profile of these structures is explicitly shown in Figure S1 in the Supporting Information, where the spectral and spatial field intensity distribution along the same DBR on different substrates (aluminum and glass) is shown. At variance with surface plasmons, Tamm states can couple directly to free-space propagating photon modes. Hence, if an emitter is placed in the vicinity of the DBR-metal interface, its emission may be efficiently channeled through far-field radiative modes, a significant enhancement of the emission intensity and control over its directionality being at reach. Experimental verification of this effect has been attained by analyzing ensembles of thin metallic patches or layers deposited onto dielectric multilayers, and the versatility and technological potential of this approach repeatedly demonstrated. [14][15][16][17] In most cases in which emission is channeled through optical Tamm states, the layer of emitters is in direct contact with the inner or outer surface of the metal film, hence favoring nonradiative decay of electrons from the excited states.Herein, we demonstrate a design that optimizes the photoluminescence (PL) intensity radiated by a DBR-metal ensemble embedding a single layer of dyed nanospheres. The nanoemitters, which occupy an area of the order of squared centimeters, are located at a predetermined depth within the last layer of the DBR, the one closer to the metal. We follow a design that results from a theoretical optimization procedure that accounts for the effect of optical Tamm states on the PL quantum yield (QY) and outcoupling efficiency in order to attain the maximum luminous power from the outer surface of the DBR. In this way we demonstrate the possibility of controlling the spectrum, directionality, and dynamics of the emission. Self-standing and flexible DBRs embedding the nanoemitters are used as conformably adaptable light-emitting coatings onto metal surfaces of arbitrary composition and curvature. The versatility of this approach is shown by building spectrally narrow perpendicularly emitting flat surfaces and curved ones from which all the emitted light converges in a well-defined focus. For the wavelength range for which outcoupling is optimized, 50% of the total light emitted from the DBR-metal ensembles is extracted within a narrow cone of numerical aperture (NA = 0.2), which implies a 10-fold extracted power enhancement with respect to a similar layer of emitters embedded in an optically homogeneous matrix. Furthermore, a QY of around 50% is estimated from PL decay rate measurements, which implies a 2-fold enhancement with respect to that observed from a dilute suspension of the same emitting spheres.This study demonstrates a design that maximizes the power radiated into free space from a monolayer of nanoemitters embedded in a flexible distributed Bragg reflector conformably attached to a metal surface. This is achieved by positioning the light source at the precise depth within the multilayer for which optical Tamm states provide enhanced quantum yi...