We estimate the decay width difference in the system including contributions and next-to-leading order QCD corrections, and find it to be around 0.3%. We explicitly show that the time measurements of an untagged decaying to a single final state isotropically can only be sensitive to quadratic terms in $\Delta Gamma_d / \Gamma_d$, and hence the use of at least two different final states is desired. We discuss such pairs of candidate decay channels for the final states and explore the feasibility of a measurement through them. The measurement of this width difference is essential for an accurate measurement of at the LHC. The nonzero width difference may also be used to identify new physics effects and to resolve a twofold discrete ambiguity in the - mixing phase. We also derive an upper bound on the value of in the presence of new physics, and point out some differences in the phenomenology of width differences in the and systems.

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