We study the continuous time dynamics of the Thermal Minority Game. We find that the dynamical equations of the model reduce to a set of stochastic differential equations for an interacting disordered system with non-trivial random diffusion. This is the simplest microscopic description which accounts for all the features of the system. Within this framework, we study the phase structure of the model and find that its macroscopic properties strongly depend on the initial conditions.Many of the current challenges for statistical physics have their origins in problems in biology [1] and economics [2,3]. In particular, the application of ideas and techniques of the statistical mechanics of disordered systems can prove useful in the study of systems of adaptive and competitive agents, which are relevant, for example, to the microscopic modeling of financial markets; and, conversely, such problems can raise new issues for statistical physics. One of these systems is the minority game (MG) [4,5], a simple model based on Arthur's "El Farol" bar problem [6] which describes the behaviour of a group of competing heterogeneous agents subject to the economic law of supply and demand. Despite its simplicity, the MG is very non-trivial, and although much progress has been made in the qualitative [7][8][9] and quantitative [10,11] understanding of its features, a full analytic solution of the MG is still missing.The main hurdles in the way of an analytical study of the MG in its original formulation were its non-locality in time due to the dependence on the game history, its discrete kinematics and dynamics, and the "best-strategy" rule (see, however, [10]). The first of these obstacles was overcome in [12], where it was shown numerically that the macroscopic behaviour of the MG was unchanged if the real history was replaced by a random one. This allowed the study of a simpler stochastic Markovian problem instead of the original deterministic non-Markovian one.In [13] a natural continuous generalization of the MG was presented. The "information" to which the agents reacted was taken as an external input to the system and it was shown that all the macroscopic features of the MG were preserved, as long as the external information was ergodic in time, the simplest choice being just noise. To handle the problem of the 'best-strategy' rule, the Thermal Minority Game (TMG) was introduced, in which a certain degree of stochasticity in the choice of the strategies by the agents was allowed, controlled by a parameter T , the "temperature", the limits T = 0 and T = ∞ corresponding to the original deterministic MG and the case of completely random strategy choices, respectively. The TMG displayed extra non-trivial structure as a function of T , notably that in the region where the MG performs worse than random, the system can be made to perform better than random by allowing a certain degree of individual stochastic error.In the present paper we carefully study the continuous time limit of the TMG, in order to obtain the simplest microsc...