Presentation is loading. Please wait.

Presentation is loading. Please wait.

Hydrogen relativistic effects II

Similar presentations


Presentation on theme: "Hydrogen relativistic effects II"β€” Presentation transcript:

1 Hydrogen relativistic effects II
a. relativistic mass effect Total Energy 𝑯= ( 𝒑 𝟐 𝒄 𝟐 + π’Ž 𝟐 𝒄 πŸ’ ) 𝟏/𝟐 + 𝑽(𝒓) Kinetic Energy 𝑬 π’Œπ’Šπ’ = ( 𝒑 𝟐 𝒄 𝟐 + π’Ž 𝟐 𝒄 πŸ’ ) 𝟏/𝟐 βˆ’ π’Ž 𝒄 𝟐 ~ 𝒑 𝟐 πŸπ’Ž βˆ’ 𝟏 πŸ– 𝒑 πŸ’ π’Ž πŸ‘ 𝒄 𝟐 +… Correction Term βˆ’ 𝟏 πŸ– 𝒑 πŸ’ π’Ž πŸ‘ 𝒄 𝟐 =βˆ’ 𝟏 πŸπ’Ž 𝒄 𝟐 𝒑 𝟐 πŸπ’Ž 𝟐 =βˆ’ 𝟏 πŸπ’Ž 𝒄 𝟐 𝑬 π’Œπ’Šπ’ 𝟎 𝟐 =βˆ’ 𝟏 πŸπ’Ž 𝒄 𝟐 𝑬 𝒏 βˆ’π‘½ 𝒓 𝟐

2 = βˆ’ 𝟏 πŸπ’Ž 𝒄 𝟐 𝑬 𝒏 𝟐 βˆ’πŸ 𝑬 𝒏 βˆ’ 𝒁 𝒆 𝟐 πŸ’π… 𝜺 𝟎 𝒓 + 𝒁 𝟐 𝒆 πŸ’ πŸ’π… 𝜺 𝟎 𝟐 𝒓 𝟐
Energy Shift βˆ† 𝑬′ 𝒏 =βˆ’ 𝟏 πŸπ’Ž 𝒄 𝟐 𝑬 𝒏 βˆ’π‘½ 𝒓 𝟐 = βˆ’ 𝟏 πŸπ’Ž 𝒄 𝟐 𝑬 𝒏 𝟐 βˆ’πŸ 𝑬 𝒏 βˆ’ 𝒁 𝒆 𝟐 πŸ’π… 𝜺 𝟎 𝒓 + 𝒁 𝟐 𝒆 πŸ’ πŸ’π… 𝜺 𝟎 𝟐 𝒓 𝟐 with 𝟏 𝒓 = 𝟏 𝒏 𝟐 βˆ™ 𝒁 𝒂 𝟎 , 𝟏 𝒓 𝟐 = 𝟏 β„“+ 𝟏 𝟐 𝒏 πŸ‘ 𝒁 𝒂 𝟎 𝟐 , 𝑬 𝒏 =βˆ’ 𝟏 πŸ’π… 𝜺 𝟎 βˆ™ 𝒁 𝟐 𝒆 𝟐 𝟐 𝒂 𝟎 βˆ™ 𝟏 𝒏 𝟐 βˆ† 𝑬 𝒏 β€² =βˆ’ 𝜢 𝟐 𝒁 𝟐 𝒏 𝟐 𝑬 𝒏 πŸ‘ πŸ’ βˆ’ 𝒏 β„“+𝟏/𝟐 The relativistic mass effect depends on l and n. It is ~ 𝜢 𝟐 𝒁 𝟐 or ~ 𝑣 2 / 𝑐 2 smaller than 𝑬 𝒏 .Therefore larger for heavy atoms with large

3 Spin-orbit interaction
Correction term depends on spin The electron moves in the electric of 𝐸 field of the nucleus .Therefore, in the rest frame of the electron exists a magnetic field 𝐸 = 1 𝐢 2 𝑣 Γ— 𝐸 with The name spin-orbit is due to π‘™βˆ™π‘  Energy shift with <π‘™βˆ™π‘ > is not diagonal in 𝑙, π‘š 𝑙 ,𝑠, π‘š 𝑠 ,but in 𝑗, π‘š 𝑗 , 𝑙 2 , 𝑠 2

4 New coupled total angular momentum j
𝑗=β„“+𝑠 𝑗 2 = β„“ 2 +2β„“βˆ™π‘ + 𝑠 2 β„“βˆ™π‘ = 1 2 ( 𝑗 2 βˆ’ β„“ 2 βˆ’ 𝑠 2 ) β„“βˆ™π‘  = β„Ž 2 2 {𝑗 𝑗+1 βˆ’β„“ β„“+1 βˆ’π‘  𝑠+1 } The relativistic mass effect and the spin-orbit interaction can be put together

5 c.Darwin-Term βˆ’ β„Ž 2 4 π‘š 2 𝑐 2 π‘’π‘¬βˆ™π›» β„“=0
βˆ’ β„Ž 2 4 π‘š 2 𝑐 2 π‘’π‘¬βˆ™π›» β„“=0 This term has no classical analogue βˆ†πΈβ€²β€²β€² = πœ‹ β„Ž 2 2 π‘š 2 𝑐 2 𝑍 𝑒 2 4πœ‹ πœ€ 0 Ξ¨ 0 2 =βˆ’ Ξ± 2 𝑍 2 𝑛 2 𝐸 𝑛 𝑛

6 Total relativistic energy shift note: for l=0 there is no spin –orbit interaction, put together in one expression which is also valid for l=0 we have βˆ†πΈ=βˆ† 𝐸 β€² +βˆ† 𝐸 β€²β€² +βˆ† 𝐸 β€²β€²β€² =βˆ’ 𝛼 2 𝑍 2 𝑛 2 𝐸 𝑛 βˆ’ 𝑛 𝑗+1/2 𝑗=β„“Β± 1 2 note: Total energy shift does not depend on l(even though the individual terms do). Therefore terms with the same j are degenerate. The lambshift(discussed next removes this degeneracy

7 Fine-structure of the n=2 and n=3 levels of hydrogen according to the Dirac theory for the Balmer – Ξ± line at 656 nm (red)

8

9 Fine-structure of the n=2 terms with Lamb-shift note: degeneracy in 𝑙 is removed The indicated transition frequency is 1058 MHz

10 Lamb-shift The electromagnetic field is quantized in QED
Lamb-shift The electromagnetic field is quantized in QED. A quantum mechanical harmonic oscillator has fluctuations in the ground state=Zitterbewegung =vacuum fluctuations ,

11 g-factor of the electron


Download ppt "Hydrogen relativistic effects II"

Similar presentations


Ads by Google