c16 JWBS043-Rogers September 13, 2010 11:28 Printer Name: Yet to Come
BREAKING DEGENERACY 261TABLE 16.1 The First Six Wave Functions for Hydrogen.ψ 1 s=1
π^1 /^2(
1
a) 3 / 2
e−Zr/aψ 2 s=
1
4 ·(2π)^1 /^2(
2 −
Zr
a) 3 / 2
e−Zr/^2 aψ 2 pz=
1
4 ·(2π)^1 /^2(
Z
a) 5 / 2
re−Zr/^2 acosθψ 2 px=1
4 ·(2π)^1 /^2(
Z
a) 5 / 2
re−Zr/^2 asinθcosφψ 2 py=
1
4 ·(2π)^1 /^2(
Z
a) 5 / 2
re−Zr/^2 asinθsinφψ 3 s=1
81(3π)^1 /^2(
Z
a) 3 / 2 (
27 − 18Zr
a
+ 2Z^2 r^2
a^2) 3 / 2
e−Zr/^3 aTABLE 16.2 The First ThreesWave Functions for
Hydrogen (Simplified Form).1 se−r
2 s ( 2 −r)e−r= 2 e−r−re−r
3 s(
27 − 18 r+ 2 r^2)
e−r= 27 e−r− 18 re−r+ 2 r^2 e−rR(r) 27 18 r 2 r
2
e
.63rl(r) 001015510R(r)l(r)r
FIGURE 16.8 Roots of the radial 3swave function of atomic hydrogen as a function of
distancer. Three nodes correspond to zeros of the function at aboutr= 2 , 7 ,and∼15. The
functionl(r) simply draws a horizontal line.