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External-cavity diode lasers provide absolute references for WDM testing Successful WDM operation depends he rapid growth in data traffic is driving development of higher- on eliminating crosstalk between capacity optical-fiber-transmis- the different wavelength channels. This sion methods based on wave- requires that all the active and passive length-division multiplexing system components operate within the (WDM). In WDM, several lasers at dif- spectral window they were designed for, without undue ferent wavelengths drift or chirp. At the simultaneously Michael Lang manufacturing, transmit separate streams of data along a single fiber. At installation, and servicing/repair the receiving end, the different wave- stages, this requirement creates a need lengths are optically separated and indi- to check the wavelength performance vidually detected. The transmission of key components such as lasers, filcapacity of an existing fiber link can, ters, and fiber gratings. Wavelength therefore, be instantly increased by a meters, spectrometers, and spectrum factor equal to the number of individual analyzers are important in this area. wavelengths used. The rapid evolution However, while these tools may suffice of WDM technology has created the for field testing of the latest WDM sysneed for laser sources with output that tems, more-accurate, absolute methods is reliably locked to a known absolute are needed for use in quality control wavelength (frequency) with high precision. Recently, the International H12C14N Telecommunications Union (Arlington, VA) created a standard for 32-channel WDM transmission that consists of 40 1.50 1.51 1.52 1.53 1.54 1.55 1.56 wavelength channels, separated by only 100 GHz (0.8 nm), H13C14N eight of which are for overhead—signal management. The close channel spacing is necessary to ensure that all the 1.50 1.51 1.52 1.53 1.54 1.55 1.56 channels fit under the highgain portion of the erbium12C H 2 2 doped fiber-amplifier gain curve, centered around 1545 nm. Looking to the future, higher-density WDM formats 1.50 1.51 1.52 1.53 1.54 1.55 1.56 with 64 channels separated by only 50 GHz (0.4 nm) are pre13 C2H2 dicted. And some researchers are already experimenting with channel spacings of less than 2 GHz. Absorbance T 1.50 MICHAEL LANG is Product Manager of Newport Corporation’s Tunable Laser Diode products manufactured in Boulder, Colorado. e-mail: [email protected] 1.51 1.52 1.53 1.54 1.55 1.56 and testing laboratories, as well as for the research and development effort to produce future generations of WDM technology. Absolute wavelength metrics One method of providing an absolute yet compact wavelength standard is to lock the output of a diode laser to an atomic or molecular spectral line. Indeed, such absorption and emission lines have long been used as absolute wavelength standards in several fields. Until recently, however, there were almost no spectral standards in the 1550-nm spectral region. This absence was partly because there are few strong spectral absorptions in this region and also because there was little commercial demand for such absolute standards. The explosive growth of WDM technology has changed this situation. In the past two years, tremendous advances have been made in calibrating the spectra of both acetylene (C2H2) and hydrogen 1.57 cyanide (HCN), because these molecules have a combination of vibrational overtone absorption lines that span the entire 1550-nm erbium gain region (see Fig. 1). The first atlas of 1.57 acetylene lines has now been published by the Tokyo Institute of Technology,1 which claims 150-kHz absolute precision in the frequency domain—traceable to the cesium atomic-clock 1.57 frequency via an absorption line of rubidium. Also, researchers at NIST (Boulder, CO) have characterized the small, yet measurable, pressure shifts (up to 200torr pressure) of these lines. 1.57 Wavelength (µm) FIGURE 1. Vibrational overtone bands of hydrogen cyanide (HCN) and acetylene (C2H2) together span the erbium gain region. Third-derivative locking Unlike the single atomic lines of neon and krypton, acetylene and hydrogen cyanide each Reprinted from the June 1998 edition of LASER FOCUS WORLD Copyright 1998 by PennWell Design and Applications have a comb of spectral lines through- drifts in the absorption measurement. A out the spectral region of interest. feedback loop actively adjusts the dc Equally important, their absorption position of the tuning mirror to maintain lines can be detected in simple, compact a zero third-derivative signal. Using this cells with no need for noisy, delicate approach, the compact, portable source discharge cells. For these reasons, Envi- has a long-term stability of ±1 MHz, or ronment Optical Sensors Inc. (ESOI; one part in 108. Boulder, CO) chose acetylene and