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     Introduction  - part III     
 
      and

   The Physics of Helium        (starts below)


   More facts about the physics of the simplest of the atoms - hydrogen - and hydrogen-like ions

      0010.png

       0010.png


Hydrogen spectrum  - an exercise - fill in the energies, L-values, N-values
 
      0013_hydrospec_larg.png

       0013_hydrospec_larg.png

 
Hydrogen spectrum  - an exercise - energies, L-values, N-values
 
      0015_hydrospec_larg-1.png

       0015_hydrospec_larg-1.png


Hydrogen spectrum  - an exercise - can be continued

      0017_hydrospec_larg-2.png

       0017_hydrospec_larg-2.png


Radial functions of hydrogen (-like) atom (ion)

      0020_Psi_hydrogen_citizendum.png

       0020_Psi_hydrogen_citizendum.png

 
Spherical harmonics L=0  and  L=1
 
      0025_Y_1_and_0_all_wiki1.png

       0025_Y_1_and_0_all_wiki1.png

 
Spherical harmonics L=2
 
      0029_Y_2_all_wiki.png

       0029_Y_2_all_wiki.png

 
Spherical harmonics L=3
 
      0033_Y_3_all_wiki-1.png

       0033_Y_3_all_wiki-1.png

Helium atom - Starting the first Regular Topic

The model of helium atom Coordinate system - Hamiltonian
    What is potential energy ( reminder on classical mechanics )   ( later on: electron indistinguishable = identical )
      0050_Starting_Helium_Hamiltonian.png

       
0050_Starting_Helium_Hamiltonian.png


Helium atom - but also other ions with only 2 electrons remaining
      singly ionized Li, doubly ionized Be, triply ionized B, and finally - 4 times ionized carbon ....   etc up to U 90+

      0055.png

       0055.png


Two spectra of helium atom - parahelium and orthohelium   -  energy scale "interrupted"
    ( some might have believed there are two types of Helium atom - no just two quite different states
                              these two states are the states of the spin - this is a very important feature )

      0056_Para_Ortho_helium.png

       0056_Para_Ortho_helium.png


Two spectra of helium atom - parahelium and orthohelium   -  energies correct

      0057_Para_Ortho_helium_overview.png

       0057_Para_Ortho_helium_overview.png

 
               ( later on: electron indistinguishable = identical )
Symmetry requirement - eliminates "unnecessary parts of coordinate space (one possible perspactive)
Rotation of a "stick" with two "identical" ends - only half of the 360 degrees is the dynamical variable
      for the whole circle (one end)  2 pi is the region   -  Q.M. continuity -> periodicity on 2 pi - allows only integer m in exp( i m phi)
      for our stick  - periodicity on pi ( not 2 pi ) - thus only even integer values m allowed in
exp( i m phi)

      0060_Symmetry-eliminates_coordinate_spaces.png

       0060_Symmetry-eliminates_coordinate_spaces.png


Historically - Pauli principle first observation
Exchange symmetry used to put Pauli principle into a mathematical structure
   - the necessary symmetry is  - antisymmetry  - minus sign by exchange  - leads to ZERO function for the same "orbital"

      0070_Pauli_Principle.png

       0070_Pauli_Principle.png


The next element is the electron spin

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