Exercise 81 obtained formulas for hydrogen like atoms in which the nucleus is not assumed infinite, as in the chapter, but is of mass m1, whilem2is the mass of the orbiting negative charge. In positronium, an electron orbits a single positive charge, as in hydrogen, but one whose mass is the same as that of the electron -- a positron. Obtain numerical values of the ground state energy and “Bohr radius” of positronium.

Short Answer

Expert verified

(a) The ground State energy of positronium is -6.8 eV .

(b) Bohr radius of positronium is 0.106 nm .

Step by step solution

01

Energy of ground-state of positronium

As you know from that, the ground state energy is,

Eground=Z2μmE1n2

Where, zis the atomic number, μis the Reduced mass, n is the principal quantum number, m is the mass, E1is the Energy of ground state of hydrogen atom.

You also know that the electron and positron have same masses.

Hence, the reduced mass will be half of the mass of electron

Eground=Z2μmE1n2=1212mmE112=-6.8eV

Hence, ground state energy of the positronium is -6.8 eV .

02

Bohr Radius of the positronium

As you know that,

The Bohr’s Radius

rn=mzμa0

Where, a0is radius of hydrogen atom

If the reduced mass will be half of the mass of electron,

rn=mZμa0=mZ12ma0=0.106nm

Hence, Bohr Radius of the positronium is 0.106 nm.

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Most popular questions from this chapter

At heart, momentum conservation is related to the universe being "translationally invariant," meaning that it is the same if you shift your coordinates to the right or left. Angular momentum relates to rotational invariance. Use these ideas to explain at least some of the differences between the physical properties quantized in the cubic three-dimensional box versus the hydrogen atom.

Using the functions given in Table 7.4, verify that for the more circular electron orbit in hydrogen (i.e.,l=n-1), the radial probability is of the form

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Show that the most probable radius is given by

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Question: A particle is trapped in a spherical infinite well. The potential energy is 0for r < a and infinite for r > a . Which, if any, quantization conditions would you expect it to share with hydrogen, and why?

When applying quantum mechanics, we often concentrate on states that qualify as “orthonormal”, The main point is this. If we evaluate a probability integral over all space of ϕ1*ϕ1or of ϕ2*ϕ2, we get 1 (unsurprisingly), but if we evaluate such an integral forϕ1*ϕ2orϕ2*ϕ1 we get 0. This happens to be true for all systems where we have tabulated or actually derived sets of wave functions (e.g., the particle in a box, the harmonic oscillator, and the hydrogen atom). By integrating overall space, show that expression (7-44) is not normalized unless a factor of 1/2is included with the probability.

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