There are many rotational lines in the hydrogen cyanide absorption lines as C 2 H 2 or HCN spectra to which the the basis for a series of rugged reference WDM reference source can be stabisources for WDM work (see Fig. 2). lized. In practice, the end user selects The emitting element is a laser diode from this list of absolute wavelengths— with a highly efficient (reflectivity just as RF engineers have selected the <10–5) antireflection coating on its front facet. This diode Tuning mirror operates in a Piezo translation Littman-Metcalf Collimated Fiber external cavity, laser diode Out where the position of the tuning mirror Diffraction grating Beamsplitter determines the output wavelength. The Beamsplitter collimated output of this cavity is couInGaAs Absorption cell photodetector pled into a FC/APC InGaAs (fiberconnecphotodetector tor/angled physical connector) fiber coupler. A beam- FIGURE 2. WDM reference source from Environmental Optical Sensors splitter, positioned Inc. consists of an external-cavity diode laser locked to an integral absorpbefore this coupler, tion cell containing either acetylene (C2H2) or hydrogen cyanide (HCN). splits off 5% of the collimated laser light, which allows a frequency of crystal reference oscillators normalized (dual-channel) measure- for many years. The angle of the tuning ment of the absorption in a cell contain- mirror is then permanently set at the ing C2H2 or HCN, by a pair of indium factory. To further enhance the econogallium arsenide (InGaAs) photo- my of this approach, several active heads (at different wavelengths) can be detectors. Both C 2 H 2 and HCN have linewidths on the order WDM of 1 GHz, due to reference source Doppler broadening. To accurately lock to Source Fast InGaAs line center, a techunder test detector Spectrum analyzer nique called thirdor frequency counter derivative locking is used. A small (about 1 MHz) frequency FIGURE 3. Wavelength-division-multiplexing source is calibrated by meadither is applied to suring a heterodyne beat frequency using a high-speed InGaAs detector. the laser diode by the piezoelectric actuator that translates the used interchangeably with the same tuning mirror. The detection electronics electronic controller. then take the third derivative of the normalized absorption signal in the fre- Heterodyne source testing quency domain. This third derivative These reference sources can be used to has the twin advantages of being calibrate the accuracy of important extremely steep as it passes through zero WDM diagnostic tools such as waveand being immune to any background length meters and high-resolution spec- trometers, which are then used to check the passive components such as fiber gratings and receiver filters. These diagnostic tools also can measure the wavelength of the stabilized distributed-feedback diodes and fiber-grating controlled laser-diode sources used in WDM. The most accurate measurements of these sources, however, are made by direct measurement against the WDM reference source. The laser being measured can then be traced back to the cesium clock with ±1 MHz precision. In this type of heterodyne measurement, the output of the WDM reference source and the test laser are coupled into a high-speed InGaAs photodetector (see Fig. 3). The resulting beat frequency is measured with a high-accuracy spectrum analyzer or frequency counter. How fast must the photodetector be? When answering this question, another advantage of C2H2 and HCN becomes apparent. The rotational line spacing in both molecules is less than 30 GHz. It is possible, therefore, to select a WDM reference source within roughly 15 GHz of a given frequency. Detecting beat frequencies of 15 and even 30 GHz is straightforward, because there are offthe-shelf InGaAs photodetectors capable of 50-GHz detection and custom devices up to 100 GHz. Larger intervals can be calibrated by “daisy-chaining” the photodetectors. The WDM reference source is used to calibrate one laser at an interval of less than 50 GHz, which is then used to calibrate another laser at an additional interval of less than or equal to 50 GHz, and so on. Passing along a frequency standard from one source to another in this type of linkage has long been the standard method by which all calibrated spectral lines are ultimately referenced back to the cesium atomic clock through intermediate calibrated spectral features. The overall backbone capacity of fiberoptic telecommunications systems is expected to double approximately every 3.7 months. This growth rate makes development of stabilized, accurate, absolute frequency references a technological imperative. ❏ REFERENCE 1. K. Nakagawa et al., “Accurate optical frequency atlas of the 1.5 µm bands of acetylene,” JOSA, B, vol. 13, 2708 (1996). Newport Corporation • 1791 Deere Ave. • Irvine, CA 92606 • 800-222-6440 M-11984