We show that an Optical Parametric Oscillator which is simultaneously resonant for several modes, either spatial or temporal, generates both below and above threshold a multimode non-classical state of light consisting of squeezed vacuum states in all the non-oscillating modes. We confirm this prediction by an experiment dealing with the degenerate TEM01 and TEM10 modes. We show the conservation of non-classical properties when the threshold is crossed. The experiment is made possible by the implementation of a new method to lock the relative phase of the pump and the injected beam. (11dB) have been recently observed below threshold [6]. Experimental results are less spectacular above threshold, because of the detrimental effect of the pump beam excess noise. Generally speaking, the non-classical properties increase when one approaches from below or from above the oscillation threshold, or any other bifurcation point of the non-linear dynamics of the device [7,8], but it is not always the case: for instance the signal-idler intensity difference squeezing is independent of the pumping level. This property of "non-critially squeezed light" has been further explored by the Valencia group[10] in the context of quantum imaging, which has found other squeezing effects that are independent of the pumping level. These effects are related to spatial symmetry-breaking, either translational[9] or rotational[10]: in a cavity of cylindrical symmetry, the parametric gain is the same for Gaussian modes TEM 01 where the two lobes are aligned along any direction in the transverse plane. However, above the oscillation threshold, a unique TEM 01 mode is produced. It is shown that this spontaneous symmetry breaking "induces" the generation of a squeezed vacuum state in the mode orthogonal to the emitted one with a squeezed value independent of the pumping level and clamped to its value at threshold. The emitted field is thus a two-mode non-classical field, made of the superposition of a bright mode and a vacuum-squeezed mode.In this paper, we show theoretically that this important result can be generalized to a much wider class of situations, involving either spatial or temporal modes, and we check experimentally that one can efficiently produce in this way multimode non-classical light.Let us envision the situation in which the cavity of the OPO is simultaneously resonant on several modes, which can be either spatial modes (Hermite-Gauss modes or more complicated patterns in transverse degenerate cavities), or frequency modes (separated by the free spectral range of the cavity). The annihilation operatorsâ ℓ associated with these different modes and the pump mode operatorb obey then the following well-known evolution equations, describing the effect of the parametric splitting of pump photons into couples of signal and idler photons respectively in modes ℓ and ℓ