A vectorboson is a boson with spin equal to one unit of
The most familiar vectorboson is the photon, or quantum of light, which is a gauge boson.
There also exist composite particles that are vectorbosons, such as the vector mesons, made of a quark and antiquark with a total angular momentum of one unit.
In technical terms, they are vector gauge bosons that mediate strong color charge interactions of quarks in quantum chromodynamics (QCD).
Vector particles usually have three spin states, but gauge invariance reduces the number of spin states of a gluon to two; negative intrinsic parity, and zero isospin.
The gluons are vector fields in the adjoint representation (octets, denoted 8) of colour SU(3).
Three vectorbosons are responsible for the weak nuclear force.
These particles were predicted by the Weinberg-Salam theory of the 1960s and later discovered in the 1980s., See Intermediate VectorBoson., Massive boson thought to have been abundant in the early universe, when the unified electroweak force was manifest.
Z particle (3 facts) - Massive boson thought to have been abundant in the early universe, when the unified electroweak force was manifest., Particle that transmits the unified electromagnetic and weak nuclear forces.
...the electromagnetic force, the graviton and the gravitational force, the intermediate vectorboson and the weak interaction, and the gluon and the strong interaction....
...Either of two bosons, the W particle or the Z particle, that are quanta of the weak interaction.
...A hypothetical boson having no charge or spin and small mass, proposed to explain the existence of certain symmetries of the strong nuclear force.
These are all vector (force) fields with their respective quanta: the graviton, the photon, the gluons, the W's and Z. Although the graviton is still not found, its existence can be describe by string theory.
These are all vectorbosons, i.e., force particles.
The photon, the gluons, all vectorboson with no mass, means the Higgs mechanicism does not work on them.
Due to these distinctive characteristics it can immediately be observed that the theory of the intermediate boson of the weak interactions leads to difficulties similar to the ones presented by the model of point interaction.
It is clear, then, that the renormalization of the theory with intermediate boson based on the Lagrangian (117) is hopeless.
In other words, the previous discussion indicates that the limit imposed by the unitarity to the cross section of a given process, via the optical theorem, will surely be violated by the massive intermediate vectorboson model.
VECTORS For May 2006(Site not responding. Last check: 2007-10-30)
The standard model told the experimental physicists where to look for the vectorbosons, and they were finally discovered in 1983 by Carlo Rubbia and his colleagues.
In contrast to the photon and the gluons, which are spin-1 bosons, the Higgs boson is a spin-0 boson, a fact that gives it distinctive properties.
The Higgs boson is supposed to be highly interactive with almost everything, and the interactions of Higgs boson (or, equivalently, the Higgs field) with a particle would impede the particle's motion, effectively giving the particle mass.
The current experimental status of vectorboson p T measurements is reviewed.
The recent Monte-Carlo implementations of vectorboson p T distributions are compared to the data and the issues involved in making a meaningful comparison are outlined.
Introduction The study of quark anti-quark annihilation producing high mass fl, Z and W bosons is a rich area for QCD studies.
When only electric field is present the Bogoliubov coefficients are independent of boson polarization and are the same as for scalar boson.
When both electric and magnetic fields are present and collinear, the Bogoliubov coefficients for states with boson spin perpendicular to the field are again the same as in scalar case.
For gyromagnetic ratio g=2 the vectorboson interaction with constant electromagnetic field is described by the functions, which can be expected by comparing wave functions for scalar and Dirac particle in constant electromagnetic field.
It is through the exchange of W and Z bosons that two particles interact weakly, just as it is through the exchange of photons that two charged particles interact electromagnetically.
The intermediate vectorbosons were postulated to exist in the 1960s; however, their large masses prevented their production and study at accelerators until 1983.
Their discovery was a key step toward unification of the weak and electromagnetic interactions.
VectorBoson Scattering in the Standard Model--an Overview of Formulae -- from Mathematica Information Center
Tree-level scattering amplitudes of longitudinally polarized electroweak vectorbosons in the Standard Model are calculated using Mathematica package Feyncalc.
The modifications of low-energy theorems for longitudinally polarized W and Z in the Standard Model are discussed.
We write down a minimal set of genuine four-coupling operators between vectorbosons which have no connection to the standard parametrisation of the trilinear anomalous W couplings.
These requirements are strong enough to forbid or highly suppress any contribution to weak vectorboson self-energies.
We study the effects of these couplings at the NLC (500 GeV) in all possible three vectorboson productions: e+ e- arrow W+ W - gamma, ZZ gamma and Z gamma gamma.
Calculation of the matrix elements of the Hamiltonian of the interacting vectorboson model using computer algebra - matrix elements of the Hamiltonian and some U(6)-Clebsch-Gordon coefficients.
Calculation of the matrix elements of the Hamiltonian of the interacting vectorboson model using computer algebra - basic concepts of the interacting vectorboson model and matrix elements of the SU(3)-Quadrupole operator.
Calculation of the matrix elements of the Hamiltonian of the interacting vectorboson model using computer algebra - matrix elements of the Hamiltonian - analytical results.
Generalized Electroform Field Equations of Vector-Boson Field Theory : The Mirror-Image Maxwell's Equations for Long- ...(Site not responding. Last check: 2007-10-30)
A contact-force representation for the weak part of the field is also derivable from the electroform field equations by a method described by Cottingham and Greenwood, in Introduction to Nuclear Physics.
Introducing the principle of equivalence as Einstein did in 1911, one imbeds the generalized Maxwellian equations of classical vectorboson field theory into a metric with gravitational time-dilation only to describe the forces.
The falling-ruler thought experiments sometimes used to justify curvature in the spacial part of the metric do not hold for the stationary rulers described by the GR metric, so this book takes the spacial part of the metric to be flat.
Energy Citations Database (ECD) - Energy and Energy-Related Bibliographic Citations(Site not responding. Last check: 2007-10-30)
We derive exact expressions for luminosities of massive vector-boson pairs which can be used to describe the cross sections for processes in hadron collisions or{ital e}{sup+}{ital e}{sup{minus}} annihilation which proceed via two-vector-boson scattering.
Our approach correctly takes into account the mutual influence of the emission of one vectorboson on the emission of a second one.
We show that only approximately the exact luminosities can be factorized into convolutions of single-vector-boson distributions.
vector boson - yourDictionary.com - American Heritage Dictionary(Site not responding. Last check: 2007-10-30)
vectorboson - yourDictionary.com - American Heritage Dictionary
Any of the elementary particles that mediate one of the four fundamental forces.
The particles and their corresponding forces are the photon and the electromagnetic force, the graviton and the gravitational force, the intermediate vectorboson and the weak interaction, and the gluon and the strong interaction.
Rotational limit of the interacting two-vector boson model
The rotational limit of the interacting two-vector-boson model is investigated.
In particular, reselling and systematic downloading of files is prohibited.
stacks.iop.org /0305-4616/9/521 (213 words)
Untitled Document(Site not responding. Last check: 2007-10-30)
In this working group, we consider topics associated with single W and Z boson production and decay and the possibilities presented with Run II.
Additionally, with the much higher statistics of Run II, we will be able to consider a triple-differential measurement of the jets and specific jet-tags (charm or bottom).
The attempt to drive the uncertainty on the W mass to the tens of MeV will likely require further constraints on the production model for vectorbosons at low-pT.
Sudakov logarithm resummation for vectorboson production at hadron colliders
A complete description of W and Z boson production at high-energy colliders requires the resummation of large Sudakov logarithms which dominate the production at small transverse momentum.
Currently there are two techniques for performing this resummation: impact parameter space and transverse momentum space.