Appendix A
The Hyperfine Addition to the Hydrogen Fine Structure
Emission Spectra for Orbit Shells 1 to 3 to Orbit Shells 1 and 2.
This Appendix presents calculated emission/absorption spectra for the first
3 ® 2 orbit shells of hydrogen. They include the effects of
relativistic mass correction, magnetic dipole coupling, the Lamb Shift and
hyperfine variations. The spectra are calculated using the formula
|
l( n )( m ) = |
hc ( Eor( m ) -Eor( n ) )
|
|
| (A.1) |
together with the Selection Rules.
For spectra in which the wavelength is greater than 2000Å, (A.1) is
divided by Pair, the refractive index of air. In (A.1),
Eor(# ) is given by (2.7) within which nj is given by [1],
Eq.(3.20), ensp and pnsp= ± 1/ 2 , and nf * is
increased by unity in the ground state orbitals when ensp =
- 1/ 2. Rhy is determined from
the generalised relationship
|
Rhy = |
cR¥ { Zmp +( J-Z )mN }
{ Zmp +( J-Z )mN +me }
|
|
| (A.2) |
In this and the other relationships referred to, the values of the
parameters used are as shown in the following Table A.1.
| Parameter |
Name |
Value |
Units |
Ref. |
| h |
Planck's Constant |
6.6260693E-27 |
erg secs |
[7] |
| c |
Velocity of Light in Vacuum |
2.99792458E+10 |
cm/sec |
[7] |
| Rhy |
Rydberg's Constant for Hydrogen |
See (A.2) |
sec-1 |
- |
| R¥ |
Rydberg's Constant for Infinite Nuclear Mass |
1.09737316E+5 |
cm-1 |
[7] |
| Z |
Atomic Number |
1 for Hydrogen |
- |
- |
| J |
Mass Number |
1 for Hydrogen |
- |
- |
| mp |
Proton Mass |
1.67262171E-24 |
g sec2/cm |
[7] |
| mN |
Neutron Mass |
1.6749278E-24 |
g sec2/cm |
[7] |
| me |
Electron Mass |
9.10913826E-28 |
g sec2/cm |
[7] |
| e |
Electron/Proton Charge |
-/+ 4.8032044E-10 |
esu |
See Note 1 |
| gp |
Proton magnetic moment constant of proportionality |
2.79275 |
- |
[4] |
| dp |
Proton spin dipole magnetisation constant of proportionality |
3.3548035 |
- |
[1] |
| Pair |
Refractive Index of Air |
See Table A.2 |
- |
Calculated from [8] |
Table A1 - Parameter Values.
Note 1:- Calculated from e = 1.60217653E-20 abcoulombs x c.
Also the following factors have been used to convert energy from ergs to
cm-1.
Joules = 1E-7 ergs; eV = 6.24150948E+18 Joules cm-1 = 8.065541E+3 eV
The values of Pair used, are shown in the following table, as
calculated from [8].
| Wavelength |
Pair |
| 3889 | 1.000283373820 |
| 3970 | 1.000282912237 |
| 4101 | 1.000282223812 |
| 4340 | 1.000281143049 |
| 4861 | 1.000279342657 |
| 6562 | 1.000276235841 |
| 9545 | 1.000274299185 |
| 10049 | 1.000274132698 |
| 10938 | 1.000273891534 |
| 12817 | 1.000273537699 |
| 18751 | 1.000273036604 |
| 19445 | 1.000273006377 |
| 21654 | 1.000272927044 |
| 26251 | 1.000272823218 |
| 37395 | 1.000272707134 |
| 40510 | 1.000272691823 |
| 46525 | 1.000272669382 |
| 74577 | 1.000272628864 |
| 75003 | 1.000272628349 |
| 123682 | 1.000272605744 |
| 190568 | 1.000272607289 |
| > 200000 | 1.000272526299 |
Table A.2 - Pair vs Wavelength.
The only apparent anomaly in this table is that the values for l =
123,682Å and 190,568Å appear reversed.
The calculated orbital energy levels and transition emission spectra are
shown below in Table A.3 expressed as wavelengths in Ångstroms for
inter-shell transitions, and cm for intra-shell transitions.
