Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

American Journal of Physics

Double-group theory on the half-shell and the two-level system. I. Rotation and half-integral spin states

William G. Harter, Narciso dos Santos

Published Mar 1, 1978• 15 citations
Publisher

Abstract

A geometrical construction by Hamilton is used to simplify the quantum mechanics of half-integral spin. A slide rule is described which can be used to (a) compute products of half-integral or integral spin rotation operators, (b) convert between the Euler-angle and ’’axis-angle’’ rotation operator parameters, and (c) calculate the time evolution of a spin-1/2 state for a constant Hamiltonian operator. A type of nomogram is developed which suggests ways to simplify the ’’double-group’’ theory of half-integral spin in molecular point symmetry, as well as the ’’ordinary’’ group theory for integral spin systems. Cubic and icosahedral symmetry group characters are derived for half-integral spin operators.

DOI
10.1119/1.11134

Related papers

Statistical approach to quantum mechanics II: Nonrelativistic spin

G. H. Goedecke

In this second paper in a series, we show that the the general statistical approach to nonrelativistic quantum mechanics developed in the first paper yields a representation of quantum spin and magnetic moments based on classical nonrelativistic spinning top models, using Euler angle coordinates. The models allow half-odd-integer spin and predict supraluminal speeds only for electrons and other leptons, which must be treated relativistically. The spin operators in the space-fixed frame satisfy the usual commutation rules, while those in the rotating body-fixed frame satisfy "left-handed" rules. The commutation rules are independent of the structure of the top, so all nonrelativistic rigidly rotating objects must have integer or odd-half-integer spin. Physical boundary conditions restrict all mixed spin states to involve only half-odd-integer or only integer spin eigenstates. For spin 1/2, the theory automatically yields a modified Pauli-Schrödinger equation. The Hamiltonian operator in this equation contains a rigid rotator term and a term involving the square of the magmetic field, as well as an interaction term having the usual form in spherically symmetric and some cylindrically symmetric models, valid for any magnetogyric ratio.

arXiv:1408.1721•Aug 7, 2014•0 citations

Particle Spin and Rotation

N. Rosen

It is proposed to treat the spin of a particle phenomenologically by considering the particle as a small rotating sphere, the rotation of which is described by euler parameters. If the rotation is quantized in the space of the euler parameters, one obtains both integral and half-integral values for the spin. In this way one arrives at a formalism in which the spin components can be represented as differential operators in the Schroedinger representation.

Physical Review•Jun 1, 1951•26 citations

Quantum theory of molecular orientation

Victor V. Albert, Eric Kubischta, Mikhail Lemeshko +1 more

We formulate a quantum phase space for rotational and nuclear-spin states of rigid molecules. For each nuclear spin isomer, we re-derive the isomer's admissible angular momentum states from molecular geometry and nuclear-spin data, introduce its angular position states using quantization theory, and develop a generalized Fourier transform converting between the two. We classify molecules into three types -- asymmetric, rotationally symmetric, and perrotationally symmetric -- with the last type having no macroscopic analogue due to nuclear-spin statistics constraints. We discuss two general features in perrotationally symmetric state spaces that are Hamiltonian-independent and induced solely by symmetry and spin statistics. First, we quantify when and how an isomer's state space is completely rotation-spin entangled, meaning that it does not admit any separable states. Second, we identify isomers whose position states house an internal pseudo-spin or "fiber" degree of freedom, and the fiber's Berry phase or matrix after adiabatic changes in position yields naturally robust operations, akin to braiding anyonic quasiparticles or realizing fault-tolerant quantum gates. We outline how the fiber can be used as a quantum error-correcting code and discuss scenarios where these features can be experimentally probed

