Orthohelium Alternative Electron Configuration

In the previous post we let RealQM compute the first line in the spectrum of Helium from ground state as Orthohelium assuming that one electron is excited from 1S to 2S and obtained an energy of 0.728 Hartree in accordance with observation as a line easy to observe as the difference between $-2.175$ and $-2.903$ Hartree. 

We compare assuming instead excitation to the 2nd eigenvalue of Schrödinger's equation for Helium in the form given by RealQM. You can run the code here. We obtain the same energy of 0.728 Hartree in agreement with observation. 

RealQM thus gives the same first line in the spectrum of Helium with two different electron configurations.

Note that in Standard Quantum Mechanics StdQM the first exited states of Helium comes on two forms, as Orthohelium with the the two electrons having the same spin as a triple state, and Parahelium with different spin as a singlet state. RealQM corresponds to Orthohelium since in RealQ there is only same spin. 

Orthohelium is much easier to observe (more stable) than Parahelium and so appears to represent more solid physics. 

The fact that RealQM gives correct 1st line of Helium as Orthohelium with two different electron configurations is another piece of evidence that RealQM captures physics. Both configurations have in the RealQM electric dipoles varying over time and so radiate, with the 1S to 2S weaker.

The electron configuration of Orthohelium in StdQM is very complex, and as such probably with less physics. 

Recall that DFT being focussed on ground states has to struggle with excited states in heavy software. It may show to be remarkable that the 3-line code of RealQM can outperform DFT.

 

RealQM Spectrum of Helium: 1st Excited State as Orthohelium

We now explore the spectrum of Helium delivered by RealQM. The spectrum of an atom primarily reflects energy differences between the ground state and excited states, but also between excited states.

Standard Quantum Mechanics StdQM presents the first exited state of the Helium atom with two electrons to be a singlet state with the two electrons having opposite spin named Parahelium, but there is also a triplet state with the electrons having same spin named Orthohelium. 

The first line in the spectrum of Helium (smallest energy jump from ground state) corresponding to an energy of $-2.175$ Hartree is that of Orthohelium, compared to $-2.903$ for the ground state, while Parahelium has 0.03 higher energy of $-2.145$ Hartree. 

Let us see what RealQM delivers. Since in RealQM all electrons have the same spin, RealQM connects to Orthohelium giving the first line in the spectrum. We let RealQM model this state with one electron around the kernel and the other electron in an excited state outside. You can here run the code to find that RealQM gives an energy of $-2.175\pm 0.005$ Hartree depending on iteration stop criterion. 

We thus see that RealQM gives a result in agreement with observation of the 1st line in the spectrum of Helium in the form of a very simple arrangement of the two electrons: An inner electron around the kernel and an outer electron around the kernel + inner electron. Run code to see. The corresponding triplet state of StdQM is very complicated:

Orthohelium corresponds to the first line in the Lyman series for Hydrogen (with drop of wave length from 122 nm to 62.6 nm), with details on further lines to come.

PS The ground state of Helium with its two electrons overlapping with opposite spin in StdQM, is in RealQM modeled with the electrons split into halfspaces without overlapping. See this code. The transition to excited state in RealQM is thus from a state of half space split electrons into a state with spherically symmetric electrons, one inner and one outer, which appears to require a quite precise excitation input.

Helium/Neon 1st Excited RealQM

We now let RealQM compute the first excited state of Helium with one electron moving from 1st shell to 2nd shell thus giving the excited state a 1+1 configuration. We get the following results: 

• Excited state with 1st el 1st shell, 2nd el 2nd shell = -2.16 (ref -2.145) (code)
• Reference with same code but only 1 el                  = -2.00  (ref -2.000) (code)
• Reference Helium ground state                                = -2.903
• Excitation energy                                                      = 0.758  Hartree    (20.61 eV)

We see good agreement. The difference between RealQM and stdQM is that electrons do not overlap in RealQM and meet with homogeneous Neumann condition (zero flux) and charge density continuity, while in stdQM in the 1s2s configuration the outer 2s electron overlaps with the inner 1s electron. 

Spin plays no role in RealQM, while in stdQM the two electrons are assumed to have different spin (whatever the physics of spin may be). 

For Neon RealQM gives about the same excitation energy as the difference between a 2+4+4 and 2+4+3+1 configuration with 1 electron in a new outer shell (code), in accordance with observation (0.8 Hartree).