Violation of (space) parity in atomic physics, molecular physics and chemistry is briefly reviewed. The review is structured by frequently asked questions related to the concept of space parity, its violation and the consequences thereof in physics, chemistry and biology. This article is categorized under: Theoretical and Physical Chemistry > Spectroscopy Structure and Mechanism > Molecular Structures Theoretical and Physical Chemistry > Thermochemistry K E Y W O R D S chirality, electroweak quantum chemistry, fundamental symmetries, parity violation, periodic system of fundamental particles, relativistic quantum chemistry 1 | WHAT IS (SPACE) PARITY?In mathematics, the concept of even and odd parity is related to integer numbers and their behavior under division by the number two. Those integers which can be divided by two without remainder are called even, those that are divided by two with remainder one are called odd. Consequently, one can speak of a given integer to possess either even parity or odd parity (see also Reference 1). In quantum mechanics, instead, the term parity is used for the transformation properties of states and operators with respect to discrete symmetry operations such as space inversion, time reversal or charge conjugation. Space inversion (in conventional three-dimensional space) implies reflection of spatial coordinates of all particles at the origin, time reversal implies reversal of all particle momenta and charge conjugation implies change from particles to their anti-particles and vice versa. States that remain unaltered under application of such a discrete symmetry operation are called space parity even (Peven) or charge parity even (C-even), respectively, those which change sign under application of these discrete symmetry operations are called space parity odd (P-odd) or charge parity odd (C-odd). Time reversal is special in this regard as the corresponding operator describing time reversal is an antiunitary operator which does not have eigenvalues. In contrast to states, operators can be classified as being time parity even (T-even) or time parity odd (T-odd) (see Reference 2 for a more detailed discussion of time-reversal symmetry). When no additional classification is given, the word parity conventionally refers to space parity, and we will use that convention also within this review.An arbitrary quantum state does not necessarily have to possess well-defined parity (P-even or P-odd), but in linear quantum mechanics instead, such a quantum state can be written as a superposition of states with well-defined parity.Elementary particles as quanta of fields are usually described with the help of so-called intrinsic parities (see e.g., Reference 3). One characterizes these fields for instance as scalar fields and vector fields or pseudo-scalar fields and pseudo-scalar fields and vector fields, depending on their behavior with respect to space inversion. Scalar fields and pseudo-vector fields remain