A homogeneously broadened two-mode ring laser has two metastable states in which one or the other mode intensity is zero. Quantum fluctuations cause the system to switch spontaneously, and at random times, between these states. The probability distribution of the light intensity of one laser mode has been measured, and found to exhibit two completely resolved peaks at zero and nonzero intensities, as predicted. This confirms the existence of a first-order laser phase transition.PACS numbers: 42.50.+ q, 42.60.EbNumerous experiments with single-frequency ring lasers have demonstrated that, when the gain medium is homogeneously broadened, one of the two traveling-wave modes tends to suppress the other one. 1 " 5 This phenomenon, which appears to have been first predicted by White, 6 is the result of mode competition for the emitted photons. The equations of motion of the twomode laser exhibit two metastable solutions, in which one or the other mode amplitude is zero. However, in general there is no stable state, and sooner or later a large quantum fluctuation causes the system to switch spontaneously from one metastable state to the other. The mode switching is associated with a discontinuity in the order parameter for the phase transition of the laser field, 7 and therefore corresponds to one of the few cases in which a laser exhibits a firstorder phase transition. 4 As a result of the metabistability, the probability distribution (P(l) of the light intensity / of either mode exhibits two peaks, for which evidence has recently been obtained by photon-counting experiments. 4 However, it was not possible to extract the form of {l) explicitly from the counting measurements., We now wish to report the results of direct measurements of the probability distribution (P(/), that confirm the existence of the first-order laser phase transition in a quantitative manner.The equations of motion for the slowly varying complex mode amplitudes E x (t) 9 E 2 (t) of a twomode laser were already derived by Lamb. 8 ' 9 With the addition of Langevin noise terms q x (t) 9 q 2 (t) to represent the spontaneous emission fluctuations, and in dimensionless units, they , take the form dE x /dt =(<*! -| JSj 2 -I |E a | 2 )E X + q ± , dE 2 /dt = (a 2 -| E 2 1 2 -€ I E x | 2 )E 2 + q 2 .