| Orbital Energy - EOR |
To ® From ¯ |
n |
1 |
2 |
3 |
| n*f |
0.5 |
1.5 |
1.5 |
0.5 |
1.5 |
1.5 |
0.5 |
0.5 |
1.5 |
1.5 |
1.5 |
1.5 |
0.5 |
0.5 |
2.5 |
2.5 |
1.5 |
1.5 |
2.5 |
| ergs |
cm-1 |
n |
n*f |
ensp |
pnsp |
nf | Term |
s(+) | sh1(-) |
sh2(-) |
sh3(+) |
p(-) |
ph(-) |
s(+) |
sh(+) |
p(+) |
ph(+) |
p(-) |
ph(-) |
s(+) |
sh(+) |
d(-) |
dh(-) |
p(+) |
ph1(+) |
d(+) |
| -2.1787E-11 |
0.0000 |
1 |
0.5 |
0.5 |
0.5 |
1.5 |
s(+) |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| -2.1787E-11 |
0.0275 |
1.5 |
-0.5 |
-0.5 |
0.5 |
sh1(-) |
N.P. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| -2.1787E-11 |
0.0474 |
1.5 |
-0.5 |
0.5 |
1.5 |
sh2(-) |
21.1061 |
N.P. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| -2.1787E-11 |
0.0596 |
0.5 |
0.5 |
-0.5 |
0.5 |
sh(+) |
N.P. |
N.P. |
N.P. |
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
| -5.4468E-12 |
82258.881 |
2 |
1.5 |
-0.5 |
-0.5 |
0.5 |
p(-) |
1215.6737 |
N.P. |
N.P. |
1215.6746 |
|
|
D.Z. |
|
|
|
|
|
|
|
|
|
|
|
|
| -5.4468E-12 |
82258.884 |
1.5 |
-0.5 |
0.5 |
1.5 |
ph(-) |
1215.6736 |
N.P. |
N.P. |
N.P. |
N.P. |
|
|
D.Z. |
|
|
|
|
|
|
|
|
|
|
|
| -5.4468E-12 |
82258.917 |
0.5 |
0.5 |
0.5 |
1.5 |
s(+) |
N.P. |
1215.6736 |
1215.6739 |
N.P. |
D.Z. |
N.P. |
|
|
|
|
|
|
|
|
|
|
|
|
|
| -5.4468E-12 |
82258.924 |
0.5 |
0.5 |
-0.5 |
0.5 |
sh(+) |
N.P. |
1215.6735 |
1215.6737 |
N.P. |
N.P. |
D.Z. |
N.P. |
|
|
|
|
|
|
|
|
|
|
|
|
| -5.4467E-12 |
82259.247 |
1.5 |
0.5 |
0.5 |
2.5 |
p(+) |
1215.6683 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
|
|
|
|
|
|
|
|
|
|
|
| -5.4467E-12 |
82259.248 |
1.5 |
0.5 |
-0.5 |
1.5 |
ph(+) |
1215.6683 |
N.P. |
N.P. |
1215.6691 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
|
|
|
|
|
|
|
|
|
|
|
| -2.4208E-12 |
97492.165 |
3 |
1.5 |
-0.5 |
-0.5 |
0.5 |
p(-) |
1025.7230 |
N.P. |
N.P. |
1025.7236 |
N.P. |
N.P. |
6562.773 |
6562.776 |
N.P. |
N.P. |
|
|
D.Z. |
|
|
|
|
|
|
| -2.4208E-12 |
97492.165 |
1.5 |
-0.5 |
0.5 |
1.5 |
ph(-) |
1025.7230 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
6562.772 |
N.P. |
N.P. |
N.P. |
N.P. |
|
|
D.Z. |
|
|
|
|
|
| -2.4208E-12 |
97492.174 |
0.5 |
0.5 |
0.5 |
1.5 |
s(+) |
N.P. |
1025.7232 |
1025.7234 |
N.P. |
6562.753 |
6562.754 |
N.P. |
N.P. |
6562.911 |
N.P. |
D.Z. |
N.P. |
|
|
|
|
|
|
|
| -2.4208E-12 |
97492.177 |
0.5 |
0.5 |
-0.5 |
0.5 |
sh(+) |
1025.7232 |
1025.7234 |
N.P. |
N.P. |
6562.752 |
6562.753 |
N.P. |
N.P. |
N.P. |
6562.910 |
N.P. |
D.Z. |
N.P. |
|
|
|
|
|
|
| -2.4208E-12 |
97492.270 |
2.5 |
-0.5 |
-0.5 |
1.5 |
d(-) |
N.P. |
1025.7222 |
1025.7224 |
N.P. |
6562.712 |
6562.713 |
N.P. |
N.P. |
6562.870 |
6562.870 |
N.P. |
N.P. |
N.P. |
N.P. |
|
|
D.Z. |
|
|
| -2.4208E-12 |
97492.271 |
2.5 |
-0.5 |
0.5 |
2.5 |
dh(-) |
N.P. |
N.P. |
1025.7224 |
N.P. |
N.P. |
6562.713 |
N.P. |
N.P. |
6562.869 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
|
|
D.Z. |
|
| -2.4208E-12 |
97492.272 |
1.5 |
0.5 |
0.5 |
2.5 |
p(+) |
1025.7219 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
6562.726 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
D.Z. |
N.P. |
|
|
|
| -2.4208E-12 |
97492.272 |
1.5 |
0.5 |
-0.5 |
1.5 |
ph(+) |
1025.7219 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
6562.726 |
6562.730 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
D.Z. |
N.P. |
|
|
| -2.4208E-12 |
97492.306 |
2.5 |
0.5 |
0.5 |
3.5 |
d(+) |
N.P. |
N.P. |
N.P. |
1025.7225 |
N.P. |
N.P. |
N.P. |
N.P. |
6562.854 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
|
| -2.4208E-12 |
97492.306 |
2.5 |
0.5 |
-0.5 |
2.5 |
dh(+) |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
6562.854 |
6562.854 |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
N.P. |
Table A.3 - Hyperfine and Normal Spectral Wavelengths
for Transitions from Cells 1 to 3, to Cells 1 & 2.
The spreadsheet that produced Table A.3 is available for download as:-
Hydrogen Spectra
Three other sheets are incorporated in this spreadsheet.
(i) The revised hydrogen fine structure orbital energy levels and emission
spectra and other data, (See Appendix B).
(ii) The relevant orbital energy levels and spectral wavelengths from [6].
(iii) The differences in the values in (i) and (ii).
Note that this spreadsheet is a working document that has "evolved" as the
development in this series of papers has progressed. Presentation has not
therefore been aesthetically optimised.
P6 Version 1.0.0
Ó
P.G.Bass, August 2007
|