NUCLEAR AND PARTICLE PHYSICS -2

 

                    Properties of Nucleus_- I

I-Nuclear angular momentum

L- Nuclear orbital angular moment

S- Nuclear spin  angular momentum

Angular momentum- angular momentum of a nucleus is a constant quantity because nucleus being an isolated system i.e. the external torque is equal to zero.

I represent angular momentum quantum number. The eigen values of the square of the angular momentum operator are I(I+1) in the unit of

 2 Ψ = I(I+1) 2 Ψ

Iz is the Z- component of total angular momentum

zΨ = mΨ, m is the eigen values of z, m ℏ is the Z component of angular momentum.

both have common eigen function [ ,]

Total angular momentum (I) = ℏ✓{I(I+1)}

For a given value of I, m can take 2I+1 values from +I to –I

I is not only integer but half integer i.e. I= 0, 1/2, 1, 3/2 …..

Half integer value of I is due to the Pauli’s proposed intrinsic spin.

Total angular momentum is the sum of orbital angular momentum and spin angular momentum, I=L + S

Intrinsic spins are integers if the mass number A is even and half integer when A is odd.

Intrinsic spin ranges from zero as in 4He and 12C up to 7 as in 176Lu.

The total, orbital and spin angular momentum of the nuclus,

PI2= I(I+1) 2

PL2 = L(L+1) 2

PS2= = S(S+1) 2

Parity:

This refers to the behaviour of a wave function at the symmetric position. the wave function of a physical system at (X, Y, Z) is Ψ (X, Y, Z) that of Ψ (-X, -Y, -Z) at (-X, -Y, -Z). The Hamiltonian of the system is invariant under space invariance then

Ψ (-X, -Y, -Z) = Ψ (X, Y, Z) 

 Ψ (-X, -Y, -Z) = - Ψ (X, Y, Z)

In the first case, the wave function has even parity, and in the second case, the wave function has odd parity. Elementary particles may possess intrinsic parity which is related to the inversion of some internal axis of the particle. The law of conservation of parity, states that the parity is conserved in a process if the mirror image of process is also a process which can occur in nature. By convention, the parity of nucleus is taken as even.

 By interchanging of the coordinates of two particles, if the sign of the wave function does not change, then the wave function is symmetric and the resulting Quantum statistics is Bose-Einstein statistics. When the sign of the wave function changes as a result of interchange of the coordinates, then we get anti- symmetric wave function and the statistics is Fermi-Dirac statistics.

P Ψ (X1, X2) = ± Ψ (-X1, -X2)

P is the parity operator whose eigen values are +1 and -1.

P= +1 for even parity and P= -1 for odd parity.

Magnetic dipole moment

The magnetic moment 𝜇 is related to the angular momentum by,

𝜇 = ( e/2m) L and more generalised relation is 𝜇 = g ( e/2m)L

                                                                                                              

For nucleus, the magnetic moment  𝜇 = g (e/2Mp)  I, where I is the total angular momentum.

𝜇= g 𝜇N (I/), where 𝜇N=  ( e/2Mp) is called nuclear magneton.

The measured values of the magnetic moment of proton and neutron are 

𝜇p = 2.7927 𝜇N                                  𝜇B = 9.27 × 10-24 J/T

𝜇n = -1.9131 𝜇N                              𝜇N = 5.05 × 10-27 J/T

The above values so that the proton and neutron magnetic moment are of the order 10-3 times the electronic magnetic moment. The values are unexpected. The expected ones: The protons should have 1 𝜇N and the neutron should have 0 because neutrons have no charge. 

 

This indicates that both neutron and proton have non-uniform charge distribution and in the case of neutron the direction of the magnetic moment is opposite to that of the spin angular momentum vector. This can be understood from meson's theory. It means that the sign of electric charge constantly exchanged between nuclear particles. This helps to contribute to non-zero orbital magnetic moments. 

 The magnetic moments of protons and neutrons are related to their intrinsic spin angular momentum as follows.

Spin angular momentum pp = sp                    pn=sn where sp = sn = ½

For electrons,  𝜇e / pe= ge(e/2Me )       where ge = -2, Lande’s factor

For protons and neutrons,

   μp/ ppgp(e/2Mp ) ;  gp =2μN  = 2x 2.7927=5.5855

   μn/ pngn(e/2Mn ) ;  gn =2μN = -3.8263

𝜇pgp(e/2Mp )sp   ;         𝜇p = (gp/2)𝜇N

𝜇ngn(e/2Mn )sn   ;         𝜇n = (gn/2)𝜇N

These results show that proton and neutron have a complex structure.

 

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