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We estimate the long-distance contribution to the \Delta{\Gamma}s of B_ssystem, based mainly on two-body D^(*)_s\Dbar^(*)_s modes and three-bodyD^(*)_s\Dbar^(*)\Kbar^(*) modes (and their CP conjugates). Some higher c\bar{s}resonances are also considered. The contribution to \Delta{\Gamma}s/{\Gamma}sby two-body modes is 10.2+-3.0%, slightly smaller than the short-distanceresult of 13.3+-3.2%. The contribution to width difference by D*_s0(2317),D_s1(2460), and D_s1(2536) resonances is negligible. For the three-body modes,we adopt the factorization formalism and model the form factors with off-shellD^(*)_s poles, the D_{sJ}(2700) resonance, and non-resonant (NR) contributions.These three-body modes can arise through current-produced or transitiondiagrams, but only SU(3)-related D^(*)_{u,d} \Dbar^(*)\Kbar modes from currentdiagram have been measured so far. The pole model results for D^*_{u,d}\Dbar^(*)\Kbar agree well with data, while D_{u,d} \Dbar^(*)\Kbar rates agreewith data only within a factor of 2 to 3. All measured three-body rates can bereproduced by including NR contribution. The total \Delta{\Gamma}s/{\Gamma}sobtained is 16.7+-8.5%, which agrees with the short-distance result withinuncertainties. For illustration, we also demonstrate the effect of D_{sJ}(2700)in modes with D^(*)K^*. In all scenarios, the total width difference remainconsistence to the short-distance result. Our result indicates that (a) theoperator product expansion (OPE) in short-distance picture is a validassumption, (b) approximating the two-body decays to saturate width differencehas a large correction, (c) the effect of three-body modes cannot be neglected,and (d) in addition to D^(*)_s poles, the D_{sJ}(2700) resonance also plays animportant role in three-body modes. Future experiments are necessary to improvethe estimation of \Delta{\Gamma}s from long-distance picture.

Long-Distance Contribution to \Delta\Gamma s/\Gamma s of the $B_s-\bar{B}_s$ System