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Small changes in documentation

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This commit is contained in:
Fernando P. Panadero 2023-11-30 12:19:10 +01:00
parent ed9d18b25d
commit 30d3c2ae89
2 changed files with 4 additions and 3 deletions
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5
docs/src/dirac.md
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@ -41,10 +41,11 @@ where $$m_0$$ and $$\theta$$ are respectively the values `.m0` and `.th` of [`Di
Note that $$|\theta(i)|=1$$ is not built into the code, so it should be imposed explicitly. Note that $$|\theta(i)|=1$$ is not built into the code, so it should be imposed explicitly.
Additionally, if |`dpar.csw`| > 1.0E-10, the clover term is assumed to be stored in `ymws.csw`, which Additionally, if |`dpar.csw`| > 1.0E-10, the clover term is assumed to be stored in `ymws.csw`, which
can be done via the [`Csw`](@ref) function. In this case we have an extra term in `Dw!`: can be done via the [`Csw`](@ref) function. In this case we have the Sheikholeslami–Wohlert (SW) term
in `Dw!`:
```math ```math
\frac{i}{2}C_{sw} \sum_{\pi = 1}^6 F^{cl}_\pi \sigma_\pi \psi(\vec{x}) \frac{i}{2}c_{sw} \sum_{\pi = 1}^6 F^{cl}_\pi \sigma_\pi \psi(\vec{x})
``` ```
where the $$\sigma$$ matrices are those described in the `Spinors` module and the index $$\pi$$ runs where the $$\sigma$$ matrices are those described in the `Spinors` module and the index $$\pi$$ runs
as specified in `lp.plidx`. as specified in `lp.plidx`.

2
src/Solvers/Propagators.jl
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@ -99,7 +99,7 @@ end
""" """
function Tbndpropagator(U, dpar::DiracParam{T}, dws::DiracWorkspace, lp::SpaceParm{4,6,1,D}, maxiter::Int64, tol::Float64, c::Int64, s::Int64) function Tbndpropagator!(pro, U, dpar::DiracParam{T}, dws::DiracWorkspace, lp::SpaceParm{4,6,1,D}, maxiter::Int64, tol::Float64, c::Int64, s::Int64)
Returns the propagator from the t=T boundary to the bulk for the SF boundary conditions for a source with color 'c' and spin 's'. The factor c_t is included while the factor 1/sqrt(V) is not. Returns the propagator from the t=T boundary to the bulk for the SF boundary conditions for a source with color 'c' and spin 's'. The factor c_t is included while the factor 1/sqrt(V) is not.
For the propagator from t=0 to the bulk, use the function bndpropagator(U, dpar::DiracParam{T}, dws::DiracWorkspace, lp::SpaceParm{4,6,1,D}, maxiter::Int64, tol::Float64, c::Int64, s::Int64) For the propagator from t=0 to the bulk, use the function bndpropagator(U, dpar::DiracParam{T}, dws::DiracWorkspace, lp::SpaceParm{4,6,1,D}, maxiter::Int64, tol::Float64, c::Int64, s::Int64)