For the first time, the beat spectra between adjacent modes of a nearly single-mode semiconductor laser are measured. Self-locking processes are observed, indicating the importance of three-mode interactions. Measurements of the laser linewidth and relative intensity noise ire also presented.Longitudinal-mode competition causes many undesirable properties of the noise spectrum o F a nearly single-mode laser, including enhancement of the low-frequency (I 1 GHz) relative intensity noise (RIN) [1,2] and rebroadening of the laser linewidth. Beating between the fields of adjacent modes also causes pulsations in the carrier population and carrier distribution function [3]. Threemode interactions modify the longitudinal mode spectra through four-wave mixing [4] and self frequency-locking [5]. In this paper we show direct experimental evidence for self frequencylocking in a semiconductor laser.In order to illustrate the importance and generality of mode-coupling interactions, Fig. 1 s h o w the RF spectrum of a directly modulated bulk 1.3 pm-wavelength Fabry-Perot laser. The wings of the RF spectrum surrounding the peak at 3 GHz (modulation frequency) are caused by translatilm of the low-frequency intensity noise to the subcarrier frequency [6]. The different RF spectra are paired with different optical emission spectra (inserts) arising from small changes in the current (.<2 mA) and temperature (5 degrees) at constant power. The peculiar shape of the emission spectrum associated with lower RIN suggests that it may originate from the self-frequency modulation of a dominant longitudinal mode at a modulation frequency close to the longitudinal mode separation [5], while the higher-noise spectrum may instead result from the incoherent superposition of multiple, competing modes without a single, dominant mode. Fig. 2 shows the beat spectra of adjacent longitudinal modes in a 2.5-mm.-long InGaAdGaAs SQW laser. The 14 GHz intermode frequency corresponds to a difference of 0.04 nm at the lasing wavelength of 970 nm. The inserts show the gross longitudinal mode spectra (resolution is 0.1 nm). At 1.1 times threshold the beat spectrum shown in Fig. 2a has a width of -20 MHz with iin unresolved shoulder due to the overlap of the beats between the main mode and side modes on either side (i.e., three modes, two beats) with small dispersion. At this power the beat linewidth is in approximate agreement with independent linewidth measurements, if it is assumed that the noi,se between modes is not strongly correlated. At about 1.3 times threshold the side-mode suppression is -30 dB, and the beat spectrum disappears. It reappears in Fig. 2b at about 1.5 times threshold after a sudden locking transition in which the beat frequency is slightly shifted and the beat linewidth dramatically narrows by about four orders of magnitude. This transition is accompanicd by a distinct change in the longitudinal mode spectrum, indicative of self-frequency modulation.Self-frequency modulation (accompanied by amplitude variations) has been independently v...