Sunday, October 7, 2018

YUKAWA THEORY (FULL EXPLAIN)


YUKAWA THEORY
In order to explain the origin of strong nuclear forces which are believed to exist in between nucleons, Yukawa in 1935 proposed a theory of nuclear forces known’s as the Meson theory of nuclear forces. He predicted the existence of particle having rest mass intermediate the rest masses of an electron and proton and named as Meson.
According to Yukawa’s theory the force between two nucleons is due to the continuous rapid exchange of mesons between them as the electric force between the two charged particles is due to the exchange of photons. The most important particle of the nuclear force is that it has finite range. It decreases extremely rapidly when interacting particles are more than one Fermi apart. Experiments show that in practice there is a critical length beyond which this interaction does not exist. In this respect a nuclear force differs fundamentally from a force with infinite range such as the electric force. We must therefore expect that the dimension of length. Such a potential was first proposed by Yukawa which has the form Yukawa potential
Where g is positive constant and r i

s the separation between two nucleons.
Yukawa explained on the theoretical ground that for a finite nuclear range 10^-13 cm
The rest mass of meson should be 200 times the rest mass of an electron. The first particle of intermediate mass to be detected was u meson with rest mass 200 times the rest mass of electron. The u meson was found to have weak interactions with nuclei and did not
Agree with Yukawa theory that mesons have strong nuclear interactions with nuclei.
This problem was solved with the discovery of pi-mesons (pions) in 1947. The pions were found to have strong interactions with nuclei and they are believed to be Yukawa’s particles. The nuclear force is caused by the continuous rapid exchange of pions between the nucleons. The pions exist in three states pi-positive, pi-negative, pi-neutral. The rest mass of charged pion is 273me and that of neutral pion is 264me, where me is rest mass of electron. The exchange reactions involved in nuclear forces are
Which shows that pi-positive and pi-negative are exchange particles of p-n
And n-p forces while pi-neutral is exchange particle for p-p and n-n forces.


YUKAWA INTERACTION POTENTIAL FOR MESON FIELD


Yukawa interaction potential for meson field
Nuclear forces are produced by a field known as meson field it is short range field within a distance of 10^-13 cm. the meson field is produced by π meson which are continuously exchanging between nucleons.
In obtain wave equation for meson field we consider relatisvistic relation for energy


WHAT IS NUCLEAR PHYSICS( BASIC DEFINATIONS)



THEORETICAL ESTIMATE OF PIONS MASS


Theoretical estimate of pions mass
It can be noted that each one of the exchange reaction violates the law of conservation of energy for a very short time between emission and absorption of pions.
This temporary failure of energy conservation can be used to obtain a theoretical estimate of the pions mass
According to uncertainty principle.
Where del-E is the uncertainty in the energy measurements and del-t is the time interval between the ejection of a pion by one nucleon and its capture by another and h is planks constant. The range R of a nuclear force is about 1.5 Fermi if the pion travels with velocity of light c then

This value of change in energy gives the mass of pion exchanged between the nucleus and is very close to the mass of pion (140MeV) determined experimentally. This proves that exchange particle involved in exchange reaction is pi-meson as predicted by Yukawa

SUCCESS OF MESON THEORY


  1. (1) If all the pions exchanges are permitted It is straight forward to couple the corresponding fields to nucleons in such a way that charge independence results.
  2. (2) Pion exchange idea also explains the saturation of nuclear forces. A study of complex nuclei shows that average binding energy per nucleon is constant which leads to the idea of saturation of nucleons.
  3. (3) Pion exchange also eliminates the equation of magnetic moments of nucleons. A neutron as a particle with +ve core surrounded by –ve charged pions cloud exhibit a magnetic moment while remaining neutral in over all charge