Nuclear Physics

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  1. Introduction
  2. Nuclear Systematics

[edit] Units and Conventions

We shall use natural units. So, we shall choose \hbar = c = 1 where \hbar is the Plank's constant and c is the velocity of light. Because the product of length and momentum has dimensions of \hbar, the units of length and momentum are inverse of each other. Similarly length/time has dimensions of velocity and therefore the units of length and time are same. Einstein's mass energy relation is E = mc2 and the energy-momentum relation is E=\sqrt{p^2+m^2}. These relations imply that the units of energy, momentum and mass are same. The angular momentum has same dimensions as the Plank's constant so it is dimensionless. The dimensions of all the physical quantities in natural units can be fixed using such arguments.

The natural length scale in nuclear physics is set by the typical size of nuclei. It is chosen to be 1fm = 10 − 13cm. The unit of time can be chosen to be same. In cgs units 1fm of time is 10^{-13}  cm/c = 1./3. \times 10^{-23} sec. The energy, momentum and mass can then be measured in inverse fm. Alternatively, we can choose to measure energy, momentum and mass in units of MeV, which is a typical energy scale in nuclear physics. Then the length and time is measured in inverse MeV. The product of \hbar and c has the dimension of energy times time and its value is 197.3 MeV fm. We can use this fact to convert energy units into length units. That is, 197.3MeV = 1fm − 1. For back-of-the envelop calculations we can take 200MeVfm = 1. This introduces an error of about a percent in the calculations.

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