The Standard Model of particle physics is the theory describing three of the four known fundamental forces (the electromagnetic, weak, and strong interactions, and not including the gravitational force) in the universe, as well as classifying all known elementary particles. It was developed in stages throughout the latter half of the 20th century, through the work of many scientists around the world,^{[1]} with the current formulation being finalized in the mid1970s upon experimental confirmation of the existence of quarks. Since then, confirmation of the top quark (1995), the tau neutrino (2000), and the Higgs boson (2012) have added further credence to the Standard Model. In addition, the Standard Model has predicted various properties of weak neutral currents and the W and Z bosons with great accuracy.
Although the Standard Model is believed to be theoretically selfconsistent^{[2]} and has demonstrated huge successes in providing experimental predictions, it leaves some phenomena unexplained and falls short of being a complete theory of fundamental interactions. It does not fully explain baryon asymmetry, incorporate the full theory of gravitation^{[3]} as described by general relativity, or account for the accelerating expansion of the Universe as possibly described by dark energy. The model does not contain any viable dark matter particle that possesses all of the required properties deduced from observational cosmology. It also does not incorporate neutrino oscillations and their nonzero masses.
The development of the Standard Model was driven by theoretical and experimental particle physicists alike. For theorists, the Standard Model is a paradigm of a quantum field theory, which exhibits a wide range of phenomena including spontaneous symmetry breaking, anomalies and nonperturbative behavior. It is used as a basis for building more exotic models that incorporate hypothetical particles, extra dimensions, and elaborate symmetries (such as supersymmetry) in an attempt to explain experimental results at variance with the Standard Model, such as the existence of dark matter and neutrino oscillations.
In 1954, Chen Ning Yang and Robert Mills extended the concept of gauge theory for abelian groups, e.g. quantum electrodynamics, to nonabelian groups to provide an explanation for strong interactions.^{[4]} In 1961, Sheldon Glashow combined the electromagnetic and weak interactions.^{[5]} In 1967 Steven Weinberg^{[6]} and Abdus Salam^{[7]} incorporated the Higgs mechanism^{[8]}^{[9]}^{[10]} into Glashow's electroweak interaction, giving it its modern form.
The Higgs mechanism is believed to give rise to the masses of all the elementary particles in the Standard Model. This includes the masses of the W and Z bosons, and the masses of the fermions, i.e. the quarks and leptons.
After the neutral weak currents caused by Z boson exchange were discovered at CERN in 1973,^{[11]}^{[12]}^{[13]}^{[14]} the electroweak theory became widely accepted and Glashow, Salam, and Weinberg shared the 1979 Nobel Prize in Physics for discovering it. The W^{±} and Z^{0}bosons were discovered experimentally in 1983; and the ratio of their masses was found to be as the Standard Model predicted.^{[15]}
The theory of the strong interaction (i.e. quantum chromodynamics, QCD), to which many contributed, acquired its modern form in 197374 when asymptotic freedom was proposed^{[16]}^{[17]} (a development which made QCD the main focus of theoretical research)^{[18]} and experiments confirmed that the hadrons were composed of fractionally charged quarks.^{[19]}^{[20]}
The term "Standard Model" was first coined by Abraham Pais and Sam Treiman in 1975,^{[21]} with reference to the electroweak theory with four quarks.^{[22]}
The Standard Model includes members of several classes of elementary particles, which in turn can be distinguished by other characteristics, such as color charge.
All particles can be summarized as follows:
Elementary particles  
Elementary fermionsHalfinteger spinObey the FermiDirac statistics  Elementary bosonsInteger spinObey the BoseEinstein statistics  
Quarks and antiquarksSpin = Have color chargeParticipate in strong interactions  Leptons and antileptonsSpin = No color chargeElectroweak interactions  Gauge bosonsSpin = 1Force carriers  Scalar bosonsSpin = 0  
Three Generations
 Four kinds (four fundamental interactions)
 Unique Higgs boson (^{} _{}H^{0} _{})  
Notes:
[†] An antielectron (^{}
_{}e^{+}
_{}) is conventionally called a "positron".
