TY - JOUR
T1 - Unbounded Trace Orbits of Thue–Morse Hamiltonian
AU - Liu, Qinghui
AU - Qu, Yanhui
AU - Yao, Xiao
N1 - Publisher Copyright:
© 2017, Springer Science+Business Media New York.
PY - 2017/3/1
Y1 - 2017/3/1
N2 - It is well known that, an energy is in the spectrum of Fibonacci Hamiltonian if and only if the corresponding trace orbit is bounded. However, it is not known whether the same result holds for the Thue–Morse Hamiltonian. In this paper, we give a negative answer to this question. More precisely, we construct two subsets Σ II and Σ I II of the spectrum of the Thue–Morse Hamiltonian, both of which are dense and uncountable, such that each energy in Σ II∪ Σ III corresponds to an unbounded trace orbit. Exact estimates on the norm of the transfer matrices are also obtained for these energies: for E∈ Σ II∪ Σ III, the norms of the transfer matrices behave like ec1γ√n≤‖Tn(E)‖≤ec2γ√n.However, two types of energies are quite different in the sense that each energy in Σ II is associated with a two-sided pseudo-localized state, while each energy in Σ III is associated with a one-sided pseudo-localized state. The difference is also reflected by the local dimensions of the spectral measure: the local dimension is 0 for energies in Σ II and is larger than 1 for energies in Σ III. As a comparison, we mention another known countable dense subset Σ I. Each energy in Σ I corresponds to an eventually constant trace map and the associated eigenvector is an extended state. In summary, the Thue–Morse Hamiltonian exhibits “mixed spectral nature”.
AB - It is well known that, an energy is in the spectrum of Fibonacci Hamiltonian if and only if the corresponding trace orbit is bounded. However, it is not known whether the same result holds for the Thue–Morse Hamiltonian. In this paper, we give a negative answer to this question. More precisely, we construct two subsets Σ II and Σ I II of the spectrum of the Thue–Morse Hamiltonian, both of which are dense and uncountable, such that each energy in Σ II∪ Σ III corresponds to an unbounded trace orbit. Exact estimates on the norm of the transfer matrices are also obtained for these energies: for E∈ Σ II∪ Σ III, the norms of the transfer matrices behave like ec1γ√n≤‖Tn(E)‖≤ec2γ√n.However, two types of energies are quite different in the sense that each energy in Σ II is associated with a two-sided pseudo-localized state, while each energy in Σ III is associated with a one-sided pseudo-localized state. The difference is also reflected by the local dimensions of the spectral measure: the local dimension is 0 for energies in Σ II and is larger than 1 for energies in Σ III. As a comparison, we mention another known countable dense subset Σ I. Each energy in Σ I corresponds to an eventually constant trace map and the associated eigenvector is an extended state. In summary, the Thue–Morse Hamiltonian exhibits “mixed spectral nature”.
KW - Local Hausdorff dimension
KW - Pseudo localization
KW - Subordinate solution
KW - Thue–Morse Hamiltonian
KW - Trace orbit
UR - http://www.scopus.com/inward/record.url?scp=85011545427&partnerID=8YFLogxK
U2 - 10.1007/s10955-017-1726-x
DO - 10.1007/s10955-017-1726-x
M3 - Article
AN - SCOPUS:85011545427
SN - 0022-4715
VL - 166
SP - 1509
EP - 1557
JO - Journal of Statistical Physics
JF - Journal of Statistical Physics
IS - 6
ER -