What is the meaning of the electron energy states in a hydrogen atom?

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Discussion Overview

The discussion centers on the meaning and interpretation of electron energy states in a hydrogen atom, specifically the notation used for these states such as 1s1/2, 2s1/2, 2p1/2, and 2p3/2. Participants explore the implications of this notation for the number of electrons and protons in various atomic configurations, including hydrogen and its ions.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about the notation, suggesting that 2s1/2 implies two electrons, which would indicate a hydrogen ion (H-).
  • Another participant clarifies that in a hydrogen atom, there is only one electron and that the states refer to the possible energy levels of this single electron.
  • A participant inquires about how to represent the states of H- or H2+, indicating a need for clarification on notation for multiple electrons and protons.
  • One participant corrects the misunderstanding regarding fractional subscripts, explaining that they relate to total angular momentum and not the number of electrons.
  • There is a reference to external resources that use similar notation, prompting questions about whether these states apply solely to hydrogen.
  • Another participant confirms that the notation is indeed for hydrogen and discusses the significance of the J subscript in determining the state.
  • A participant asks about the calculation of J for the 2p3/2 state, indicating interest in the underlying principles of the notation.
  • There is a mention of a table of atomic energy levels for neutral hydrogen, which includes explanations of the quantum numbers involved.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the interpretation of the notation, with some asserting it refers to a single electron while others question its implications for multi-electron systems. The discussion remains unresolved regarding the clarity of the notation and its application to different atomic configurations.

Contextual Notes

There are limitations in the understanding of the notation and its implications for different atomic states, particularly regarding the distinction between single and multiple electron systems. The discussion highlights the complexity of quantum state representation without resolving the ambiguities present.

zincshow
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You see hydrogen electron energy states labeled as 1s1/2, 2s1/2, 2p1/2 and 2p3/2.

My confussion may be with understanding the definitions, but does not the 2s1/2 state imply that there are 2 electrons around as the 1st s orbital is filled. But, by definition doesn't that mean you are dealing with h- acid? ie a hydrogen proton with 2 electrons. Same thing with 2p - doesn't it imply a second electron?
 
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No. In a hydrogen atom with one proton and one electron, the electron can be in any of the possible states. If it is in the 1s state, then the atom is in its ground state or unexcited state. If the electron is in any higher state, we are talking about an excited state that will eventually decay to the ground state. But there is still just one electron, or else we are not talking about a hydrogen atom.
 
Thank you, if these 1s1/2, 2s1/2, 2p1/2 and 2p3/2 all represent a state of a single electron and single proton, how (or can I?) represent the states of a single proton and two electrons (H-) or the states of two protons and a single electron (H2+)?
 
First, something's not right here. A configuration is given like so:
1s1 (1 electron in the 1s orbital, e.g. ground-state hydrogen),
1s2 (2 electrons in 1s, ground-state helium, or H-), 1s12s1 (1 electron in 1s, 1 in 2s, which could be triplet helium or an excited singlet helium, for instance).

You don't have fractional numbers when giving the orbital configuration. You must be confusing them with http://en.wikipedia.org/wiki/Term_symbol" , where a 1/2 subscript denotes a total angular momentum J=1/2. Term symbols give additional information, since as you can see from the above, the orbital configuration does not uniquely determine the state.
 
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zincshow said:
They use that type of notation at http://hyperphysics.phy-astr.gsu.edu/HBASE/quantum/lamb.html#c2
Are the states they talk about all 1 electron 1 proton combos?

Yes, it's all hydrogen. They're mixing it up a bit, putting J as a subscript as with term symbols. If you only have one electron, knowing J (and the orbital) is enough to determine the state completely.
 
From the wiki page you posted:

Calculate J as:
if less than half of the subshell is occupied, take the minimum value J = | L − S | ;
if more than half-filled, take the maximum value J = L + S;
if the subshell is half-filled, then L will be 0, so J = S.

Do you know the combination they use to get the 2P3/2?
 
alxm said:
Yes, it's all hydrogen. They're mixing it up a bit, putting J as a subscript as with term symbols. If you only have one electron, knowing J (and the orbital) is enough to determine the state completely.

Was that my imagination or did this post just change? Technical glitches? My memory must be going.
 
Here is a table of the atomic energy levels of neutral hydrogen:

http://physics.nist.gov/PhysRefData/Handbook/Tables/hydrogentable5.htm

The first column lists the configuration for a single atomic electron; 1s1/2, 2s1/2, 2p1/2, 2p3/2

the first # (before s or p) is n (the principal quantum number); the second number, listed in the third column, is J = L ± 1/2

L is orbital quantum number; s stands for L = 0, and p stands for L = 1

The energy levels are in inverse cm above the ground state. Divide level in cm-1 by 8061 to get electron volts.

Bob S
 

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