We analyze the breathing-mode oscillations of a harmonically quenched Tonks-Giradeau (TG) gas using an exact finite-temperature dynamical theory. We predict a striking collective manifestation of impenetrability-a collective many-body bounce effect. The effect, although being invisible in the evolution of the in situ density profile of the gas, can be revealed through a nontrivial periodic narrowing of its momentum distribution, taking place at twice the rate of the fundamental breathing-mode frequency. We identify physical regimes for observing the many-body bounce and construct the respective nonequilibrium phase diagram as a function of the quench strength and the initial temperature of the gas. We also develop a finite-temperature hydrodynamic theory of the TG gas wherein the many-body bounce is explained by an increased thermodynamic pressure during the isentropic compression cycle, which acts as a potential barrier for the particles to bounce off. DOI: 10.1103/PhysRevA.96.041605 Collective dynamics in many-body systems emerge as a result of interparticle interactions. Such dynamics can be characterized by a coherent or correlated behavior of the constituents, which cannot be predicted form the single-particle or noninteracting picture. Collective dynamics can therefore serve as an important probe of the underlying interactions and is at the heart of a variety of nonequilibrium phenomena in many-body physics, including the archetypical examples of superfluidity and superconductivity. Among physical systems of current theoretical and experimental interest for understanding nonequilibrium many-body dynamics are ultracold quantum gases [1-10], which offer a versatile platform for realizing minimally complex but highly controllable models of many-body theory.In quantum gases, the simplest manifestations of collective dynamics relate to the frequencies of monopole (breathingmode) and multipole oscillations in harmonic trapping potentials [5,[11][12][13][14][15][16][17][18][19][20][21]. These frequencies, depending on trap configurations, can vary significantly from those of ideal (noninteracting) gases. For example, in a weakly interacting one-dimensional (1D) Bose gas at sufficiently low temperatures, the breathing-mode oscillations of the in situ density occur at a frequency of ω B √ 3ω (where ω is the frequency of the trap) [5,18,19,[22][23][24][25][26][27][28], whereas in an ideal Bose gas the breathing-mode frequency is ω B = 2ω. An even more dramatic qualitative departure from the ideal gas behavior was observed recently in the dynamics of the momentum distribution of a weakly interacting 1D quasicondensate [5,28]: For sufficiently low temperatures, the momentum distribution was oscillating at a frequency of 2ω B , i.e., at twice the rate of the fundamental breathing-mode frequency of the in situ density profile ω B √ 3ω. Furthermore, at intermediate temperatures the oscillations could be decomposed as a weighted superposition of just two harmonics, one oscillating at 2ω B and the other at ω B .In a str...