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ETTC'2003 - SEE

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BACK<br />

Low Phase Noise Optical Links for Reference Frequency<br />

Distribution in Satellite Payloads<br />

Gianandrea QUADRI, Horacio MARTINEZ-REYES,<br />

Benoit BENAZET (1) , Olivier LLOPIS<br />

LAAS-CNRS, 7 Avenue du Colonel Roche, 31077 Toulouse, Cedex 04, France<br />

(1) Alcatel Space, 26 av. J. F. Champollion, B.P. 1187, 31037 Toulouse, France<br />

Abstract — Various circuits dedicated to high spectral<br />

purity signal transmission using fiber optics are presented.<br />

Three application types are investigated : reference<br />

frequency distribution at 10 MHz, IF distribution at<br />

800 MHz and microwave synthesized signals at 3.5 GHz. The<br />

reception circuit is an optically synchronized oscillator,<br />

which provides a good signal conditioning far from the<br />

carrier while maintaining the high input signal quality close<br />

to the carrier.<br />

I. INTRODUCTION<br />

Fiber optics constitutes an attractive alternative to<br />

conventional wiring for numerous analog applications.<br />

Indeed, in addition to its small size and low mass, the fiber<br />

does not interfere with electronic devices and provides an<br />

excellent isolation of the transmitted signal. One of the<br />

targeted application of our work is the reference<br />

frequency signal distribution to various subsystems of a<br />

telecommunications satellite. Another application could<br />

be remote antenna synchronization and control.<br />

However, to meet our system requirements, the fiber<br />

optics link should not degrade the signal quality, and<br />

particularly its phase noise. To this purpose, the optically<br />

synchronized oscillator [1,2] is an efficient approach<br />

which naturally filters the signal far from the carrier, thus<br />

removing the additional noise due to the optical link.<br />

Moreover, an optically controlled oscillator delivers a<br />

constant output power, which is an interesting feature for<br />

a clock or reference frequency delivering network.<br />

Different types of optically synchronized oscillators<br />

may be investigated. The simplest one uses a conventional<br />

photodiode to detect the amplitude modulated optical<br />

signal, and the resulting microwave signal is used in a<br />

classical injection lock of a microwave oscillator, or as a<br />

reference signal in a PLL. In this case, we speak about an<br />

indirect optically synchronized oscillator. Another<br />

possibility is to realize the oscillator with a transistor<br />

sensitive to the optical power (photo-transistor) and thus<br />

to control directly the oscillator amplifying element.<br />

In this study, various solutions are investigated for a<br />

low phase noise optical link at 10 MHz, 800 MHz and<br />

3.5 GHz. Indirect synchronization has been chosen for the<br />

two lower frequencies, and both indirect and direct<br />

synchronization have been investigated at 3.5 GHz using<br />

two types of active devices : an InP based bipolar phototransistor<br />

(photo-HBT) [3], and an InP based HEMT<br />

device [4].<br />

The application goal for the 10 MHz link is the<br />

reference frequency distribution in a telecommunications<br />

satellite. The signal from the ultra stable quartz crystal<br />

oscillator should be transmitted with no degradation of its<br />

phase noise, and this is a very stringent requirement.<br />

The 800 MHz application is also in the field of<br />

telecommunications satellites, and corresponds to an<br />

intermediate frequency in the satellite.<br />

The 3.5 GHz frequency is a first attempt to compare<br />

the different approaches for high spectral purity<br />

microwave signal distribution. The application is not<br />

clearly defined today, but it could be in the field of active<br />

antennas.<br />

II. PHOTO-OSCILLATOR ; THEORY<br />

The indirect optical injection locking can be efficiently<br />

described by combining the classical noise modeling of an<br />

optical link [5,6] to the theory of injection locked<br />

oscillators [7,8]. The only questionable point is probably<br />

in the interaction between the two systems : has the<br />

photodiode (or its associated amplifier) an effect on the<br />

oscillator noise ? But if the two systems are isolated in<br />

some way from one to another, this approach should<br />

apply. The following equation (from Kurokawa’s theory<br />

[8]), is an expression of the output phase noise spectral<br />

density of a synchronized oscillator, versus the input<br />

signal phase noise Sφ input, the free running oscillator phase<br />

noise Sφ free, the locking bandwidth flock and the offset<br />

from carrier fm.<br />

2<br />

⎛ f m ⎞<br />

⎜ ⎟<br />

⎜ f ⎟<br />

1<br />

⎝ lock ⎠<br />

Sϕ<br />

=<br />

⋅ S<br />

S<br />

sync<br />

ϕ +<br />

⋅<br />

2 input<br />

2 ϕ free<br />

⎛ f m ⎞<br />

⎛ f m ⎞<br />

1 + ⎜ ⎟<br />

+ ⎜ ⎟<br />

⎜ f ⎟<br />

1<br />

⎜<br />

lock<br />

f ⎟<br />

⎝ ⎠<br />

⎝ lock ⎠

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