Difference between revisions of "Regularized moduli spaces"
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− | Given the [[moduli spaces of pseudoholomorphic polygons]] <math>\overline\mathcal{M}(x_0;x_1,\ldots,x_d)</math> for each tuple of Lagrangians <math>L_0,\ldots,L_d\subset M</math>, generators <math>x_0\in\text{Crit}(L_0,L_d), x_1\in\text{Crit}(L_0,L_1), \ldots, x_d\in\text{Crit}(L_{d-1},L_d)</math>, and a fixed compatible almost complex structure <math>J</math>, we need to explain how to obtain regularizations <math>\overline\mathcal{M}^k(x_0;x_1,\ldots,x_d;\nu)</math> for expected dimensions <math>k=0,1</math> by a choice of perturbations <math>\nu</math>. | + | Given the [[moduli spaces of pseudoholomorphic polygons]] <math>\overline\mathcal{M}(x_0;x_1,\ldots,x_d)</math> for each tuple of Lagrangians <math>L_0,\ldots,L_d\subset M</math>, generators <math>x_0\in\text{Crit}(L_0,L_d), x_1\in\text{Crit}(L_0,L_1), \ldots, x_d\in\text{Crit}(L_{d-1},L_d)</math>, and a fixed compatible almost complex structure <math>J</math>, |
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+ | talk about Fredholm index <math>\overline\mathcal{M}^k(\ldots) = \{ b\in \mathcal{M}(\ldots) \,|\, IND ... = k\}</math> | ||
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+ | we need to explain how to obtain regularizations <math>\overline\mathcal{M}^k(x_0;x_1,\ldots,x_d;\nu)</math> for expected dimensions <math>k=0,1</math> by a choice of perturbations <math>\nu</math>. | ||
Moreover, we need to choose these perturbations ''coherently'' to ensure that the boundary of each 1-dimensional part is given by Cartesian products of 0-dimensional parts, | Moreover, we need to choose these perturbations ''coherently'' to ensure that the boundary of each 1-dimensional part is given by Cartesian products of 0-dimensional parts, | ||
<center> | <center> |
Revision as of 21:57, 28 May 2017
Given the moduli spaces of pseudoholomorphic polygons for each tuple of Lagrangians , generators , and a fixed compatible almost complex structure ,
talk about Fredholm index
we need to explain how to obtain regularizations for expected dimensions by a choice of perturbations .
Moreover, we need to choose these perturbations coherently to ensure that the boundary of each 1-dimensional part is given by Cartesian products of 0-dimensional parts,
TODO
Finally, we need to check that for each pair ,
when considered as boundary point , has symplectic area and weight function .