TL;DR: In this paper, a new approach to the model-independent description of quantum field theories is introduced, which incorporates in a local sense the principle of general covariance of general relativity, thus giving rise to the concept of a locally covariant quantum field theory.
Abstract: A new approach to the model-independent description of quantum field theories will be introduced in the present work. The main feature of this new approach is to incorporate in a local sense the principle of general covariance of general relativity, thus giving rise to the concept of a locally covariant quantum field theory. Such locally covariant quantum field theories will be described mathematically in terms of covariant functors between the categories, on one side, of globally hyperbolic spacetimes with isometric embeddings as morphisms and, on the other side, of *-algebras with unital injective *-monomorphisms as morphisms. Moreover, locally covariant quantum fields can be described in this framework as natural transformations between certain functors. The usual Haag-Kastler framework of nets of operator-algebras over a fixed spacetime background-manifold, together with covariant automorphic actions of the isometry-group of the background spacetime, can be re-gained from this new approach as a special case. Examples of this new approach are also outlined. In case that a locally covariant quantum field theory obeys the time-slice axiom, one can naturally associate to it certain automorphic actions, called ``relative Cauchy-evolutions'', which describe the dynamical reaction of the quantum field theory to a local change of spacetime background metrics. The functional derivative of a relative Cauchy-evolution with respect to the spacetime metric is found to be a divergence-free quantity which has, as will be demonstrated in an example, the significance of an energy-momentum tensor (up to addition of scalar functions) for the locally covariant quantum field theory. Furthermore, we discuss the functorial properties of state spaces of locally covariant quantum field theories that entail the validity of the principle of local definiteness.
TL;DR: A single free spin- 1 / 2 particle is considered and the reduced density matrix for its spin is not covariant under Lorentz transformations and the spin entropy is not a relativistic scalar and has no invariant meaning.
Abstract: We consider a single free spin- $\frac{1}{2}$ particle. The reduced density matrix for its spin is not covariant under Lorentz transformations. The spin entropy is not a relativistic scalar and has no invariant meaning.
TL;DR: In this article, it was shown that a Lorentz covariant coordinate system can be chosen in the case of the Kerr-Schild geometry which leads to the vanishing of the pseudo energy-momentum tensor and hence to the linearity of the Einstein equations.
Abstract: It is shown that a Lorentz covariant coordinate system can be chosen in the case of the Kerr–Schild geometry which leads to the vanishing of the pseudo energy–momentum tensor and hence to the linearity of the Einstein equations. The retarded time and the retarded distance are introduced and the Lienard–Wiechert potentials are generalized to gravitation in the case of world‐line singularities to derive solutions of the type of Bonnor and Vaidya. An accelerated version of the de Sitter metric is also obtained. Because of the linearity, complex translations can be performed on these solutions, resulting in a special relativistic version of the Trautman–Newman technique and Lorentz covariant solutions for spinning systems can be derived, including a new anisotropic interior metric that matches to the Kerr metric on an oblate spheroid.
TL;DR: In this paper, a new general relativity formulated on the Weitzenbock space-time has been proposed, which is invariant under a class of local Lorentz transformations.
Abstract: We make a short comment on our new general relativity formulated on the Weitzenb\"ock space-time. The new general relativity considered here has one free parameter besides the Einstein constant $\ensuremath{\kappa}$. The total action is invariant under a class of local Lorentz transformations, besides being invariant under general coordinate and global Lorentz transformations. The consequences of this "restricted local Lorentz invariance" are studied.
TL;DR: In this article, a Lagrangian density capable of giving the Lorentz form of the electromagnetic equations in the material coordinate system of elasticity theory for a moving, deforming body is derived.
Abstract: The Maxwell electromagnetic equations are obtained expressed in the material coordinate system of elasticity theory for a moving, deforming body. They are shown to be form-invariant to the deformation transformation. The transformation laws for the electric field, the electric displacement, the magnetic induction, the magnetic intensity, the charge density, the current density, the vector and scalar potentials, the polarization, and the magentization are found. The boundary conditions on the fields are derived in the material coordinate system and the simplicity of the derivation for moving, deforming bodies is emphasized. The boundary conditions are then transformed to the familiar spatial coordinate system. A Lagrangian density capable of giving the Lorentz form of the electromagnetic equations in the material coordinate system is found. The Lorentz form of the equations is shown not to be form-invariant to the deformation transformation.