JMP  Vol.4 No.9 , September 2013
Theory of Deuteron and MCPE

All the experimental values of the Deuteron nucleus except the magnetic moment are theoretically derived using the ordinary methods of quantum mechanics along with the morphed gravitational potential energy. To convince that the potential energy function used is indeed the right one, it is applied to determine the energy spectrums of the nuclei: 1) Triton, 2) helium-3, 3) lithium-7, 4) Beryllium-9, and 5) Beryllium-8. The Morphed Coulomb Potential Energy (MCPE) is also obtained. With the help of MCPE and the gravitational potential energy of the electron, the charge quantum number is obtained. For galaxies, the two dominant forces that are responsible for the expansion, contraction or stationary state of the universe are obtained.

Cite this paper
C. Chandraraju, "Theory of Deuteron and MCPE," Journal of Modern Physics, Vol. 4 No. 9, 2013, pp. 1180-1184. doi: 10.4236/jmp.2013.49159.
[1]   H. A. Enge, “Introduction to Nuclear Physics,” Addison-Wesley, Ontario, 1966.

[2]   C. C. Raju, Journal of Modern Physics, Vol. 4, 2013, pp. 459-462.

[3]   C. C. Raju, Journal of Nuclear and Particle Physics, Vol. 3, 2013, pp. 25-28.

[4]   C. C. Raju, International Journal of Theoretical Physics, Vol. 36, 1997, pp. 2937-2939. doi:10.1007/BF02435719

[5]   L. I. Schiff, “Quantum Mechanics,” McGraw-Hill, New York, 1955.

[6]   G. Baym, “Lectures on Quantum Mechanics,” W.A. Benzamin, New York, 1969.

[7]   E. E. Anderson, “Modern Physics and Quantum Mechanics,” W.B. Sanders, Toronto, 1971.

[8]   R. R. Roy and B. P. Nigam, “Nuclear Physics,” WileyEastern, Delhi, 1979.

[9]   R. J. Bin-Stoyle, “Nuclear and Particle Physics,” Thompson, India, 1991.

[10]   M. L. Pandya and R. P. S.Yadav, “Elements of Nuclear Physics,” KedarNath Ram, Meerat, 1994.

[11]   S. S. M. Wong, “Introductory Nuclear Physics,” Prentice Hall, India, 1996.