arXiv:2403.04572•Mar 7, 2024•0 citations

Symmetry properties of exciton states in one-dimensional systems

Douglas B. Abraham, Alan McLachlan

We discuss a cyclic chain of N identical sites, each with two possible quantum states, whose Hamiltonian may be written in terms of the spin operators for N spins S = 1/2, and transformed into the Fermi site excitation representation. We show that in the Fermion wave representation the requirement that the states transform according to irreducible representations of the translational symmetry group demands that the quasiparticle momenta are drawn from the representations of the double group. They must be all integral or all half-integral when the number of quasiparticles is odd or even respectively. The requirement that a quantum-mechanical operator has a definite symmetry type leads to very complicated conditions unless the operator conserves the odd or even particle number. If it does the symmetry operator can be defined in terms of Fermi wave operators and projection operators. The time reversal transformation is developed in detail and applied to problems of degeneracy in McConnell's model of singlet excitons and in the anisotropic transverse Heisenberg antiferromagnet. In the Bogoliubov-Valatin transformation time reversal shifts the quasiparticle momenta by ± π, converting integral into half-integral momenta when N is odd. The energies of the excited states are doubly-periodic functions of the momentum.

Molecular Physics•Jan 1, 1967•10 citations

Eine Lösungstheorie für Mehrteilchensysteme mit Spin

H. Näpfel

A system of interacting particles is treated by the methods of quantum mechanics. Among the variables the three Euler angles are introduced which give the orientation of the system as a whole in an inertial frame of reference. This allows an expansion of the Schrödinger eigenfunctions in terms of elements of irreducible representations of the rotation group. This method, originally suggested by Wigner, is extended to include particles with spin. Two and three particle systems, one particle having spin 1/2, the rest being spinless, are treated explicitly. If the two spinless particles are regarded as the core of a nucleus, the spin 1/2 particle as an extra nucleon, one can compare this “three particle nuclear model” with other nuclear models. It permits calculations of Nilsson diagrams and, compared with other models, a more straightforward adjustment of parameters to empirical data.

Zeitschrift für Naturforschung A•Apr 1, 1968•0 citations

MERLIN SCIENCE — The Double Cover: Unifying Quantum Spin and Classical Rotation — E8 Intelligence Research

Andrew Stewart Caldin

Here is the narration for the MERLIN SCIENCE video. --- Today, we're talking about a structural bridge, not new physics. The finding is this: the SU(2) double-cover of SO(3) is the mathematical hinge that lets quantum spin and classical rotation coexist, and the Bloch sphere is where that hinge lives in plain sight. For the working scientist, here's the context. You know that a 360-degree rotation in space brings an object back to itself. But for a spin-1/2 particle, you need 720 degrees. That's not a quirk; it's the double cover. SU(2) is topologically a three-sphere, and SO(3) is that sphere with antipodal points identified. The map between them sends a rotation by angle theta in SO(3) to a rotation by theta over two in SU(2). That half-angle is not an approximation. It's exact. Now, the mechanism. On the Bloch sphere, the state is parameterized by theta over two, not theta. That same half-angle appears in the icosahedral group. The icosahedron's rotational symmetries live in SO( Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

