lattice/latticegpu.jl
1
0
Fork 0
mirror of https://igit.ific.uv.es/alramos/latticegpu.jl.git synced 2025-05-14 11:13:42 +02:00
Code Issues Projects Releases Packages Wiki Activity Actions

Small changes in documentation

Browse source
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
Download patch file Download diff file Expand all files Collapse all files

5
docs/src/dirac.md
View file

@ -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.
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
\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
as specified in `lp.plidx`.

2
src/Solvers/Propagators.jl
View file

@ -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.
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)