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Subatomic Physics

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464 Strong Interactions<br />

(c) The isospin.<br />

(d) The magnetic moment.<br />

(e) The quadrupole moment.<br />

14.17. Show that the ground state of a two-body system with central force must be<br />

an s state, that is, have orbital angular momentum zero.<br />

14.18. Deuteron—Theory. Treat the deuteron as a three-dimensional square well,<br />

with depth −V0 and range R.<br />

(a) Write the Schrödinger equation. Justify the value of the mass used in<br />

the Schrödinger equation.<br />

(b) Assume the ground state to be spherically symmetric. Find the groundstate<br />

wave function inside and outside the well. Determine the binding<br />

energy in terms of V0 and R. Show that B fixes only the product V0R 2 .<br />

(c) Sketch the ground-state wave function. Estimate the fraction of time<br />

that the neutron and proton spend outside each other’s force range.<br />

Why does the deuteron not disintegrate when the nucleons are outside<br />

the force range?<br />

14.19. Dineutrons and diprotons, that is, bound states consisting of two neutrons or<br />

two protons, are not stable. Explain why not in terms of what is known about<br />

the deuteron.<br />

14.20. At one time evidence for a bound state consisting of an antiproton and a<br />

neutron had been found, and the binding energy of this pn system was noted<br />

to be 83 MeV. [L. Gray, P. Hagerty, and T. Kalogeropoulos, Phys. Rev. Lett.<br />

26, 1491 (1971).] Describe this system by a square well with radius b =1.4fm<br />

and depth V0. Compute V0 and compare the numerical value with that of the<br />

deuteron.<br />

14.21. ∗ Antideuterons have been observed. How were they identified? [D. E. Dorfan<br />

et al., Phys. Rev. Lett. 14, 1003 (1965); T. Massam et al., Nuovo Cim. 39,<br />

10 (1965).]<br />

14.22. Verify that a cigar-shaped nucleus, with the nuclear symmetry axis parallel<br />

to the z axis, has a positive quadrupole moment.<br />

14.23. Show that the quadrupole moment of a nucleus with spin 1<br />

2 is zero.<br />

14.24. Show that the quadrupole moment of the deuteron is “small,” i.e., that it<br />

corresponds to a small deformation.

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