Using Egs=-79.0eV for the ground state energy of helium, calculate the ionization energy (the energy required to remove just one electron). Hint: First calculate the ground state energy of the helium ion, He+, with a single electron orbiting the nucleus; then subtract the two energies.

Short Answer

Expert verified

The first ionization energy is 24.6eV.

Step by step solution

01

Definition of the hyperfine harmonic oscillator

A harmonic oscillator is a system that experiences a restoring forceFproportionate to the displacement xwhen it is moved from its equilibrium position, where k is a positive constant.

02

The ionization energy

Subtract Helium's ground state energy from its first excited state yields the first ionization energy (energy necessary to remove one electron).

The energy of the Helium ion'sHe+ground state is equal to the energy of the first excited state.

So, calculate the ground state energy ofHe+as:

He+ is a Hydrogen like atom. It contains just one electron but two protons in its nucleus, which indicates it has only one electron.

Hydrogen atom energy,

EH=-13.6eVZ2n2

ForHydrogen ground state n = 1 , and Z = 1.

For helium, Z = 2, then the expression will be :

EHe=-13.6eV2212EHe=-54.4eV

Ground state energy for helium is:

Egs=-79.0eV

SubtractingEHe andEgs ground state energy as:

Ejoin=-54eV--79eV=24.6eV

Thus, the first ionization energy is 24.6eV.

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Most popular questions from this chapter

Use a gaussian trial function (Equation 7.2) to obtain the lowest upper bound you can on the ground state energy of (a) the linear potential V(x)=α|x| (b) the quartic potential:V(x)=αx4

Find the best bound on Egsfor the delta-function potentialV(x)=-αδ(x), using a triangular trial function (Equation 7.10, only centered at the origin). This time a is an adjustable parameter.

As an explicit example of the method developed inProblem 7.15, consider an electron at rest in a uniform magnetic field B=B2kfor which the Hamiltonian is (Equation 4.158):

H=-γB (4.158).

H0=eBzmSz (7.57).

The eigenspinors, xaarelocalid="1655969802629" xb,andthecorrespondingenergies,EaandEb,aregiven in Equation 4.161. Now we turn on a perturbation, in the form of a uniform field in the x direction:

{x+,withenergyE+=-γB0ħ/2x-,withenergyE-=+-γB0ħ/2 (4.161).

H'=eBxmSx (7.58).

(a) Find the matrix elements of H′, and confirm that they have the structure of Equation 7.55. What is h?

(b) Using your result inProblem 7.15(b), find the new ground state energy, in second-order perturbation theory.

(c) Using your result inProblem 7.15(c), find the variation principle bound on the ground state energy.

Quantum dots. Consider a particle constrained to move in two dimensions in the cross-shaped region.The “arms” of the cross continue out to infinity. The potential is zero within the cross, and infinite in the shaded areas outside. Surprisingly, this configuration admits a positive-energy bound state

(a) Show that the lowest energy that can propagate off to infinity is

Ethreshold=π2h28ma2

any solution with energy less than that has to be a bound state. Hint: Go way out one arm (say xa), and solve the Schrödinger equation by separation of variables; if the wave function propagates out to infinity, the dependence on x must take the formexp(ikxx)withkx>0

(b) Now use the variation principle to show that the ground state has energy less than Ethreshold. Use the following trial wave function (suggested by Jim Mc Tavish):

ψ(x,y)=A{cos(πx/2a)+cos(πy/2a)e-αxaandyacos(πx/2a)e-αy/axaandy>acos(πy/2a)e-αy/ax.aandya0elsewhere

Normalize it to determine A, and calculate the expectation value of H.
Answer:

<H>=h2ma2[π28-1-(α/4)1+(8/π2)+(1/2α)]

Now minimize with respect to α, and show that the result is less thanEthreshold. Hint: Take full advantage of the symmetry of the problem— you only need to integrate over 1/8 of the open region, since the other seven integrals will be the same. Note however that whereas the trial wave function is continuous, its derivatives are not—there are “roof-lines” at the joins, and you will need to exploit the technique of Example 8.3.

Find the lowest bound on the ground state of hydrogen you can get using a Gaussian trial wave function

ψ(r)=Ae-br2,

where A is determined by normalization and b is an adjustable parameter. Answer-11.5eV

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