The Standard Model includes 12 elementary particles of spin , known as fermions. According to the spinstatistics theorem, fermions respect the Pauli exclusion principle. Each fermion has a corresponding antiparticle.
The defining property of quarks is that they carry color charge, and hence interact via the strong interaction. The phenomenon of color confinement results in quarks being very strongly bound to one another, forming colorneutral composite particles called hadrons that contain either a quark and an antiquark (mesons) or three quarks (baryons). The lightest baryons are the proton and the neutron. Quarks also carry electric charge and weak isospin. Hence they interact with other fermions via electromagnetism and the weak interaction. The remaining six fermions do not carry color charge and are called leptons. The three neutrinos do not carry electric charge either, so their motion is directly influenced only by the weak nuclear force, which makes them notoriously difficult to detect. By contrast, by virtue of carrying an electric charge, the electron, muon, and tau all interact electromagnetically.
Each member of a generation has greater mass than the corresponding particles of lower generations. The firstgeneration charged particles do not decay, hence all ordinary (baryonic) matter is made of such particles. Specifically, all atoms consist of electrons orbiting around atomic nuclei, ultimately constituted of up and down quarks. On the other hand, second and thirdgeneration charged particles decay with very short halflives and are observed only in very highenergy environments. Neutrinos of all generations also do not decay and pervade the universe, but rarely interact with baryonic matter.
In the Standard Model, gauge bosons are defined as force carriers that mediate the strong, weak, and electromagnetic fundamental interactions.
Interactions in physics are the ways that particles influence other particles. At a macroscopic level, electromagnetism allows particles to interact with one another via electric and magnetic fields, and gravitation allows particles with mass to attract one another in accordance with Einstein's theory of general relativity. The Standard Model explains such forces as resulting from matter particles exchanging other particles, generally referred to as force mediating particles. When a forcemediating particle is exchanged, the effect at a macroscopic level is equivalent to a force influencing both of them, and the particle is therefore said to have mediated (i.e., been the agent of) that force. The Feynman diagram calculations, which are a graphical representation of the perturbation theory approximation, invoke "force mediating particles", and when applied to analyze highenergy scattering experiments are in reasonable agreement with the data. However, perturbation theory (and with it the concept of a "forcemediating particle") fails in other situations. These include lowenergy quantum chromodynamics, bound states, and solitons.
The gauge bosons of the Standard Model all have spin (as do matter particles). The value of the spin is 1, making them bosons. As a result, they do not follow the Pauli exclusion principle that constrains fermions: thus bosons (e.g. photons) do not have a theoretical limit on their spatial density (number per volume). The types of gauge bosons are described below.
The interactions between all the particles described by the Standard Model are summarized by the diagrams on the right of this section.
The Higgs particle is a massive scalar elementary particle theorized by Peter Higgs in 1964, when he showed that Goldstone's 1962 theorem (generic continuous symmetry, which is spontaneously broken) provides a third polarisation of a massive vector field. Hence, Goldstone's original scalar doublet, the massive spinzero particle, was proposed as the Higgs boson, and is a key building block in the Standard Model.^{[8]}^{[9]}^{[10]}^{[24]} It has no intrinsic spin, and for that reason is classified as a boson (like the gauge bosons, which have integer spin).
The Higgs boson plays a unique role in the Standard Model, by explaining why the other elementary particles, except the photon and gluon, are massive. In particular, the Higgs boson explains why the photon has no mass, while the W and Z bosons are very heavy. Elementaryparticle masses, and the differences between electromagnetism (mediated by the photon) and the weak force (mediated by the W and Z bosons), are critical to many aspects of the structure of microscopic (and hence macroscopic) matter. In electroweak theory, the Higgs boson generates the masses of the leptons (electron, muon, and tau) and quarks. As the Higgs boson is massive, it must interact with itself.
