Quasielastic incoherent neutron scattering (QENS) is an important tool for the exploration of the dynamics of complex systems such as biomolecules, liquids, and glasses. The dynamics is reflected in the energy spectra of the scattered neutrons. Conventionally these spectra are decomposed into a narrow elastic line and a broad quasielastic band. The band is interpreted as being caused by Doppler broadening due to spatial motion of the target molecules. We propose a quantum-mechanical model in which there is no separate elastic line. The quasielastic band is composed of sharp lines with twice the natural line width, shifted from the center by a random walk of the protein in the free-energy landscape of the target molecule. The walk is driven by vibrations and by external fluctuations. We first explore the model with the Mössbauer effect. In the subsequent application to QENS we treat the incoming neutron as a de Broglie wave packet. While the wave packet passes the protons in the protein and the hydration shell it exchanges energy with the protein during the passage time of about 100 ns. The energy exchange broadens the ensemble spectrum. Because the exchange involves the free-energy landscape of the protein, the QENS not only provides insight into the protein dynamics, but it may also illuminate the free-energy landscape of the protein-solvent system. quasielastic neutron scattering | neutron wave packet | protein free-energy landscape Q uasielastic effects are a key to understanding the dynamics of complex systems, from water to proteins (1, 2). A novice trying to understand quasielastic incoherent neutron scattering (QENS) is easily mystified. "Quasielastic" is usually taken to mean broadening of the elastic line due to spatial diffusion of the scattering particle. This definition is vague. We introduce a model that permits an unambiguous definition. It describes the QENS of proteins as involving a random walk in the free-energy landscape (FEL), driven by external fluctuations and by thermal vibrations. During the walk, the neutrons exchange energy with the protein, thus broadening the energy spectrum.In QENS the energy spectrum I(ΔE) of the scattered neutrons is measured as a function of the energy transfer ΔE relative to the energy of the elastic line at ΔE = 0. At present the QENS spectra are separated into a narrow elastic peak and a broad quasielastic band shown schematically in Fig. 1A. The band is taken to consist of broad Lorentzians with width Γ h centered at ΔE = 0 as sketched in Fig. 1B. The broadening is attributed to spatial motion of the target atoms, for instance by continuous diffusion, by jumps from one lattice site to another, or by conformational changes in proteins. The motions lead to different width Γ h for different proteins. We call this model SMM, for "spatial motion model," and discuss it in more detail later. We have introduced a radically different model, ELM, for "energy landscape model" (3). In the ELM, there is no separate elastic line pinned to the center. The entire spectrum is ...