Difference between revisions of "Z3 grid source"
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| + | ==Comments== | ||
| + | * '''The original motivation of using Z<sub>3</sub> grid source is to cue "mismatch issue" when the low modes are substituted by the exact many-to-all solutions.''' | ||
| + | * In order to take advantage of noise estimator, we use Z<sub>3</sub> noise as the source vector during the overlap inversion. We put Z<sub>3</sub> noise as a spacial grid at t = 0 time slices. For the 32<sup>3</sup>×64 lattices, the 64 grid points seems to be enough. | ||
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==Meson correlators on 24<sup>3</sup>×64 lattices at m<sub>l</sub> = 0.005 and m<sub>s</sub> = 0.04== | ==Meson correlators on 24<sup>3</sup>×64 lattices at m<sub>l</sub> = 0.005 and m<sub>s</sub> = 0.04== | ||
Revision as of 20:56, 14 January 2011
Comments
- The original motivation of using Z3 grid source is to cue "mismatch issue" when the low modes are substituted by the exact many-to-all solutions.
- In order to take advantage of noise estimator, we use Z3 noise as the source vector during the overlap inversion. We put Z3 noise as a spacial grid at t = 0 time slices. For the 323×64 lattices, the 64 grid points seems to be enough.
