Abstract-The hierarchy of states is developed with increasing the value of l, the orbital angular momentum, is now called "Shrivastava's hierarchy of fractional states". We have examined the odd denominator states as extended to a hierarchy of continued fraction which describes a very large abundance of fractional states. The heirarchy developed by random numbers m and p i (i=1,2,…,4) by using the continued fraction is known as the Haldane's hierarchy. We find that the predictions of the Dirac equation agree with the idea of fractional charges. We have introduced the combination of spin and orbital quantum numbers, including the negative sign for spin, in such a way that there occur fractional charges through the Bohr magneton. This leads to doubling of eigen values so that we define an additional matrix the properties of which are important when magnetic field is present. There is a spin-charge coupling so that spin ½ particle can have the zero or one charge. The Dirac equation can accommodate not only charges of 0 and ±e but also fractional values such as 1/3 and 2/3. Index Terms-Dirac equation, fractional charges, hierarchy, angular momentum.
I. INTRODUCTIONRecently, in three papers, we have laid down the basically correct theory of the quantum Hall effect [1]- [3]. It has been found [4], [5] in the Hall effect that the transverse conductivity as a function of magnetic field shows plateaus at certain fractions of e 2 /h. The measurement of the resistivity in the plateau region can be performed with very high precision. In the absence of scattering processes, at low temperatures and high fields, the classical Hall current is described by the fraction,
I x = B eV n y s( 1) where V y is the applied voltage, e the charge of the electron, B the magnetic field and n s the surface carrier density,where is a filling factor andis the degeneracy factor per unit area obtained from the shift Manuscript received March 30, 2013; revised May 30, 2013. Keshav N. Shrivastava is with the University of Malaya, Kuala Lumpur, and with the University of Hyderabad, Hyderabad 500046, India (e-mail: keshav1001@yahoo.com).of the oscillator wave function upon the application of magnetic field. Substituting (2) and (3) in (1) we find that,which means that the conductivity is given by, From (2) and (3) we find that,which means that the carrier density and the field are adjusted in such a way that the filling factor of the energy levels is an integer. From the occurrence of plateau in the Hall the value of h/e 2 . The plateaus in the Hall resistivity as a function of magnetic field were observed at many different fractions in addition to integer values.
II. HALDANE'S HIERARCHYHaldane [6] suggested that the fractional filling factors occur according to a hierarchy which is built from numbers m and p i (i=1, 2 or 3) determined from a continued fraction in which the number of terms determine the number of fractions. These numbers m and p i are not derived from any physical properties but are integers. Since m and p i are not related to t...