Solid-state electrothermal energy interconversion utilising the electrocaloric effect is currently being considered as a viable source of applications alternative to contemporary cooling and heating technologies. Electrocaloric performance of a dielectric system is critically dependent on the number of uncorrelated polar states, or 'entropy channels' present within the system phase space. Exact physical origins of these states are currently unclear and practical methodologies for controlling their number and creating additional ones are not firmly established. Here we employ a multiscale computational approach to investigate the electrocaloric response of an artificial layered-oxide material that exhibits Goldstone-like polar excitations. We demonstrate that in the low-electric-field poling regime, the number of independent polar states in this system is proportional to the number of grown layers, and that the resulting electrocaloric properties are tuneable in the whole range of temperatures below T C by application of electric fields and elastic strain. INTRODUCTION Electrocaloric (EC) effect is defined as the variation of the dielectric material entropy as a function of the electric field at a given temperature, which results in an adiabatic temperature change. Recently, there has been significant progress 1-3 in the development of polar (i.e., possessing spontaneous polarisation) dielectrics that display large EC temperature shifts ΔT under electric-field poling. These systems include a variety of ferroelectric ceramics, 4-6 polymers 7-10 and liquid crystals. 11 A few relaxor and antiferroelectric materials may exhibit negative EC effect, which is especially advantageous for solid-state refrigeration. 12 The best values of positive EC ΔT in modern nanoengineered materials range from 20 to 45 K, for electric-field sweeps ΔE ⩾ 500 kV/cm, 1-6,13,14 whereas negative EC ΔT remain below − 10 K for much smaller ΔE. [15][16][17][18] The magnitude of the EC ΔT is proportional to a logarithm of the number of possible polar states, or independent 'entropy channels' in the system. 3,19 Therefore, it is highly desirable to acquire precise understanding of physical phenomena underpinning the emergence of these states and develop practical methods for engineering additional entropy channels into dielectrics. Moreover, since entropic changes involving evolution of other ferroic order parameters can be cumulative with the EC effect, more advanced multicaloric materials concepts blending polar, magnetic and elastic energy-interconversion functionalities, are also being considered. [20][21][22][23][24] Here we use a multiscale computational approach that combines ab initio quantum mechanical simulations, phenomenological Landau theory and thermodynamical evaluations to investigate the EC response of a 'material template' based on a quasi-two-dimensional system that exhibits polar Goldstone-like [25][26][27] excitations. This template system is an 'n = 2' Ruddlesden-Popper (RP) type 28 PbSr 2 Ti 2 O 7 (PSTO) layered-oxide