Seesaw mechanism
In the theory of grand unification of particle physics, and, in particular, in theories of neutrino masses and neutrino oscillation, the seesaw mechanism is a generic model used to understand the relative sizes of observed neutrino masses, of the order of eV,  compared to those of quarks and charged leptons, which are millions of times heavier. The name of the seesaw mechanism was given by Tsutomu Yanagida in a Tokyo conference in 1981. There are several types of models, each extending the Standard Model. The simplest version, "Type 1," extends the Standard Model by assuming two or more additional right-handed neutrino fields
inert under the electroweak interaction,
and the existence of a very large mass scale. This allows the mass scale to be identifiable with the postulated scale of grand unification. Type 1 seesaw 
This model produces a light neutrino, for each of the three known neutrino flavors, and a corresponding very heavy neutrino for each flavor, which has yet to be observed. The simple mathematical principle behind the seesaw mechanism is the following property of any 2×2 matrix of the form

It has two eigenvalues:

and

The geometric mean of  and  equals , since the determinant . Thus, if one of the eigenvalues goes up, the other goes down, and vice versa. This is the point of the name "seesaw" of the mechanism. In applying this model to neutrinos,  is taken to be much larger than 
Then the larger eigenvalue,  is approximately equal to  while the smaller eigenvalue is approximately equal to

This mechanism serves to explain why the neutrino masses are so small. The matrix  is essentially the mass matrix for the neutrinos. The Majorana mass component  is comparable to the GUT scale and violates lepton number conservation; while the Dirac mass components  are of order of the much smaller electroweak scale, called the VEV or vacuum expectation value below. The smaller eigenvalue  then leads to a very small neutrino mass, comparable to , which is in qualitative accord with experiments—sometimes regarded as supportive evidence for the framework of Grand Unified Theories. Background 
The 2×2 matrix  arises in a natural manner within the standard model by considering the most general mass matrix allowed by gauge invariance of the standard model action, and the corresponding charges of the lepton- and neutrino fields. Call the neutrino part of a Weyl spinor  a part of a left-handed lepton weak isospin doublet; the other part is the left-handed charged lepton 

as it is present in the minimal standard model with neutrino masses omitted, and let  be a postulated right-handed neutrino Weyl spinor which is a singlet under weak isospin – i.e. a neutrino that fails to interact weakly, such as a sterile neutrino. There are now three ways to form Lorentz covariant mass terms, giving either

and their complex conjugates, which can be written as a quadratic form,

Since the right-handed neutrino spinor is uncharged under all standard model gauge symmetries,  is a free parameter which can in principle take any arbitrary value. The parameter  is forbidden by electroweak gauge symmetry, and can only appear after the symmetry has been spontaneous broken by a Higgs mechanism, like the Dirac masses of the charged leptons. In particular, since  has weak isospin  like the Higgs field , and  has weak isospin 0, the mass parameter  can be generated from Yukawa interactions with the Higgs field, in the conventional standard model fashion,

This means that  is naturally of the order of the vacuum expectation value of the standard model Higgs field, 
the vacuum expectation value (VEV)

if the dimensionless Yukawa coupling is of order . It can be chosen smaller consistently, but extreme values  can make the model nonperturbative. The parameter  on the other hand, is forbidden, since no renormalizable singlet under weak hypercharge and isospin can be formed using these doublet components – only a nonrenormalizable, dimension 5 term is allowed. This is the origin of the pattern and hierarchy of scales of the mass matrix  within the "Type 1" seesaw mechanism. The large size of  can be motivated in the context of grand unification. In such models, enlarged gauge symmetries may be present, which initially force  in the unbroken phase, but generate a large, non-vanishing value  around the scale of their spontaneous symmetry breaking. So given a mass  one has  A huge scale has thus induced a dramatically small neutrino mass for the eigenvector

See also 
 Majoron
 Spinor

Footnotes

References

External links
 

Neutrinos
Physics beyond the Standard Model