks were successfully generated, respectively. The undesired optical sidebands were suppressed to be more than 15 dB for both cases.
Keywords: delayed interferometer, stabilizatin of interferometer, optical time-division multiplexing (OTDM), OTDM multiplexer, clock multiplier
Ĩ«§Úċļ§Úċ}ļqÅuyĬļĬĘļģnĘ
Ĩ«§Úċ}(+qIX>įjëx°q7ZC7ģnĘ
· ä ą d ] a ù _
1.
ËĖĹĥqĤmá.é»ļqm
çâ'iĠqÅuyĬĺoptical time-division multiplexing; OTDMϹă.ãíô ĬĈ + 1-4)ĽOTDM (+qL/2HiĠ ļIJ¾ +qIX>Ĵåjë£iĠÞ²¯ĵ.c+
ì),+Ľ$ļqm¥¦.à +qIX>¦1JCEÉĝ+
ļIJ¾qIX>ƧÚ(ļqIX>
įjë}+ļqIX>ª|
$ĽļQPSK ē(oē
Department of Electronics, Faculty of Science and Engineering, Doshisha University, Kyoto
Telephone: +81-774-65-6356, Fax: +81-774-65-6801 E-mail: {htoda@mail, dth0146@mail4}.doshisha.ac.jp
ì. OTDM }+&%ļOTDM qĘ
á ļqIX>įjëx°]}
±ĶĒķ+Ľ,$ļē,qm
q>P7EX.UGBjë£.}+Ã
×,+ļćijx°.±Ĉ+Ľ Êó ļØĮħüq (CW) Y^;.ã Ĩ«§ÚċĺDIĻ.}+(*ļIJ¾q IX>jë£.h³x°]}+OTDM ĬĘ+Ľ)ļL/2H DI .êw2Ó¾üļ4ģnq7ZC7OTDM ĬĘÎČûÌ.+ĽÊģnĘ ļ 1 ØĮY^;ļqIX>įjë.}
RZ$ CS-RZ7ZC7.â¶+.
ÞĮ+Ľ
Fig. 1. Delayed interferometer as an OTDM multiplexer and its stabilization scheme.
Fig. 2. Operation principle of the phase stabilization.
ĺCWĻqY^;ĺØĮ: CWĻ.ã§Úċ
}.ĽqIX>ØĮ ļCW
.}+ļqIX>įjë.x°+
+5)Ľ
Fig. 1øÏ¶.ðĽqIX>ĺØĮPĻ
ħüqĺØĮCWĻ.ØļJ^S>NWCBĺBSĻ eRV^ )+ĬĘ"rz+Ľe qĘiÁÅį£Ĩ«Åį+ĽÝÃRV
^ 1 Ě>D^=`Q3\EK4Aú
ĺPZTĻ*f),+Ľ>D^=Ĩ«Åį.
Ď+ĽĬĘtz )L/2HMVC88Y
^D1\8ĺFBGĻ.ãP¶u.İļZC 72\0\N.ãL1^FHC7. +Ľ
Fig. 2 ļ§ÚċqĘ£L§ÚċtzqI[
^Ð+ĽPZT ØÂ m- ē .ÄĽZC72\0\N§Úċtz
(
)
2 : 1 1
2 c T 1 n n
cw
p
+ +
=
=T+(2n+1) (1)
ļT IJ¾qIX>įıĺT = L/cĻļc qĥ+Ľ§Úċ.}$$CW.
}+ļqĊØÂ£ Ôlļ .ħ üè}++Ľ
ĸ ļL/2HW\8Y^; )ÿ*Ğ
ØÂ10 GHzļ~os¦2 psqIX>ĺP = 1546.2 nmĻ.T = 6.25 psĬ}ļCW.}
ÅqIX>įjë}.ÛĽ ļ
ĬĘtzq>P7EX )ÛĽFig. 3 ÛûÌ )ļIJ¾qIX>įjë. 8 g`
-x°+.îĐĽ ħü
ö ļPZTFV2HÇêÙtzĴļPZT
´ªÖ,+Ľ
3. ('
2.ğ#ĬĘ.Ó¾üļĨ«Åį.Ī vĎ+ļq7ZC7ģnĘ.϶+
+Ľ ļL/2HĨ«§Úċ.ê w2Ó¾üļ4ģnq7ZC7OTDMĬ
Ęğ#+ 6)ĽÊĘ ļ1 ØĮY Fig. 3. Phase difference between adjacent optical pulses versus CW wavelength CW.
^;ļqIX>įjë.} RZ $
CS-RZ7ZC7.â¶+ÞĮ+Ľ
Fig. 44ģnqĘ϶.ðĽU^FÉY
^;ĺMLLĻ )qIX>ĺØĮ: Pļÿ*Ğ
É: TĻ.ĬĘ"rz+ĽĨ«§ÚċĺDIĻ ļeL/2H6CNVļ>D^=`*
f),9WT^B )+ĽÝÃ0^S qL/2H PZTú¤f),ļjëē.