•Sep 8, 2026•0 citations
A geometrical construction by Hamilton is used to simplify the quantum mechanics of half-integral spin. A slide rule is described which can be used to (a) compute products of half-integral or integral spin rotation operators, (b) convert between the Euler-angle and ’’axis-angle’’ rotation operator parameters, and (c) calculate the time evolution of a spin-1/2 state for a constant Hamiltonian operator. A type of nomogram is developed which suggests ways to simplify the ’’double-group’’ theory of half-integral spin in molecular point symmetry, as well as the ’’ordinary’’ group theory for integral spin systems. Cubic and icosahedral symmetry group characters are derived for half-integral spin operators.
In this second paper in a series, we show that the the general statistical approach to nonrelativistic quantum mechanics developed in the first paper yields a representation of quantum spin and magnetic moments based on classical nonrelativistic spinning top models, using Euler angle coordinates. The models allow half-odd-integer spin and predict supraluminal speeds only for electrons and other leptons, which must be treated relativistically. The spin operators in the space-fixed frame satisfy the usual commutation rules, while those in the rotating body-fixed frame satisfy "left-handed" rules. The commutation rules are independent of the structure of the top, so all nonrelativistic rigidly rotating objects must have integer or odd-half-integer spin. Physical boundary conditions restrict all mixed spin states to involve only half-odd-integer or only integer spin eigenstates. For spin 1/2, the theory automatically yields a modified Pauli-Schrödinger equation. The Hamiltonian operator in this equation contains a rigid rotator term and a term involving the square of the magmetic field, as well as an interaction term having the usual form in spherically symmetric and some cylindrically symmetric models, valid for any magnetogyric ratio.
We formulate a quantum phase space for rotational and nuclear-spin states of rigid molecules. For each nuclear spin isomer, we re-derive the isomer's admissible angular momentum states from molecular geometry and nuclear-spin data, introduce its angular position states using quantization theory, and develop a generalized Fourier transform converting between the two. We classify molecules into three types -- asymmetric, rotationally symmetric, and perrotationally symmetric -- with the last type having no macroscopic analogue due to nuclear-spin statistics constraints. We discuss two general features in perrotationally symmetric state spaces that are Hamiltonian-independent and induced solely by symmetry and spin statistics. First, we quantify when and how an isomer's state space is completely rotation-spin entangled, meaning that it does not admit any separable states. Second, we identify isomers whose position states house an internal pseudo-spin or "fiber" degree of freedom, and the fiber's Berry phase or matrix after adiabatic changes in position yields naturally robust operations, akin to braiding anyonic quasiparticles or realizing fault-tolerant quantum gates. We outline how the fiber can be used as a quantum error-correcting code and discuss scenarios where these features can be experimentally probed
We discuss a cyclic chain of N identical sites, each with two possible quantum states, whose Hamiltonian may be written in terms of the spin operators for N spins S = 1/2, and transformed into the Fermi site excitation representation. We show that in the Fermion wave representation the requirement that the states transform according to irreducible representations of the translational symmetry group demands that the quasiparticle momenta are drawn from the representations of the double group. They must be all integral or all half-integral when the number of quasiparticles is odd or even respectively. The requirement that a quantum-mechanical operator has a definite symmetry type leads to very complicated conditions unless the operator conserves the odd or even particle number. If it does the symmetry operator can be defined in terms of Fermi wave operators and projection operators. The time reversal transformation is developed in detail and applied to problems of degeneracy in McConnell's model of singlet excitons and in the anisotropic transverse Heisenberg antiferromagnet. In the Bogoliubov-Valatin transformation time reversal shifts the quasiparticle momenta by ± π, converting integral into half-integral momenta when N is odd. The energies of the excited states are doubly-periodic functions of the momentum.
A system of interacting particles is treated by the methods of quantum mechanics. Among the variables the three Euler angles are introduced which give the orientation of the system as a whole in an inertial frame of reference. This allows an expansion of the Schrödinger eigenfunctions in terms of elements of irreducible representations of the rotation group. This method, originally suggested by Wigner, is extended to include particles with spin. Two and three particle systems, one particle having spin 1/2, the rest being spinless, are treated explicitly. If the two spinless particles are regarded as the core of a nucleus, the spin 1/2 particle as an extra nucleon, one can compare this “three particle nuclear model” with other nuclear models. It permits calculations of Nilsson diagrams and, compared with other models, a more straightforward adjustment of parameters to empirical data.
Here is the narration for the MERLIN SCIENCE video. --- Today, we're talking about a structural bridge, not new physics. The finding is this: the SU(2) double-cover of SO(3) is the mathematical hinge that lets quantum spin and classical rotation coexist, and the Bloch sphere is where that hinge lives in plain sight. For the working scientist, here's the context. You know that a 360-degree rotation in space brings an object back to itself. But for a spin-1/2 particle, you need 720 degrees. That's not a quirk; it's the double cover. SU(2) is topologically a three-sphere, and SO(3) is that sphere with antipodal points identified. The map between them sends a rotation by angle theta in SO(3) to a rotation by theta over two in SU(2). That half-angle is not an approximation. It's exact. Now, the mechanism. On the Bloch sphere, the state is parameterized by theta over two, not theta. That same half-angle appears in the icosahedral group. The icosahedron's rotational symmetries live in SO( Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com