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We investigate experimentally and theoretically the dynamical properties of a Mott insulator in decoupled one-dimensional chains.
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The skewness is defined as γ = 1 W σ 3 ∫ d ω ( ω − ω ¯ ) 3 S ( q , ω ) \gamma=\frac{1}{W\sigma^{3}}\int d\omega(\omega-\bar{\omega})^{3}S(q,\omega) , where σ 2 = 1 W ∫ d ω ( ω − ω ¯ ) 2 S ( q , ω ) \sigma^{2}=\frac{1}{W}\int d\omega(\omega-\bar{\omega})^{2}S(q,\omega) and ω ¯ = 1 W ∫ d ω ω S ( q , ω ) \bar{\omega}=\frac{1}{W}\int d\omega\omega S(q,\omega)
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2011
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