Why does the system has lower energy if its wave function is symmetric?

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Discussion Overview

The discussion revolves around the relationship between the symmetry of a wave function and the energy state of a quantum system, particularly in the context of the parity operator and the Hamiltonian. Participants explore whether symmetric wave functions are always associated with lower energy states compared to antisymmetric ones, referencing concepts such as the node-counting theorem.

Discussion Character

  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant questions the assumption that symmetric wave functions always correspond to lower energy states compared to antisymmetric wave functions, suggesting that this is not generally true.
  • Another participant introduces the "node-counting theorem," which posits that for bound states, the energy levels are ordered by the number of nodes in the wave function, implying that states with fewer nodes have lower energy.
  • It is noted that antisymmetric wave functions must have at least one node, while symmetric wave functions can have zero nodes, potentially leading to lower energy states for the latter.
  • A request for references or textbooks discussing the node-counting theorem is made, indicating a lack of accessible resources on the topic.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between wave function symmetry and energy states, with no consensus reached on whether symmetric wave functions always have lower energy than antisymmetric ones.

Contextual Notes

The discussion highlights the potential oversight of the node-counting theorem in quantum mechanics literature and the difficulty in finding references or proofs related to it.

xfshi2000
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Hi all:
I am confused that in general case, if [H,p]=0 (where H is Hamiltonian of system and P is parity operator), system wave function is either symmetric or antisymmetric. How do we know that system is in lower energy state if its wave function is symmetric by comparing that system is described by antisymmetric wave function? What I said is true or not? If true, what is physical significance behind?

thanks

xf
 
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xfshi2000 said:
Hi all:
I am confused that in general case, if [H,p]=0 (where H is Hamiltonian of system and P is parity operator), system wave function is either symmetric or antisymmetric. How do we know that system is in lower energy state if its wave function is symmetric by comparing that system is described by antisymmetric wave function? What I said is true or not? If true, what is physical significance behind?

thanks

xf

It is not generally true that symmetric (wrt parity) wave-functions always have lower energy than anti-symmetric ones. However, there is a "node-counting theorem" (at least for bound states) which basically states the energies of the states are ordered according to the number of nodes in the wave-function. I.e. a state with a wave-function with n nodes has a lower energy than a state with n+1 nodes and so on. Since any anti-symmetric wave-function must have at least one node there usually (always?) exists a symmetric wave-function with zero nodes which has the lowest energy.

At least this is what I can remember, please correct me if I am wrong (I'm too lazy to look it up)
 
Last edited:
jensa said:
It is not generally true that symmetric (wrt parity) wave-functions always have lower energy than anti-symmetric ones. However, there is a "node-counting theorem" (at least for bound states) which basically states the energies of the states are ordered according to the number of nodes in the wave-function. I.e. a state with a wave-function with n nodes has a lower energy than a state with n+1 nodes and so on. Since any anti-symmetric wave-function must have at least one node there usually (always?) exists a symmetric wave-function with zero nodes which has the lowest energy.

At least this is what I can remember, please correct me if I am wrong (I'm too lazy to look it up)



thanks for your answer. By the way, where can I find node-counting theorem? which textbook talk about this theorem?
 
Unfortunately I don't know a good reference discussing this. It seems to be very overlooked in QM books. Probably it is more likely to find this in some book on differential equations. Some googling led me to this http://www.emis.de/journals/AM/98-1/kusano.ps" . Not sure if it helps you.

Many people refer to this theorem without giving any references. I remember having a very hard time finding a proof of this theorem and now I don't remember where I found it. Good luck!
 
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