Previous realizations of synthetic gauge fields for ultracold atoms do not allow the spatial profile of the field to evolve freely. We propose a scheme which overcomes this restriction by using the light in a multimode cavity, in conjunction with Raman coupling, to realize an artificial magnetic field which acts on a Bose-Einstein condensate of neutral atoms. We describe the evolution of such a system, and present the results of numerical simulations which show dynamical coupling between the effective field and the matter on which it acts. Crucially, the freedom of the spatial profile of the field is sufficient to realize a close analogue of the Meissner effect, where the magnetic field is expelled from the superfluid. This back-action of the atoms on the synthetic field distinguishes the Meissner-like effect described here from the Hess-Fairbank suppression of rotation in a neutral superfluid observed elsewhere.The Meissner effect [1] is the sine qua non of superconductivity [2]. As captured by the Ginzburg-Landau equations [3], the superfluid order parameter couples to the electromagnetic fields such that there is perfect diamagnetism. Physically this arises because the normal paramagnetic response of mater is completely suppressed by the phase stiffness of the superfluid, leaving only the diamagnetic current [4]. Magnetic field thus decays exponentially into the bulk [5]. Exponentially decaying fields are symptomatic of a massive field theory, and so can be seen as a direct consequence of the the Anderson-Higgs mechanism [6,7] giving the electromagnetic field a mass gap. Central to all these phenomena is that minimal coupling between the electromagnetic field and the superfluid modifies the equations of motion for both the superfluid and the electromagnetic field.The concept of "synthetic" gauge fields has attracted much attention over the last few years. In the context of ultracold atoms, realizations have included schemes based on dark states [8,9] or Raman driving [10][11][12], or inducing Peierls phases in lattice systems [13][14][15][16][17][18][19][20][21][22][23] (for a review, see [24][25][26][27]). There have also been proposals to realize gauge fields for photons, including "free space" realizations using Rydberg atoms in non-planar ring cavity geometries [28] as well as Peierls phases for photon hopping in coupled cavity arrays [29][30][31]. However, with a few exceptions, all these have involved static gauge fields-there is no feedback of the atoms (or photons) on the synthetic field. Thus, even in the pioneering demonstration of a Meissner phase of chiral currents [23], it is noted that these experiments are closer to the HessFairbank effect [32] (suppression of rotation in a neutral superfluid), and do not show expulsion of the synthetic field. In contrast, a charged superfluid acts back on the magnetic field.The synthetic field cannot be expelled in the above schemes because it is set by a fixed external laser or the system geometry. The exceptions are thus proposals where the strength of synth...