The spectral properties of interacting strongly chaotic systems are investigated for growing interaction strength. A very sensitive transition from Poisson statistics to that of random matrix theory is found. We introduce a new random matrix ensemble modeling this dynamical symmetry breaking transition which turns out to be universal and depends on a single scaling parameter only. Coupled kicked rotors, a dynamical systems paradigm for such transitions, are compared with this ensemble and excellent agreement is found for the nearest-neighbor-spacing distribution. It turns out that this transition is described quite accurately using perturbation theory.Quantization of fully chaotic systems is known to lead to the spectral fluctuations of random matrix theory (RMT) [1] and to exhibit energy level repulsion [2]. More generally, even non-integrable models without apparent classical limits, such as spin systems, can also show such features [3,4]. In contrast, integrable systems generally follow Poisson statistics, which are devoid of level repulsion [5]. It is also well understood that combining spectra of different irreducible representations tends toward Poisson statistics in the limit of superposing many sequences [6,7]. An instance where this occurs is for the spectra of two separable, but individually chaotic systems. Whereas each subsystem possesses RMT fluctuations, the full spectrum tends to Poisson fluctuations in the large dimensionality limit [8].This begs the question of what happens to spectral fluctuations if such separable, but quantum chaotic subsystems, interact. There are many motivations for studying such systems. For example, they may be of direct physical interest, such as conduction electrons in chaotic quantum dots interacting through a screened Coulomb potential [9]. Another motivation derives from quantum information theory where the development of entanglement is of particular importance [10]. Two quantum spin chains with RMT spectral fluctuations coupled in a ladder configuration is a many-body situation where such transitions are possible as well.Typically, the interaction between two subsystems leads to entanglement and paves the way for RMT fluctuations of the combined system. This Poisson-to-RMT transition can be viewed as a dynamical symmetry breaking in analogy to fundamental symmetry breaking; the first exact RMT solution to a symmetry breaking problem involved time-reversal invariance [11]. For modeling a particular dynamical system, it is important to connect dynamical system parameters with the abstract transi- There are a couple of other possible cases of a Poissonto-RMT transition, a metal-insulator transition where states transition from localized to extended [14], and the perturbation of an integrable dynamical system [12,15] that renders it chaotic for sufficient perturbation strength. In neither of these possibilities is there a simple globally coupled Poisson-to-RMT ensemble. Various complications, such as the metal-insulator transition, the KAM theorem regarding the surviv...