We present a comprehensive theoretical framework for probing quantum entanglement in the decay angular distributions of a spin-
S particle-antiparticle pair
AAˉ, where each particle decays sequentially into a two-body final state,
A→B+C and
Aˉ→Bˉ+Cˉ, with
B(Bˉ) carrying spin
b and
C(Cˉ) being spinless. Starting from the most general polarized initial state, we derive the fully differential angular distribution
W(θ1,θ2,ϕ1,ϕ2) and identify observables
⟨cos(2S(ϕ1∓ϕ2))⟩ whose expectation values directly depend on the entanglement-sensitive coefficients
Re(α−S,∓SαS,±S∗) of the initial state. The proportionality factor
C(S,b) in these relations is computed explicitly. For bosonic decays (
b=0,1,2,…),
C(S,b) is universal and independent of decay dynamics; in particular,
C(S,0)=1/2 for any
S, and
C(1,1)=1/8, matching known results for
W+W− decays. For fermionic decays (
b=21,23,25…),
C(S,b) depends explicitly on the spin analysis powers
αA/Aˉ, making entanglement extraction more decay-dependent. We further demonstrate, within the context of
e+e−→γ∗→AAˉ production, how
αA/Aˉ can be determined experimentally using specific angular observables restricted to the beam-axis region. Our results highlight the special role of bosonic decays in providing clean, model-independent tests of quantum entanglement at colliders, while outlining a pathway for entanglement measurement in fermionic cases through supplementary polarization information.
These two accompanying papers treat two mode entanglement for systems of identical massive bosons and the relationship to spin squeezing and other quantum correlation effects. Entanglement is a key quantum feature of composite systems where the probabilities for joint measurements on the composite sub-systems are no longer determined from measurement probabilities on the separate sub-systems. We focus on the meaning of entanglement, the quantum paradoxes associated with entangled states, and important tests that allow an experimentalist to determine whether a quantum state - in particular, one for massive bosons is entangled. Our tests for entanglement fully utilise the symmetrisation principle and super-selection rules for bosonic massive particles. These papers provides detailed arguments necessary for the conclusions of a recent paper which presented results for rigorously demonstrating the entanglement of a two-mode Bose-Einstein condensate (BEC). In the first paper (I), we discuss the meaning of entanglement for systems of identical particles. For such systems, the relevant quantum density operators must satisfy the symmetrisation principle and global and local super-selection rules prohibiting states in which there are coherences between differing particle numbers. We fully justify these requirements. In the second quantisation approach, both the system and sub-systems are modes (or sets of modes) rather than particles, particles being associated with different mode occupancies. In the accompanying review paper (II), we consider spin squeezing and other tests for entanglement for two-mode bosonic systems. Starting from paper (I) we determine which tests are useful for detecting entanglement in massive bosonic (BEC), as opposed to photonic, systems. Several new inequalities are derived, and recent key experiments are analysed.
We construct a quantum information-centered approach to describe the experimentally observed behavior of hyperon spin-pair correlations in high-energy collider experiments. The evolution of the spin density matrix of the hyperon pair is treated in the language of quantum channels, accounting both for the spin dynamics in
C2⊗C2 and for the pair's angular separation
ΔR. We show that the experimental data are consistent with an evolution under a two-qubit depolarizing channel, from which a Lindblad master equation is derived. This provides an open quantum system picture of spin dynamics during the hadronization transition, which is not naturally captured by other quantum channels, and we discuss its microscopic origins. These results show that quantum information science can offer new insights into confinement dynamics beyond the classification of entanglement in the final particle states.
Bell-type experiments that test correlated observables typically involve measurements of spin or polarization on multi-particle systems in singlet states. These observables are all non-commuting and satisfy an uncertainty relation. Theoretically, the non-commuting nature should be independent of whether the singlet state consists of multiple particles or a single particle. In addition, if Bell-type inequalities can be found for experiments involving spin and polarization, the same should be true for experiments involving other non-commuting observables such as position and momentum. In fact the original EPR paper used position and momentum, though in a different experimental situation. As such, an experiment is proposed to measure (quantum mechanically) position and momentum for a single oscillator as a means for deriving a Bell-type inequality for these correlated observables. The experiment, if realizable, would shed light on the basic nature of matter, perhaps pointing to some form of self-entanglement, and would also help to further elucidate a possible mechanism behind the Heisenberg uncertainty principle. Violation of these inequalities would, in fact, offer yet another confirmation of the principle.
There have been numerous studies of entanglement in spin systems. These have usually focused on examining the entanglement between individual spins or determining whether the state of the system is completely separable. Here, we present conditions that allow us to determine whether blocks of spins are entangled. We show that sometimes these conditions can detect entanglement better than conditions involving individual spins. We apply these conditions to study entanglement in spin-wave states, both when there are only a few magnons present and also at finite temperature.
An analysis is presented of the state that arises after photons have been spontaneously emitted by a pair of spatially separated excited two-level atoms with spin-1/2 ground and excited states. Selection of possible decay scenarios conditioned on the helicities of the photons (even on the helicity of the one emitted first) makes it possible to reveal ground-state spin-projection correlations between atoms. The correlations are due to quantum interference between alternative scenarios (the atom that has emitted a particular photon cannot be identified). The correlations obtained by the chosen selection method are classical.