fig1 is a schematic representation of the passive - to - active coupled cavity laser of the invention ; fig4 is a diagram showing continuous wave and square wave pulsed spectra for the laser alone 4 ( a ) and for the coupled cavity arrangement of the invention 4 ( b ). the principles on which the invention is based are illustrated by fig1 . the active laser cavity is shown in close proximity to the passive graded index cavity . an air space of 10μ is shown between the active and passive cavities . alternative - y , the two cavities may be butted , or even joined together with epoxy or the like . if separated as shown it is preferred that they be close e . g . within 50μ , and preferably within 10μ , to maximize coupling . this spacing will affect power output more than mode purity so it is a design tradeoff depending on the power needed . there is however a point where losses become so large that insufficient power is coupled back into the active resonant cavity to effect mode selection . the front end of the graded index cavity facing the laser can be antireflection coated in case reflection from that surface affects mode stability . referring again to fig1 the passive graded index cavity is bounded by a totally or partially reflecting mirror . the reflectivity of the mirror depends on the amount , if any , of radiation desired from that end of the coupled cavity assembly . the device can be designed for output coupled to a transmission fiber through the mirror as shown in fig2 in which case the mirror will be designed to pass the amount of light output . also it can be designed with a power ( or even a spectral ) monitor at the other facet of the active cavity as shown . fig3 shows an alternative arrangement with the output radiation taken from the active cavity of the device . the monitor is optically coupled to the partially transmission mirror . the coupled - cavity laser of this invention was demonstrated in the following way . grinrod cavities with a short length compared to the laser cavity length were prepared from graded index multimode fiber . the fiber was epoxied inside a glass capillary tube , and was polished from both ends to a predetermined length . one end was then coated with cr and au for high reflectivity . the coated end was then epoxied on a glass rod for handling . the coupling geometry of the grinrod cavity to the laser was as shown in fig1 . the mode spacing of the ingaasp bh laser is 7å , from which the effective cavity length in air is 1200μm . the air gap between the grinrod cavity and the laser facet was ≲ 10μm . this air spaced cavity did not contribute to the mode selection effect due to its large cavity mode spacing ≳ 120 × laser mode spacing ). the graded index fiber used for the grinrod cavity had a 0 . 29 numerical aperture and 70μm core diameter . the length of the grinrod cavity was 170μm which was made shorter than a quarter pitch to have a focal point in air . this results in nearly a 4 : 1 ratio of the external cavity mode spacing to the laser mode spacing . a ratio chosen between 3 : 1 and 6 : 1 would be appropriate . by employing the coupled cavity approach described here it is also appropriate to use shorter active laser cavities than one might otherwise find expedient from the standpoint of laser lifetime . the 6mw / facet continuous wave spectrum for the ingaasp bh laser biased at 51ma ( i th = 23ma ) at 23 degrees c . is shown in fig4 ( a ). a maximum of 40 % increase in light output was observed when the grinrod cavity was coupled to the laser . the corresponding 6 mw continuous wave single - longitudinal - mode spectrum at the same heat sink temperature is shown in fig4 ( b ). the laser with the coupled external cavity was pulsed by a square wave generator from threshold to 6mw . a beam splitter was used for simultaneous measurements of the spectrum and the light output pulses detected with a high speed ingaas / inp pin photodiode . ( see t . p . lee , c . a . burrus , k . ogawa , and a . g . dentai , electronics letters , volume 17 , no . 12 , p . 431 , 1981 ). the on / off extinction ratio was better than 30 : 1 . the spectra of the grinrod external cavity laser under 300 mhz and 500 mhz square wave modulation are also shown in fig4 ( b ). the corresponding multimoded spectra for the laser alone are shown in fig4 ( a ). the same longitudinal mode was stabilized with the external cavity as the modulation rate was varied . the most significant side mode intensity relative to the main mode intensity was suppressed by 23 db and 20 db respectively at 300 mhz and 500 mhz . under continuous wave operation the side mode suppression ratio was better than 25 db . when the laser was pulsed from above i th , the amplitude of the first relaxation oscillation peak decreased and the mode suppression ratio approached that under continuous wave operation with the penalty of a decreased on / off light output extinction ratio . various additional modifications and extensions of this invention will become apparent to those skilled in the art . all such variations and deviations which basically rely on the teachings through which this invention has advanced the art are properly considered to be within the spirit and scope of this invention .