The existence and unambiguity of the principal axis system of the EPR
tensors
- URL: http://arxiv.org/abs/2305.06778v1
- Date: Thu, 11 May 2023 13:06:13 GMT
- Title: The existence and unambiguity of the principal axis system of the EPR
tensors
- Authors: Stanislav Komorovsky
- Abstract summary: We provide a comprehensive theory about the existence of principal axes of the EPR tensors.
Both g- and a-tensors have two sets of principal axes -- one in the real and one in the fictitious spin space.
We present arguments based on the group theory why only eigenvalues of the G-tensor, $mbG = mbgmbg!mathsfT$, and the sign of the determinant of the g-tensor are observable quantities.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: Although the role of the electron paramagnetic resonance (EPR) g-tensor and
hyperfine coupling tensor in the EPR effective spin Hamiltonian is discussed
extensively in many textbooks, certain aspects of the theory are missing. In
this text we will cover those gaps and thus provide a comprehensive theory
about the existence of principal axes of the EPR tensors. However, an important
observation is that both g- and a-tensors have two sets of principal axes --
one in the real and one in the fictitious spin space -- and, in fact, are not
tensors. Moreover, we present arguments based on the group theory why only
eigenvalues of the G-tensor, $\mb{G} = \mb{g}\mb{g}^{\!\mathsf{T}}$, and the
sign of the determinant of the g-tensor are observable quantities (an
analogical situation also holds for the hyperfine coupling tensor). We keep the
number of assumptions to a minimum and thus the theory is applicable in the
framework of the Dirac--Coulomb--Breit Hamiltonian and for any spatial symmetry
of the system.
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