The kinetic energy operator is a mathematical representation used in quantum mechanics to describe the kinetic energy of a particle in a system. It is denoted as \\hat{T} and is often represented as \\hat{T} = -\\frac{\\hbar^2}{2m} \\nabla^2, where \\hbar is the reduced Planck's constant and m is the mass of the particle. This operator plays a crucial role in both the time-dependent and time-independent Schrödinger equations, which are foundational in describing how quantum systems evolve over time and how they behave at rest, respectively.