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Avoided Crossing


An avoided crossing is the approach and subsequent separation of two eigenvalues of a matrix or linear operator family without their becoming equal as a real parameter varies. It is often called an avoided level crossing.

For example, consider the real symmetric matrix family

 H(t)=[t g; g -t],

where t in R and g is a fixed nonzero real number. Its eigenvalues are

 lambda_+/-(t)=+/-sqrt(t^2+g^2).

The gap lambda_+(t)-lambda_-(t) has minimum 2|g| at t=0. When g=0, the two diagonal entries t and -t instead cross at the origin.

For a general real symmetric matrix A=(a_(ij)) of size 2×2, a repeated eigenvalue requires both a_(11)=a_(22) and a_(12)=0. These are two independent real conditions, so the coincidence has codimension 2. For a 2×2 Hermitian matrix, the off-diagonal entry may be complex, and its vanishing imposes two real conditions in addition to a_(11)=a_(22), giving codimension 3 (von Neumann and Wigner 1929; Seyranian et al. 2005, p. 1725). Thus an unconstrained family with one real parameter generically avoids such coincidences within either of these matrix classes. Additional symmetry can permit an actual crossing.

For fixed g!=0, analytic continuation of the displayed family to complex t gives square-root branch points at t=+/-ig, where i is the imaginary unit. At either value the matrix is nonzero but its square vanishes, so the coincident eigenvalues have only one independent eigenvector. These are exceptional points. This model illustrates the connection between avoided crossings for a real parameter and branch point structure in the complex plane (Heiss and Steeb 1991). A diabolic point, in contrast, has two linearly independent eigenvectors at a double eigenvalue.


See also

Diabolic Point, Eigenvalue, Exceptional Point, Hermitian Matrix, Real Symmetric Matrix

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References

Heiss, W. D. and Steeb, W.-H. "Avoided Level Crossings and Riemann Sheet Structure." J. Math. Phys. 32, 3003-3007, 1991. https://doi.org/10.1063/1.529044.Keck, F.; Korsch, H. J.; and Mossmann, S. "Unfolding a Diabolic Point: A Generalized Crossing Scenario." J. Phys. A: Math. Gen. 36, 2125-2137, 2003. https://doi.org/10.1088/0305-4470/36/8/310.Pato, M. P. "Level Repulsion and the Dynamical Diagonalization of Matrices." Physica A 312, 153-158, 2002. https://doi.org/10.1016/S0378-4371(02)00863-4.Rotter, I. "Correlations in Quantum Systems and Branch Points in the Complex Plane." Phys. Rev. C 64, 034301, 2001a. https://doi.org/10.1103/PhysRevC.64.034301.Rotter, I. "Dynamics of Quantum Systems." Phys. Rev. E 64, 036213, 2001b. https://doi.org/10.1103/PhysRevE.64.036213. Erratum: Phys. Rev. E 66, 039902, 2002. https://doi.org/10.1103/PhysRevE.66.039902.Seyranian, A. P.; Kirillov, O. N.; and Mailybaev, A. A. "Coupling of Eigenvalues of Complex Matrices at Diabolic and Exceptional Points." J. Phys. A: Math. Gen. 38, 1723-1740, 2005. https://doi.org/10.1088/0305-4470/38/8/009.Trott, M. "Solution of Equations." §1.5 in The Mathematica GuideBook for Symbolics. New York: Springer-Verlag, 2006. https://doi.org/10.1007/0-387-28815-5. https://www.mathematicaguidebooks.org/.von Neumann, J. and Wigner, E. P. "Über das Verhalten von Eigenwerten bei adiabatischen Prozessen." Phys. Z. 30, 467-470, 1929.

Cite this as:

Weisstein, Eric W. "Avoided Crossing." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/AvoidedCrossing.html

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