++ĽDI1 qĘ£L1 (= cT/4ļc qĥ).ĎļIX>įıT/4IJ¾2 qIX>.tz+Ľ,.qĘ£L2 (= cT/2).Ď DI2rz+ļÿ*ĞØÂ4ģ
n,q7ZC7tz,+Ľ ļ2 DI .}+%ØĮ CW NZ^Mq ĺØĮ CWĻ ļĬĘtzp )rz+϶
+ĽPZT ļ,,ØÂm1m2
- ē.Äļ2.ğ#(ļ ZC72\0\NCWq§Úċtz$,+
ēØÂ¶u¼¦.Ît+ļ,đ£m
*ļL1^FHC7. +ļØĮCW +§Ú¢$ ĕjĀZC7,+ĽÊ
Ę ļDI2.¢jĀZC7ļCWq.DI1
"Ģĩļm1m2+ļ1 ØĮ
Y^;2DI.}+ĽFig. 5 ļCW
IX>qØĮ P q§ÚÐ+Ľ (a) ëĺRZĻq7ZC7.â¶++Ľ Üþ P§Ú.ĄÆþļ,Ç&
Ç¡+LļIX>įjë 0&
+Ľ$ļL= L1CW§ÚĺþĻ Üþġë+(CW.Ď+ĽDI1.
þĕjĀ}+ļIX>įjë 0 qIX>â¶+ĺFig. 5(a)ÜaĻĽÅļ
L = L2 = 2L1 ļÜþþ ë+%ļ
DI2.þ¢jĀĺFig. 5(a)ÜbĻ}
+ļĬĘtz jë RZq7ZC7.
â¶+Ľ_ÃļjëęĺCS-RZĻq7ZC7 .â¶+ ļFig. 5(b)(ļL= L1Üþ
þë+(CW.Ď,!(Ľ
ĸ ļÿ*ĞØÂ10GHzļ¦10psL/
2HW\8Y^;ĺlP =1546.06nmĻ.ãļDI1 Ĩ«Åį. 25psļDI2 Ĩ«Åį. 50ps
40GHzq7ZC7.â¶ĽFig. 6 ļ (a)RZq
7ZC7ĺCW =1551.02nmĻļ(b)CS-RZq7ZC7
ĺCW =1551.18nmĻ.tzÅ>P7EX
+ĽbĈ:2FH\F15dBg`º,ĽFig.
7 ļRZq7ZC7.tzÅļ:\NW\8 (a) RZ optical clock
(b) CS-RZ optical clock
Fig. 5. Operation principle of the phase stabilization when (a) in-phase (RZ) and (b) out-of-phase (CS-RZ) optical clocks are generated.
MLL: Mode-locked laser, PD: Photo diode, LIA: Lock-in amplifier, TLS: Tunable laser source
Fig. 4. An optical clock quadruple multiplier by serially concatenating the delayed interferometers.
5<Z>9^NĉÛÅᨮ+ĽÎtø
¥¦ 40GHz +Ľÿ*ĞØÂ 40GHz
qIX>¦ 10ps+%ļqIX>į
4.
Ĩ«§ÚċqĘ£.}+ļIJ¾q IX>įjë£.x°+ OTDM ĬĘ.¿
Íļïĸ.ĂĽJ^S>NWCBĭ )+Ĩ«§ÚċL1^FHC7x°. ļØ ĮY^;ØĮ.}+ļ8g`
-IJ¾qIX>įjë£.x°+
.îĐĽ)ļqĘ£æ+L/2HĨ
«§Úċ.êw 2 Ó¾üļ1 ØĮY^
;IX>įjë},+q7ZC74ģ nĘ.¿ÍĽØĮY^;ØĮ.Īv Ď+ļ RZ$ CS-RZ 40 GHzq7Z C7.â¶ĽÊ¸× ØĮY^;±Ĉ +&Ôěè÷x°.Ă +Ľ$ļ kHz òªkØx°.Ă%ļ ĹĥĘ_vbĈ+ÞĮ&È+Ľ
ĔĜ
Êíô ļñ¹ă¼āÑϨ¶19©ª<^?ç
½ďĸÀ{.$ĽčĔ³.Ą$Ľ
%% !! ##
1) R. Ludwig, S. Weisser, C. Schmidt-Langhorst, L.
Raddatz and C. Schubert, "160 Gb/s-DPSK OTDM-transmission over 480 km using 160 km repeater spans and advanced forward-error-correction," Optical Fiber Communication (OFC 2007) and National Fiber Optic Engineers (NFOEC 2007), OWE4 (2007).
2) H. Murai, M. Kagawa, H. Tsuji, K. Fujii,
"EA-Modulator-Based Optical Time Division Multiplexing/Demultiplexing Techniques for 160-Gb/s Optical Signal Transmission," IEEE J. Sel. Top.
Quantum Electron., vol. 13, no. 1, pp. 70-78 (2007).
3) M. Daikoku, T. Miyazaki, I. Morita, H. Tanaka, F.
Kubota, and M. Suzuki, "8x160-Gb/s WDM Field Transmission Experiment With Single-Polarization RZ-DPSK Signals and PMD Compensator," IEEE Photon. Tech. Lett., vol. 18, no. 2, pp. 391-393 (2006).
(a) RZ optical clock
(b) CS-RZ optical clock
Fig. 6. Optical spectra of the generated 40GHz optical clocks by the optical clock quadruple multiplier.
(a) Without stabilization.
(b) With stabilization.
Fig. 7. Waveforms of the generated 40GHz RZ optical clock.ĺ10ps/divĻ
4) T. Hirooka, M. Okazaki, K. Osawa, and M. Nakazawa,
"160 Gbit/s-900 km DPSK transmission with time-domain optical Fourier transformation, European Conference on Optical Communication (ECOC2007), 1.3.3, (2007).
5) a·ä"Ĩ«§Úċ}(+qIX>į
jëx°," 2007m@B-10-18 (2007).
6) aėõ·ä"}Ĩ«§Úċ(+
RZq7ZC74ģnqÅuyĬĘ," 2008m
ýB-10-72 (2008).