The influence of fiber dispersion on the code form of the optical mm-wave signal generated by single sideband intensity-modulation

We have theoretically investigated the transmission performance of the optical mm-wave generation by using an external modulator based on single sideband (SSB) intensity modulation. Though the SSB millimeter (mm)-wave can immune the fading effect, the baseband signals with a high bit rate are degraded greatly after transmission along fiber. The main reason is that the fiber dispersion causes the time shift of the code edges; therefore the maximum transmission distance of the baseband signals is limited. The experimental and simulation results agree well with our theoretical analysis. We also propose a novel scheme to extend the transmission distance. In this novel scheme, the data signals are modulated only onto one of the two optical carriers; hence the shift of the code edges in the down-converted signals after transmission is eliminated.

[1]  G. Chang,et al.  All-optical mixer based on cross-absorption modulation in electroabsorption modulator , 2005 .

[2]  To extend delivery distance of the optical MM‐wave generated by DSB modulation and vestigial sideband filtering , 2006 .

[3]  A. Nirmalathas,et al.  Analysis of optical carrier-to-sideband ratio for improving transmission performance in fiber-radio links , 2006, IEEE Transactions on Microwave Theory and Techniques.

[4]  B. Della,et al.  Millimeter-wave power-fading compensation for WDM fiber-radio transmission using a wavelength-self-tunable single-sideband filter , 2002 .

[5]  Gee-Kung Chang,et al.  Optical millimeter-wave generation or up-conversion using external modulators , 2006, IEEE Photonics Technology Letters.

[6]  G. Agrawal Fiber‐Optic Communication Systems , 2021 .

[7]  Dalma Novak,et al.  Overcoming chromatic-dispersion effects in fiber-wireless systems incorporating external modulators , 1997 .

[8]  Mikio Maeda,et al.  Optical single sideband modulator for distribution of digital broadcasting signals on millimetre-wave band based on self-heterodyne , 2004 .

[9]  Wayne V. Sorin,et al.  Elimination of the fibre chromatic dispersion penalty on 1550 nm millimetre-wave optical transmission , 1997 .

[10]  D. Novak,et al.  Broad-band millimeter-wave (38 GHz) fiber-wireless transmission system using electrical and optical SSB modulation to overcome dispersion effects , 1998, IEEE Photonics Technology Letters.

[11]  Robert A. Griffin,et al.  System capacity for millimeter-wave radio-over-fiber distribution employing an optically supported PLL , 1999 .

[12]  Lin Chen,et al.  A Radio-Over-Fiber System With a Novel Scheme for Millimeter-Wave Generation and Wavelength Reuse for Up-Link Connection , 2006, IEEE Photonics Technology Letters.

[13]  Gee-Kung Chang,et al.  All-optical 16 /spl times/ 2.5 Gb/s WDM signal simultaneous up-conversion based on XPM in an NOLM in ROF systems , 2005 .

[14]  Gee-Kung Chang,et al.  Seamless integration of an 8/spl times/2.5 Gb/s WDM-PON and radio-over-fiber using all-optical up-conversion based on Raman-assisted FWM , 2005 .

[15]  Jong-In Song,et al.  Error-free simultaneous all-optical upconversion of WDM radio-over-fiber signals , 2005 .

[16]  U. Gliese,et al.  Chromatic dispersion in fiber-optic microwave and millimeter-wave links , 1996 .

[17]  Ian D. Robertson,et al.  Improved single-sideband microwave upconverter using injection of unwanted sideband , 2005 .