We study the relaxation mechanism of a highly excited charge carrier propagating in the antiferromagnetic background modeled by the t-J Hamiltonian on a square lattice. We show that the relaxation consists of two distinct stages. The initial ultrafast stage with the relaxation time τ ∼( /t0)(J/t0) −2/3 (where t0 is the hopping integral and J is the exchange interaction) is based on generation of string states in the close proximity of the carrier. This unusual scaling of τ is obtained by means of comparison of numerical results with a simplified t-Jz model on a Bethe lattice. In the subsequent (much slower) stage local antiferromagnetic excitations are carried away by magnons. The relaxation time on the two-leg ladder system is an order of magnitude longer due to the lack of string excitations. This further reinforces the importance of string excitations for the ultrafast relaxation in the two-dimensional system.In a large number of generic time-dependent manybody systems, it is conjectured that strong electronic correlations give rise to extremely fast timescales of relevant relaxation processes. In general, the nonequlibrium evolution of a simple quantum system is a complex problem with only a few exactly solvable cases, and strong interactions between charge carriers usually make the problem even harder. Although advanced numerical approaches give important information about nonequlibrium dynamics, this dynamics is in many cases too complex to be comprehended in terms of a simple physical picture. Distinguishing different elementary excitations in time domain therefore represents one of the major goals of the present research of nonequilibirum many-body systems. In this context, a rapid development of time-resolved experiments in condensed-matter systems [1][2][3][4][5][6][7] and cold atomic gases [8] provide both a challenge for theory as well as a testbed for new ideas. A large body of current theoretical research is based on studies of Hubbard-like models far from equilibrium, and it focuses both on relaxation dynamics after a sudden quench [9-13] and steadystate properties as a consequence of constant driving [14][15][16][17][18][19][20][21][22][23][24][25][26].Understanding the dynamics of photo-induced charge carriers in Mott insulators may contribute to unravelling still elusive mechanism of high-T C superconductivity, in addition, it is as well indispensable for applications of novel materials in future electronic and photovoltaic technologies. Many recent studies focused on dynamics of photo-induced carriers, i.e., doublons and holons [27][28][29][30][31][32][33][34][35][36][37][38], in particular on their nonradiative recombination process [37][38][39][40][41][42][43]. Experimentally, photo-induced carriers have been observed in, e.g., insulating cuprates, where they decay within a few hundreds of femtoseconds [44].In this manuscript, we investigate a phenomenon which precedes the recombination of photo-induced carriers, i.e., we consider a rapid exchange of energy between photo-induced carriers and...