TY - JOUR
T1 - Random Fields on Model Sets with Localized Dependency and Their Diffraction
AU - Akama, Yohji
AU - Iizuka, Shinji
PY - 2012/11
Y1 - 2012/11
N2 - For a random field on a general discrete set, we introduce a condition that the range of the correlation from each site is within a predefined compact set D. For such a random field ω defined on the model set Λ that satisfies a natural geometric condition, we develop a method to calculate the diffraction measure of the random field. The method partitions the random field into a finite number of random fields, each being independent and admitting the law of large numbers. The diffraction measure of ω consists almost surely of a pure-point component and an absolutely continuous component. The former is the diffraction measure of the expectation E[ω], while the inverse Fourier transform of the absolutely continuous component of ω turns out to be a weighted Dirac comb which satisfies a simple formula. Moreover, the pure-point component will be understood quantitatively in a simple exact formula if the weights are continuous over the internal space of Λ. Then we provide a sufficient condition that the diffraction measure of a random field on a model set is still pure-point.
AB - For a random field on a general discrete set, we introduce a condition that the range of the correlation from each site is within a predefined compact set D. For such a random field ω defined on the model set Λ that satisfies a natural geometric condition, we develop a method to calculate the diffraction measure of the random field. The method partitions the random field into a finite number of random fields, each being independent and admitting the law of large numbers. The diffraction measure of ω consists almost surely of a pure-point component and an absolutely continuous component. The former is the diffraction measure of the expectation E[ω], while the inverse Fourier transform of the absolutely continuous component of ω turns out to be a weighted Dirac comb which satisfies a simple formula. Moreover, the pure-point component will be understood quantitatively in a simple exact formula if the weights are continuous over the internal space of Λ. Then we provide a sufficient condition that the diffraction measure of a random field on a model set is still pure-point.
KW - Absolutely continuous spectrum
KW - Diffraction
KW - Model set
KW - Pure-point spectrum
KW - Quasicrystal
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U2 - 10.1007/s10955-012-0588-5
DO - 10.1007/s10955-012-0588-5
M3 - Article
AN - SCOPUS:84867996750
SN - 0022-4715
VL - 149
SP - 478
EP - 495
JO - Journal of Statistical Physics
JF - Journal of Statistical Physics
IS - 3
ER -