Exact(6)
If t is not right scattered, then the derivative is defined by f △ ( t ) = lim s → t f ( σ ( t ) ) − f ( s ) σ ( t ) − s = lim s → t f ( t ) − f ( s ) t − s, provided this limit exists.
If t is right scattered, then (vert h(t -vvert leq w(t -vvert(t)-uvert )) because (leq_{ito infty }vert h(t)-v_{i}vert =vert h(t)-vvert ).
If F is continuous at t and t is right scattered, then F is (Delta_{mathrm{gH}} -differentiable at t with F^{Delta_{mathrm{gH}} -differentiableg}F(t)}{mu(t)}.
Then we have the following: (i): If (F:mathbb{T}rightarrowmathcal{K}_{C}) is (Delta_{mathrm{gH}} -differentiable at (tinmathbb{T}^{kappa}) then it is continuous at t. (ii): If F is continuous at t anDelta_{mathrm{gH}} -differentiable(Deltat{matinmathbb{-differenT}^{kappa}thenth F^{Delta}(t)=frac{F(sitma(t))omisus_{g}F(t)}{mu(t)}.
and all x ˆ ∈ B δ 2 ( x ), where B δ 2 ( x ) is an open ball centered on x of radius δ 2. If t ∈ T is right scattered, then we can always choose a suitable δ 1 such that t ˆ = t is the only point satisfying condition (2.21) (see [22], Theorem 3.6.1]).
If no hot spot is identified and the mitotic figures are sparse and randomly scattered, then the count should begin in a field containing a mitosis, then extended to immediately adjacent nonoverlapping high-power fields until a 1 mm area of tissue containing melanoma is assessed.
Similar(52)
North of Tsuchiyama, the surface ruptures scattered and then vanished.
After arriving at the first scattering center, the photon is scattered and then continues to move with attenuation.
The minions scatter, then regroup.
The hands crept up, first a scattering, then a thicket.
Cells were initially gated on a FACSAria cell sorter (BD Biosciences) by forward and orthogonal light scatter, then analysed to collect CD138negPIneg and CD138+PIneg cells.
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