Towards relativistic atomic physics. Part 1. The rest-frame instant form of dynamics and a canonical transformation for a system of charged particles plus the electro-magnetic field
Abstract:A complete exposition of the rest-frame instant form of dynamics for arbitrary isolated systems (particles, fields, strings, fluids) admitting a Lagrangian description is given. The starting point is the parametrized Minkowski theory describing the system in arbitrary admissible non-inertial frames in Minkowski space-time, which allows one to define the energy-momentum tensor of the system and to show the independence of the description from the clock synchronization convention and from the choice of the 3-coo… Show more
“…This allows us to define the rest-frame instant form of dynamics for arbitrary isolated systems: a complete exposition of all its properties has been done in Ref. [8] and extended to non-inertial rest frames in Ref. [9].…”
A new formulation of relativistic quantum mechanics is proposed in the framework of the restframe instant form of dynamics with its instantaneous Wigner 3-spaces and with its descrption of the particle world-lines by means of derived non-canonical predictive coordinates. In it we quantize the frozen Jacobi data of the non-local 3-center of mass and the Wigner-covariant relative variables in an abstract (frame-independent) internal space h1whose existence is implied by Wigner-covariance. The formalism takes care of the properties of both relativistic bound states and scattering ones. There is a natural solution to the relativistic localization problem. The non-relativistic limit leads to standard quantum mechanics but with a frozen Hamilton-Jacobi description of the center of mass. Due to the non-locality of the Poincare' generators the resulting theory of relativistic entanglement is both kinematically non-local and spatially non-separable, properties absent in the non-relativistic limit.
“…This allows us to define the rest-frame instant form of dynamics for arbitrary isolated systems: a complete exposition of all its properties has been done in Ref. [8] and extended to non-inertial rest frames in Ref. [9].…”
A new formulation of relativistic quantum mechanics is proposed in the framework of the restframe instant form of dynamics with its instantaneous Wigner 3-spaces and with its descrption of the particle world-lines by means of derived non-canonical predictive coordinates. In it we quantize the frozen Jacobi data of the non-local 3-center of mass and the Wigner-covariant relative variables in an abstract (frame-independent) internal space h1whose existence is implied by Wigner-covariance. The formalism takes care of the properties of both relativistic bound states and scattering ones. There is a natural solution to the relativistic localization problem. The non-relativistic limit leads to standard quantum mechanics but with a frozen Hamilton-Jacobi description of the center of mass. Due to the non-locality of the Poincare' generators the resulting theory of relativistic entanglement is both kinematically non-local and spatially non-separable, properties absent in the non-relativistic limit.
“…[28] it is shown that by using the previous results one can find a canonical transformation from the canonical basis η i (τ ), κ i (τ ), A ⊥ (τ, σ r ), π ⊥ (τ, σ r ), in which the internal Poincaré generators have the expression in the case N=2 (B = ∂ × A ⊥ , c(σ) = −1/4π |σ|)…”
Section: Relativistic Atomic Physicsmentioning
confidence: 81%
“…[26,28,29,33], the three collective variables can be expressed as known functions of the Lorentz-scalar rest time τ = c T s = h ·x = h · Y = h · R, of canonically conjugate Jacobi data (frozen Cauchy data) z = M c x N W (0) and h = P /M c 14 , of the invariant mass M c = √ ǫ P 2 of the system and of its rest spinS.…”
Section: The Instant Form Of Dynamics In the Inertial Rest Frames Andmentioning
confidence: 99%
“…B) The evolution equation for the four basic gauge variables θ i (τ, σ u ) and 3 K(τ, σ u ) (the equation for the York time is the Raychaudhuri equation 28 ): these equations determine the lapse and the shift functions once four gaugefixings for the basic gauge variables are given.…”
Section: -Orthogonal Schwinger Time Gauges and Hamilton Equationsmentioning
confidence: 99%
“…In the electro-magnetic case in SR [28] the regularized coupled secondorder equations of motion of the particles obtained by using the LienardWiechert solutions for the electro-magnetic field are independent by the type of Green function (retarded or advanced or symmetric) used. The electromagnetic retardation effects, killed by the Grassmann regularization, are connected with QED radiative corrections to the one-photon exchange diagram.…”
Section: Post-minkowskian Linearization In Non-harmonic 3-orthogonal mentioning
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