Is the Spin Orbit Hamiltonian really Hermitian?

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Discussion Overview

The discussion centers on the Hermiticity of the spin-orbit Hamiltonian, particularly in the context of a two-dimensional system with an external electric field. Participants explore the implications of non-commuting operators and the conditions under which the Hamiltonian may or may not be Hermitian.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant presents the spin-orbit Hamiltonian in a specific form and questions its Hermiticity due to the non-commutation of the electric field and momentum operators.
  • Another participant argues that in a spherically symmetric potential, the spin-orbit Hamiltonian is Hermitian because the components commute.
  • A participant raises a concern about the applicability of the Hamiltonian in systems with external electric fields that lack spherical symmetry.
  • There is a suggestion that the expression E x p could be Hermitian if E is the gradient of a potential, implying a specific condition for Hermiticity.
  • A participant discusses the evaluation of the electric field operator in a discrete representation and questions how to properly evaluate it in relation to the position kets.
  • A later post references a previous discussion about the spin-orbit Hamiltonian, indicating that the cited form does not yield a self-adjoint Hamiltonian and is limited to low-order perturbational corrections.
  • Another participant seeks clarification on the applicability of the Hamiltonian in quantum transport problems and questions whether a specific adjustment involving the Hermitian adjoint is necessary.

Areas of Agreement / Disagreement

Participants express differing views on the Hermiticity of the spin-orbit Hamiltonian, with some asserting it is Hermitian under certain conditions while others argue that it may not be in specific contexts, particularly with external electric fields. The discussion remains unresolved regarding the general applicability of the Hamiltonian.

Contextual Notes

Participants highlight limitations related to the assumptions of spherical symmetry and the specific conditions under which the Hamiltonian is considered Hermitian. There are unresolved questions regarding the evaluation of operators in a discrete representation.

maverick280857
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The regular spin orbit Hamiltonian is

[tex]H_{SO} = \frac{q\hbar}{4 m^2 c^2}\sigma\cdot(\textbf{E}\times \textbf{p})[/tex]

If I consider a 2D system where E = E(x,y) and p is treated as an operator, i.e. [itex]\hat{p} = \hat{i}p_x + \hat{j}p_y[/itex] then, clearly E and p do not commute, so this doesn't look like a Hermitian operator.

Shouldn't this be added to its Hermitian adjoint (and divided by 2) to get a Hermitian Hamiltonian?
 
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The spin-orbit Hamiltonian is usually written ξ(r) L·S where ξ(r) = (1/2m2c2r) dV/dr.

Note that since V(r) is spherically symmetric, ξ(r) and L commute, so the whole thing is Hermitian.
 
But what if I want to look at the Spin Orbit Coupling in a system due to an external electric field, which may not be spherically symmetrical?
 
I think E x p is Hermitian as long as E = ∇V, isn't it? That's basically crossing ∇ with itself.
 
Well, if my position ket is of the form [itex]|x;y\rangle[/tex], and I am representing them on a rectangular grid (discrete representation)<br /> <br /> [tex]\langle x_1;y_1|E_y(x,y) p_x|x_2;y_2\rangle = \sum_{x'',y''}\langle x_1;y_1|E_y(x,y)|x'';y''\rangle \langle x'';y''|p_x|x_2;y_2\rangle[/tex]<br /> <br /> Now,<br /> <br /> [tex]\langle x_1;y_1|E_y(x,y)|x'';y''\rangle = E_y(x_1,y_1)\delta_{x_1,x''}\delta_{y_1,y''}[/tex]<br /> <br /> and<br /> <br /> [tex]\langle x'';y''|p_x|x_2;y_2\rangle = -i\hbar\langle x'';y''|\left[\frac{|x_2 + a_x;y_2\rangle - |x_2-a_x;y_2\rangle}{2 a_x}\right][/tex]<br /> <br /> The problem is... where you evaluate E_y -- at the location specified by the bra or the ket?[/itex]
 
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Can you please elaborate on that? I am trying to use this Hamiltonian with an external electric field E, in a quantum transport problem. Is it inapplicable there?

Would the correct prescription be to use 0.5(this + h.c.) where h.c. denotes the Hermitian adjoint of this operator?
 

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