Because the Higgs boson is a very massive particle and also decays almost immediately when created, only a very highenergy particle accelerator can observe and record it. Experiments to confirm and determine the nature of the Higgs boson using the Large Hadron Collider (LHC) at CERN began in early 2010 and were performed at Fermilab's Tevatron until its closure in late 2011. Mathematical consistency of the Standard Model requires that any mechanism capable of generating the masses of elementary particles must become visible^{[clarification needed]} at energies above ;^{[25]} therefore, the LHC (designed to collide two proton beams) was built to answer the question of whether the Higgs boson actually exists.^{[26]}
On 4 July 2012, two of the experiments at the LHC (ATLAS and CMS) both reported independently that they found a new particle with a mass of about (about 133 proton masses, on the order of ), which is "consistent with the Higgs boson".^{[27]}^{[28]}^{[29]}^{[30]}^{[31]}^{[32]} On 13 March 2013, it was confirmed to be the searchedfor Higgs boson.^{[33]}^{[34]}
Parameters of the Standard Model  

Symbol  Description  Renormalization scheme (point) 
Value  
m_{e}  Electron mass  0.511 MeV  
m_{?}  Muon mass  105.7 MeV  
m_{?}  Tau mass  1.78 GeV  
m_{u}  Up quark mass  ?_{MS} = 2 GeV  1.9 MeV  
m_{d}  Down quark mass  ?_{MS} = 2 GeV  4.4 MeV  
m_{s}  Strange quark mass  ?_{MS} = 2 GeV  87 MeV  
m_{c}  Charm quark mass  ?_{MS} = m_{c}  1.32 GeV  
m_{b}  Bottom quark mass  ?_{MS} = m_{b}  4.24 GeV  
m_{t}  Top quark mass  On shell scheme  173.5 GeV  
?_{12}  CKM 12mixing angle  13.1°  
?_{23}  CKM 23mixing angle  2.4°  
?_{13}  CKM 13mixing angle  0.2°  
?  CKM CP violation Phase  0.995  
g_{1} or g  U(1) gauge coupling  ?_{MS} = m_{Z}  0.357  
g_{2} or g  SU(2) gauge coupling  ?_{MS} = m_{Z}  0.652  
g_{3} or g_{s}  SU(3) gauge coupling  ?_{MS} = m_{Z}  1.221  
?_{QCD}  QCD vacuum angle  ~0  
v  Higgs vacuum expectation value  246 GeV  
m_{H}  Higgs mass 
Technically, quantum field theory provides the mathematical framework for the Standard Model, in which a Lagrangian controls the dynamics and kinematics of the theory. Each kind of particle is described in terms of a dynamical field that pervades spacetime. The construction of the Standard Model proceeds following the modern method of constructing most field theories: by first postulating a set of symmetries of the system, and then by writing down the most general renormalizable Lagrangian from its particle (field) content that observes these symmetries.
The global Poincaré symmetry is postulated for all relativistic quantum field theories. It consists of the familiar translational symmetry, rotational symmetry and the inertial reference frame invariance central to the theory of special relativity. The local SU(3)×SU(2)×U(1) gauge symmetry is an internal symmetry that essentially defines the Standard Model. Roughly, the three factors of the gauge symmetry give rise to the three fundamental interactions. The fields fall into different representations of the various symmetry groups of the Standard Model (see table). Upon writing the most general Lagrangian, one finds that the dynamics depends on 19 parameters, whose numerical values are established by experiment. The parameters are summarized in the table (made visible by clicking "show") above (note: the Higgs mass is at , the Higgs selfcoupling strength ? ~ ).
