fundamental interactions There are four types of fundamental interactions or forces in nature, namely gravitational, electromagnetic (em), weak and strong. The last two are short range and only manifest between nuclear and sub nuclear particles at very short distances. In table FI, the characteristics of the fundamental interactions have been summarized.
Out of these four fundamental interactions, the electromagnetic interaction which occurs between the charged particles is the most well understood. Quantum electrodynamics (QED) which accurately describes e.m. interactions, envisages the photon as the mediator of the force between two charged particles. To illustrate the working of this theory we take the electron magnetic moment which is predicted by Dirac to be eh /2me. However measured values are slightly higher (~ 0.001%). QED explains this difference using radiative corrections which arise from interaction of the charged particle with its own electromagnetic field. The electron emits a virtual photon to be re-absorbed later (see fig. f6b). In the next order the emitted photon may be materialized into e± pair which annihilates creating the virtual photon, to be reabsorbed by the electron (fig. f6c). These processes will contribute to the correction, the magnitude of which decreases as we go to higher orders. The theory which has been worked by R.P.Feynman gives predictions which are in excellent agreement with the experimental results.
Strong forces that binds the nucleons inside a nucleus has a very short range and are charge independent. It is the same force that operates between the hadrons* (mesons and baryons). Since hadrons are made of quarks* which are "colored" it is believed that color plays the same role as charge. The theory which is being worked out is called quantum chromodynamics. In this theory the mediators are called gluons, which are eight in number, and they themselves carry color charges unlike the photon.
Table FI
Fundamental interactions. The strength of e.m. interaction is taken 1 arbitrarily.
|
force |
Range |
Relative Strength |
particles acted upon |
name |
mediator mass (GeV) |
spin |
name & status of theory |
|
gravity |
¥ |
10-37 |
all particles |
graviton |
0 |
2 |
quantized theory not established |
|
electro- magnetic |
¥ |
1 |
all charged particles |
photon |
0 |
1 |
quantum electro dynamics, established |
|
weak |
<10-13 cm |
10-11 |
leptons & hadrons |
W+,W- & Z0 |
~ 78~ 89 |
1 1 |
unified gauge theory, almost established |
|
strong |
10-13 cm |
100 |
hadron |
gluons(8) |
0 |
1 |
quantum chromo dynamics, not established |
The weak interactions is believed to be mediated by spin 1 particles called intermediate vector bosons (0 spin and negative parity), W+, W- and Z0 which are massive. The weak interaction responsible for b decay, and many other processes is well described by V-A theory in which two forms of vector interactions (V and A) participate. The mixing of V and A causes the parity violation, or the lack of invariance under mirror reflection, which is characteristic of weak interactions.
The gravitational interaction is the weakest of all and least understood. It is speculated that gravitons are mediators of this force.
An unified theory of all interactions has eluded scientists for many years. In 1967 a major success was achieved by Abdus Salam, Steven Weinberg and Sheldon Glashow who described the weak and the electromagnetic interactions under one frame work of electro-weak force described by a family of four particles-the photon, two charged W± bosons and a neutral boson Z0 .