In quantum mechanics, a singlet originally meant a linked set of particles whose net angular momentum is zero, that is, whose overall spin quantum number , though this meaning has since been generalized to include other situations. The link between the particles may be historical, such as two widely separated particles whose current angular momentum states originated in a single quantum event; or ongoing, such as two particles bound by charge. A set of linked particles that lacks net angular momentum is said to be in a singlet state.
Singlets and the related spin concepts of doublets and triplets occur frequently in atomic physics and nuclear physics, where one often needs to determine the the total spin of a collection of particles. Since the only fundamental particle with zero spin is the extremely inaccessible Higgs boson, singlets in everyday physics are necessarily composed of sets of particles whose individual spins are non-zero, e.g. 1/2 or 1.
The origin of the term "singlet" is that bound quantum systems with zero net angular momentum emit photons within a single spectral line, as opposed to double lines (doublet state) or triple lines (triplet state). The number of spectral lines in this singlet-style terminology has a simple relationship to the spin quantum number: , and .
Singlet-style terminology is also used for systems whose mathematical properties are similar or identical to angular momentum spin states, even when traditional spin is not involved. In particular, the concept of isospin was developed early in the history of particle physics to address the remarkable similarities of protons and neutrons. Within atomic nuclei, protons and neutrons behave in many ways is if they were a single type of particle, the nucleon, with two states. The proton-neutron pair thus by analogy was referred to as a doublet, and the hypothesized underlying nucleon was assigned a spin-like doublet quantum number to differentiate between those two states. Thus the neutron became a nucleon with isospin , and the proton a nucleon with . The isospin doublet notably shares the same SU(2)mathematical structure as the angular momentum doublet. It should be mentioned that this early particle physics focus on nucleons was subsequently replaced by the more fundamental quark model, in which protons and neutrons are interpreted as bound systems of three quarks. The isospin analogy can still be aptly applied to the quarks themselves, however.
While for angular momentum states the singlet-style terminology is seldom used beyond triplets (spin 1), it has proven historically useful for describing much larger particle groups and subgroups that share certain features and are distinguished from each other by quantum numbers beyond spin. An example of this broader use of singlet-style terminology is the nine-member "nonet" of the pseudoscalar mesons.
The simplest possible angular momentum singlet is a set (bound or unbound) of two spin 1/2 (fermion) particles that are oriented so that their spin directions ("up" and "down") oppose each other; that is, they are antiparallel.
The simplest possible bound pair capable of the singlet state is positronium, which consists of an electron and positron (antielectron) bound by their opposite electric charges. The electron and positron in positronium can also have identical or parallel spin orientations, which results in a experimentally distinct form of positronium with a spin 1 or triplet state.
The simplest possible unbound singlet consists of a pair of particles with antiparallel spins, with the pair generated by a single quantum event that conserves angular momentum. Since the same particle is used in such pairs, they can has essentially any spin state. Thought experiments for unbound singlets usually assumed use of two antiparallel spin 1/2 electrons generated from a single quantum event. However, experimental creation of real singlet pairs has far more often focused on generating two antiparallel spin 1 photons, since photons are easier than electrons to generate in pairs and to maintain in an unperturbed quantum state.
The ability of positronium to form both singlet and triplet states is described mathematically by saying that the product of two doublet representations (meaning the electron and positron, which are both spin 1/2 doublets) can be decomposed into the sum of an adjoint representation (the triplet or spin 1 state) and a trivial representation (the singlet or spin 0 state). While the particle interpretation of the positronium triplet and singlet states is arguably more intuitive, the mathematical description enables precise calculations of quantum states and probabilities.
This greater mathematical precision for example makes it possible to assess how singlets and doublets behave under rotation operations. Since a spin 1/2 electron transforms as a doublet under rotation, its experimental response to rotation can be predicted by using the fundamental representation of that doublet, specifically the Lie group SU(2). Applying the operator to the spin state of the electron thus will always result in , or spin 1/2, since the spin-up and spin-down states are both eigenstates of the operator with the same eigenvalue.
Similarly, for a system of two electrons it is possible to measure the total spin by applying , where acts on electron 1 and acts on electron 2. Since this system has two possible spins, it also has two possible eigenvalues and corresponding eigenstates for the total spin operator, corresponding to the spin 0 and spin 1 states.
Singlets and Entangled States
It is important to realize that particles in singlet states need not be locally bound to each other. For example, when the spin states of two electrons are correlated by their emission from a single quantum event that conserves angular momentum, the resulting electrons remain in a shared singlet state even as their separation in space increases indefinitely over time, provided only that their angular momentum states remain unperturbed. In Dirac notation this distance-indifferent singlet state is usually represented as:
The possibility of spatially extended unbound singlet states has considerable historical and even philosophical importance, since consideration such states led eventually to experimental exploration and verification of what is now called quantum entanglement. Quantum entanglement is the ability of quantum systems to maintain relationships that appear to violate the principle of locality, which Albert Einstein considered fundamental and defended throughout his life. Along with Podolsky and Rosen, Einstein proposed the EPR paradox thought experiment to help define his concerns with the non-locality of spatially distributed singlets, using it as a way to assert that quantum mechanics was incomplete.
The difficulty captured by the EPR thought experiment was that by perturbing the angular momentum state of either of the two particles in a spatially distributed singlet state, the quantum state of the remaining particle appears to be "instantaneously" altered, even if the two particles have over time become separated by light years of distance. A critical insight made decades later by John Stewart Bell, who ironically was a strong advocate of Einstein's locality-first perspective, showed that his Bell's theorem could be used to assess the existence or non-existence of singlet entanglement experimentally. The irony was that instead of disproving entanglement, which was Bell's hope, subsequent experiments instead established the reality of entanglement. In fact, there now exist commercial quantum encryption devices whose operation depends fundamentally on the existence and behavior of spatially extended singlets.
A weaker form of Einstein's locality principle remains intact, which is this: Classical, history-setting information cannot be transmitted faster than the speed of light c, not even by using quantum entanglement events. This weaker form of locality is less conceptually elegant than Einstein's absolute locality, but is sufficient to prevent the emergence of causality paradoxes.