Representation of symmetry transformations on the sets of tripotents of
spin and Cartan factors
- URL: http://arxiv.org/abs/2101.00670v2
- Date: Sun, 31 Oct 2021 17:10:00 GMT
- Title: Representation of symmetry transformations on the sets of tripotents of
spin and Cartan factors
- Authors: Yaakov Friedman, Antonio M. Peralta
- Abstract summary: We prove that in order that the description of the spin will be relativistic, it is not enough to preserve the projection lattice equipped with its natural partial order and denoteity.
This, in particular, extends a result of Moln'ar to the wider setting of atomic JBW$*$-triples not containing rank-one Cartan factors.
- Score: 0.0
- License: http://creativecommons.org/licenses/by-nc-nd/4.0/
- Abstract: There are six different mathematical formulations of the symmetry group in
quantum mechanics, among them the set of pure states $\mathbf{P}$ -- i.e., the
set of one-dimensional projections on a complex Hilbert space $H$ -- and the
orthomodular lattice $\mathbf{L}$ of closed subspaces of $H$. These six groups
are isomorphic when the dimension of $H$ is $\geq 3$. Despite of the
difficulties caused by $M_2(\mathbb{C})$, rank two algebras are used for
quantum mechanics description of the spin state of spin-$\frac12$ particles,
there is a counterexample for Uhlhorn's version of Wigner's theorem for such
state space.
In this note we prove that in order that the description of the spin will be
relativistic, it is not enough to preserve the projection lattice equipped with
its natural partial order and orthogonality, but we also need to preserve the
partial order set of all tripotents and orthogonality among them (a set which
strictly enlarges the lattice of projections). Concretely, let $M$ and $N$ be
two atomic JBW$^*$-triples not containing rank-one Cartan factors, and let
$\mathcal{U} (M)$ and $\mathcal{U} (N)$ denote the set of all tripotents in $M$
and $N$, respectively. We show that each bijection $\Phi: \mathcal{U} (M)\to
\mathcal{U} (N)$, preserving the partial ordering in both directions,
orthogonality in one direction and satisfying some mild continuity hypothesis
can be extended to a real linear triple automorphism. This, in particular,
extends a result of Moln{\'a}r to the wider setting of atomic JBW$^*$-triples
not containing rank-one Cartan factors, and provides new models to present
quantum behavior.
Related papers
- Irreversible Diagonalization of Mechanical Quantities and the EPR Paradox [2.742138546345534]
Closure relation of quantum mechanical projection operators is not entirely true; it can be strictly falsified under unitary transformations in Fock states.
The angular momentum $J_x$, $J_y$ and $J_z$ are simultaneously diagonalized under the orthonormal set $|phi_nrangle$ of continuous rotation transformations in Fock states.
arXiv Detail & Related papers (2024-09-20T14:26:12Z) - Geometry of degenerate quantum states, configurations of $m$-planes and invariants on complex Grassmannians [55.2480439325792]
We show how to reduce the geometry of degenerate states to the non-abelian connection $A$.
We find independent invariants associated with each triple of subspaces.
Some of them generalize the Berry-Pancharatnam phase, and some do not have analogues for 1-dimensional subspaces.
arXiv Detail & Related papers (2024-04-04T06:39:28Z) - Quantum charges of harmonic oscillators [55.2480439325792]
We show that the energy eigenfunctions $psi_n$ with $nge 1$ are complex coordinates on orbifolds $mathbbR2/mathbbZ_n$.
We also discuss "antioscillators" with opposite quantum charges and the same positive energy.
arXiv Detail & Related papers (2024-04-02T09:16:18Z) - Quantum Current and Holographic Categorical Symmetry [62.07387569558919]
A quantum current is defined as symmetric operators that can transport symmetry charges over an arbitrary long distance.
The condition for quantum currents to be superconducting is also specified, which corresponds to condensation of anyons in one higher dimension.
arXiv Detail & Related papers (2023-05-22T11:00:25Z) - DHR bimodules of quasi-local algebras and symmetric quantum cellular
automata [0.0]
We show that for the double spin flip action $mathbbZ/2mathbbZtimes mathbbZ/2mathbbZZcurvearrowright mathbbC2otimes mathbbC2$, the group of symmetric QCA modulo symmetric finite depth circuits in 1D contains a copy of $S_3$, hence is non-abelian.
arXiv Detail & Related papers (2023-03-31T18:33:07Z) - Complete crystalline topological invariants from partial rotations in
(2+1)D invertible fermionic states and Hofstadter's butterfly [6.846670002217106]
We show how to extract many-body invariants $Theta_textopm$, where $texto$ is a high symmetry point, from partial rotations in (2+1)D invertible fermionic states.
Our results apply in the presence of magnetic field and Chern number $C neq 0$, in contrast to previous work.
arXiv Detail & Related papers (2023-03-29T18:00:00Z) - Quantized charge polarization as a many-body invariant in (2+1)D
crystalline topological states and Hofstadter butterflies [14.084478426185266]
We show how to define a quantized many-body charge polarization $vecmathscrP$ for (2+1)D topological phases of matter, even in the presence of non-zero Chern number and magnetic field.
We derive colored Hofstadter butterflies, corresponding to the quantized value of $vecmathscrP$, which further refine the colored butterflies from the Chern number and discrete shift.
arXiv Detail & Related papers (2022-11-16T19:00:00Z) - Beyond the Berry Phase: Extrinsic Geometry of Quantum States [77.34726150561087]
We show how all properties of a quantum manifold of states are fully described by a gauge-invariant Bargmann.
We show how our results have immediate applications to the modern theory of polarization.
arXiv Detail & Related papers (2022-05-30T18:01:34Z) - Uncertainties in Quantum Measurements: A Quantum Tomography [52.77024349608834]
The observables associated with a quantum system $S$ form a non-commutative algebra $mathcal A_S$.
It is assumed that a density matrix $rho$ can be determined from the expectation values of observables.
Abelian algebras do not have inner automorphisms, so the measurement apparatus can determine mean values of observables.
arXiv Detail & Related papers (2021-12-14T16:29:53Z) - Construction of a new three boson non-hermitian Hamiltonian associated
to deformed Higgs algebra: real eigenvalues and Partial PT-symmetry [0.0]
Fusion of Jordan-Schwinger realization of complexified $mathfraksu(2)$ with Dyson-Maleev representation.
Non-hermitian Hamiltonian has real eigenvalues and eigensymmetry inducedity.
arXiv Detail & Related papers (2021-11-07T06:40:47Z) - Fermion and meson mass generation in non-Hermitian Nambu--Jona-Lasinio
models [77.34726150561087]
We investigate the effects of non-Hermiticity on interacting fermionic systems.
We do this by including non-Hermitian bilinear terms into the 3+1 dimensional Nambu--Jona-Lasinio (NJL) model.
arXiv Detail & Related papers (2021-02-02T13:56:11Z)
This list is automatically generated from the titles and abstracts of the papers in this site.
This site does not guarantee the quality of this site (including all information) and is not responsible for any consequences.