The quantum chromodynamics (QCD) sector defines the interactions between quarks and gluons, which is a YangMills gauge theory with SU(3) symmetry, generated by T^{a}. Since leptons do not interact with gluons, they are not affected by this sector. The Dirac Lagrangian of the quarks coupled to the gluon fields is given by
where
The electroweak sector is a YangMills gauge theory with the symmetry group U(1) × SU(2)_{L},
where
Notice that the addition of fermion mass terms into the electroweak lagrangian is forbidden, since terms of the form do not respect U(1) × SU(2)_{L} gauge invariance. Neither is it possible to add explicit mass terms for the U(1) and SU(2) gauge fields. The Higgs mechanism is responsible for the generation of the gauge boson masses, and the fermion masses result from Yukawatype interactions with the Higgs field.
In the Standard Model, the Higgs field is a complex scalar of the group SU(2)_{L}:
where the superscripts + and 0 indicate the electric charge (Q) of the components. The weak hypercharge (Y_{W}) of both components is 1.
Before symmetry breaking, the Higgs Lagrangian is
which up to a divergence term, (i.e. after partial integration) can also be written as
The Yukawa interaction terms are
where G_{u,d} are 3 × 3 matrices of Yukawa couplings, with the ij term giving the coupling of the generations i and j.
This section needs expansion. You can help by adding to it. (October 2015) 
The Standard Model describes three of the four fundamental interactions in nature; only gravity remains unexplained. In the Standard Model, such an interaction is described as an exchange of bosons between the objects affected, such as a photon for the electromagnetic force and a gluon for the strong interaction. Those particles are called force carriers or messenger particles.^{[35]}
Property/Interaction  Gravitation  Electroweak  Strong  

Weak  Electromagnetic  Fundamental  Residual  
Mediating particles  Not yet observed (Graviton hypothesised) 
W^{+}, W^{} and Z^{0}  ? (photon)  Gluons  ?, ? and ? mesons 
Affected particles  All particles  Lefthanded fermions  Electrically charged  Quarks, gluons  Hadrons 
Acts on  Mass, energy  Flavor  Electric charge  Color charge  
Bound states formed  Planets, stars, galaxies, galaxy groups  n/a  Atoms, molecules  Hadrons  Atomic nuclei 
Strength at the scale of quarks (relative to electromagnetism) 
(predicted)  1  60  Not applicable to quarks  
Strength at the scale of protons/neutrons (relative to electromagnetism) 
(predicted)  1  Not applicable to hadrons 
20 
The Standard Model (SM) predicted the existence of the W and Z bosons, gluon, and the top and charm quarks and predicted many of their properties before these particles were observed. The predictions were experimentally confirmed with good precision.^{[37]}
The SM also predicted the existence of the Higgs boson, found in 2012 at the Large Hadron Collider, as the last particle of the SM.^{[38]}
Unsolved problem in physics:

Selfconsistency of the Standard Model (currently formulated as a nonabelian gauge theory quantized through pathintegrals) has not been mathematically proven. While regularized versions useful for approximate computations (for example lattice gauge theory) exist, it is not known whether they converge (in the sense of Smatrix elements) in the limit that the regulator is removed. A key question related to the consistency is the YangMills existence and mass gap problem.
Experiments indicate that neutrinos have mass, which the classic Standard Model did not allow.^{[39]} To accommodate this finding, the classic Standard Model can be modified to include neutrino mass.
If one insists on using only Standard Model particles, this can be achieved by adding a nonrenormalizable interaction of leptons with the Higgs boson.^{[40]} On a fundamental level, such an interaction emerges in the seesaw mechanism where heavy righthanded neutrinos are added to the theory. This is natural in the leftright symmetric extension of the Standard Model^{[41]}^{[42]} and in certain grand unified theories.^{[43]} As long as new physics appears below or around 10^{14}GeV, the neutrino masses can be of the right order of magnitude.
Theoretical and experimental research has attempted to extend the Standard Model into a Unified field theory or a Theory of everything, a complete theory explaining all physical phenomena including constants. Inadequacies of the Standard Model that motivate such research include:
Currently, no proposed Theory of Everything has been widely accepted or verified.
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