Fiber Optic Fundamentals - PAGE 1.
Fiber optics can challenge the first-timer to this part of analog RF signal distribution. There are some fundamentals from "the amplifier sweet spot article" that apply to getting analog RF signals onto fiber optic links and retrieving them as usable signals at the other end of the fiber. In these pages we will discuss the correct type of fiber and connectors required, the proper RF input signal levels to the fiber optic transmitters, and optimizing the fiber-to-RF conversion at the optical receiver with the correct received optical input power.
Transmission of wideband analog RF signals is only possible over single-mode
fiber (SMF-28) that has a 9-micron core diameter. Another code name for single-mode
fiber is G652. It depends on who made the fiber. If you have fiber jumpers
that are G657, the "bend insensitive fiber" in your installation, you will find
that our OTOA-1000 fiber optic attenuator will not work. The majority of fiber
installations use 1310 nm transmitters that do no work with "dispersion-shifted
fiber" that is optimized for 1550 nm wavelengths. SMF-28 and G652 fiber have
ZERO dispersion time-delay distortions at 1310 nm ONLY.
MULTI-MODE fiber will not work since the core diameter for that fiber is either
50 microns or 62.5 microns. The problem with the larger core diameters of MULTI MODE
FIBER is the reflection of the light rays bouncing off the side walls of the core, while
some rays of light go straight down the core without the zigzag path off the walls.
The effect of this causes the received light to no longer be "coherent" at the
end of the fiber. Mult-mode fiber is used in short lengths up to about 1000 feet,
and only for digital fiber signals where the laser blinks on and off representing binary
ones and zeroes. Digital signals can be regenerated at every receive point with
virtually no loss in the data. Analog RF signals cannot be regenerated. It is
important everything be done the correct way with RF signals over single-mode fiber optic
With single-mode fiber, the smaller core diameter keeps the rays of light coherent for greater distances. Transmission paths can reach many miles depending on the wavelength of the laser light transmitted. For now we will discuss only 1310 nanometer wavelength signals (1310nm). Other wavelengths can have slightly different fiber issues for those specialized networks.
Since these technical articles are about CATV applications, we will start with forward path, broadband CATV fiber optic transmitters. Many laser transmitters for converting wideband analog CATV signals to a light wave utilize "Butterfly" distributed feedback lasers (DFB) for optical power output levels from +8 dBm to +15 dBm. They have good RF linearity for CATV signals to minimize the unwanted RF distortions known as composite-triple-beats (CTB) a third-order distortion which is visible as lines in the pictures or a busy background. Composite second-order (CSO) distortions are also reduced. Poor carrier-to-noise (C/N) or noisy pictures occur when RF input signal levels are too low to overcome the noise figure of any active RF amplifier device. Lower-powered coaxial DFB lasers also have good performance for satellite L-Band applications.
Inside the fiber optic transmitter chassis, the first RF amplifier stages provide a broadband impedance match for the CATV signals transmitted to the laser device. The laser has a lower impedance than the 75-ohm coaxial cables of the network. The RF input circuitry handles that impedance transformation of the signals going to the laser itself. The laser works best with RF signals that are of EQUAL signal strength to each other. Depending on the design and gain of the RF input circuitry, each manufacturer will provide a technical manual indicating the optimum RF input level for their transmitter. The actual RF level can vary based on the number of analog and digital QAM-modulated channels. QAM signals are commonly set 6 dB lower than analog channels. The same "Sweet Spot" rules apply to any active RF device for optimum performance. This is the usual balancing act of C/N vs. CTB that occurs with any broadband analog RF amplifier device.
When discussing RF signals levels in CATV networks, the measurements are usually referenced to 1 millivolt of signal, which is 0 dBmV. Optical power levels in fiber are measured in reference to 1 milliwatt, or 0 dBm. The world of 50-ohm RF transmitters and receivers also uses the milliwatt (dBm) or 1-WATT referenced measurements (dBW).
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