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We offer a statistical solution to left truncation that can be easily applied in widely used statistical programs.
We define the flow map ζ as the solution to left { textstylebegin{array}{l} zeta_{t} (y,t)=v zeta y,t),t), zeta y,0)= {zeta_{0}}.
Furthermore ũ tends to a non-vanishing function (tilde{u}_{infty}) as (R to +infty) which is the solution to left { textstylebegin{array}{l} tilde{u}_{infty}"+ n-1 + n-1 l tilde{u}ty}' +tilde{u}_{infty}^{p} =0 quad mbox{on } (0,1), tilde{u}_{infty}geq0 quad mbox{on } (0,1), tilde{u}_{infty}(0)=tilde{u}_{infty}(1)=0.
Then u is degenerate, that is, there exists a non-trivial solution to left { textstylebegin{array}{l} L_{u} v=-Delta_{mathbf{g}} v - p u^{p-1}v =0quad textit{on } A, v = 0 quad textit{on } partial A, end{array}displaystyle right.
If (w_{R} in H_{0}^{1}(A_{R})) denotes the positive radial solution to left { textstylebegin{array}{l} Delta_{mathbf{g}} u + u ^{p} = 0 quad text{in } A_{R}, u > 0 quad text{in } A_{R}, u = 0 quad text{on } partial A_{R}, end{array}displaystyle right.
Using the Green formula, the problem (1.1) can be transformed into the following continuous parabolic variational equation: find the (uin L^{2} ( 0,T,H_{0}^{1} ( Omega ) ) cap C^{2} ( 0,T,H^{-1} ( Omega ) ) ) solution to left { textstylebegin{array}{l} ( u_{t},v ) _{Omega} +a u,v)= ( f,v ) _{Omega }, quad vin H_{0}^{1} ( Omega ), u(cdot,0)=u_{0},end{array}displaystyle right.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com