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Explicitly linked the mention of "measure" in the last section to Lebesgue measure. |
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For <math>\lambda = 1</math>, the almost Mathieu operator is sometimes called '''Harper's equation'''.
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If <math>\alpha</math> is a [[rational number]], then <math>H^{\lambda,\alpha}_\omega</math>
is a periodic operator and by [[Floquet theory]] its [[spectrum (functional analysis)|spectrum]] is purely [[absolutely continuous]].
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This lower bound was proved independently by Avron, Simon and [[Michael Herman (mathematician)|Michael Herman]], after an earlier almost rigorous argument of Aubry and André. In fact, when <math> E </math> belongs to the spectrum, the inequality becomes an equality (the Aubry-André formula), proved by [[Jean Bourgain]] and Svetlana Jitomirskaya.<ref>{{cite journal |first=J. |last=Bourgain |first2=S. |last2=Jitomirskaya |title=Continuity of the Lyapunov exponent for quasiperiodic operators with analytic potential |journal=[[Journal of Statistical Physics]] |volume=108 |year=2002 |issue=5–6 |pages=1203–1218 |doi=10.1023/A:1019751801035 }}</ref>
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▲[[Image:Hofstadter's_butterfly.png|thumb|Hofstadter's Butterfly]]
Another striking characteristic of the almost Mathieu operator is that its spectrum is a [[Cantor set]] for all irrational <math>\alpha</math> and <math>\lambda > 0</math>. This was shown by [[Artur Avila|Avila]] and [[Svetlana Jitomirskaya|Jitomirskaya]] solving the by-then famous "
Furthermore, the [[Lebesgue measure]] of the spectrum of the almost Mathieu operator is known to be
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The study of the spectrum for <math> \lambda =1 </math> leads to the [[Hofstadter's butterfly]], where the spectrum is shown as a set.
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