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In the limit, the spatial distribution, becomes close to uniform distribution.
In the limit the spike train approximates the sum of δ-functions given by Eq. (1).
In the limit as ε → 0, I ε ( t ) becomes q δ ( t ).
In the limit β0 → 0 the spectrum evidently does not exist.
In the limit of high bias, this transport picture changes, which we discuss later.
In the limit of both H → 0 and H → ∞, LYR model becomes the homogeneous model.
In the limit the exponent must be minimized for to be minimum.
In the limit ϕ k → 0, Eq. (7) is singular and λ k seems to diverge.
In the limit q = 1, distribution function tends to the nonthermal distribution function.
In the limit as n → ∞, the sum becomes the Riemann sum for the above integral.
(In the limit of a single molecule the concept becomes meaningless).
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