Regular instead of r_min
This commit is contained in:
parent
d23792b977
commit
6deee7e47c
15
dirac.jl
15
dirac.jl
|
|
@ -4,6 +4,8 @@ using DifferentialEquations, Roots
|
||||||
M_n = 939.5654133 # Neutron mass in MeV/c2
|
M_n = 939.5654133 # Neutron mass in MeV/c2
|
||||||
M_p = 938.2720813 # Proton mass in MeV/c2
|
M_p = 938.2720813 # Proton mass in MeV/c2
|
||||||
|
|
||||||
|
const r_reg = 1E-6 # regulator for the centrifugal term in fm
|
||||||
|
|
||||||
"The spherical Dirac equation that returns du=[dg, df] in-place where
|
"The spherical Dirac equation that returns du=[dg, df] in-place where
|
||||||
u=[g, f] are the reduced radial components evaluated at r,
|
u=[g, f] are the reduced radial components evaluated at r,
|
||||||
κ is the generalized angular momentum,
|
κ is the generalized angular momentum,
|
||||||
|
|
@ -17,23 +19,22 @@ function dirac!(du, u, (κ, p, E, Φ0, W0, B0, A0), r)
|
||||||
common1 = E - W0(r) - (p - 0.5) * B0(r) - p * A0(r)
|
common1 = E - W0(r) - (p - 0.5) * B0(r) - p * A0(r)
|
||||||
common2 = M - Φ0(r)
|
common2 = M - Φ0(r)
|
||||||
(g, f) = u
|
(g, f) = u
|
||||||
du[1] = -(κ/r) * g + (common1 + common2) * f / ħc
|
du[1] = -(κ/(r + r_reg)) * g + (common1 + common2) * f / ħc
|
||||||
du[2] = (κ/r) * f - (common1 - common2) * g / ħc
|
du[2] = (κ/(r + r_reg)) * f - (common1 - common2) * g / ħc
|
||||||
end
|
end
|
||||||
|
|
||||||
"Solve the Dirac equation and return g(r=r_max) for given scalar and vector potentials where
|
"Solve the Dirac equation and return g(r=r_max) for given scalar and vector potentials where
|
||||||
r_max is the outer boundary in fm,
|
r_max is the outer boundary in fm,
|
||||||
r_min (=r_max/1000) is inside boundary in fm which cannot be 0 due to the centrifugal term,
|
|
||||||
the other parameters are the same from dirac!(...)."
|
the other parameters are the same from dirac!(...)."
|
||||||
function boundaryValue(κ, p, E, Φ0, W0, B0, A0, r_max, r_min=r_max/1000)
|
function boundaryValue(κ, p, E, Φ0, W0, B0, A0, r_max,)
|
||||||
prob = ODEProblem(dirac!, [0, 1], (r_min, r_max))
|
prob = ODEProblem(dirac!, [0, 1], (0, r_max))
|
||||||
sol = solve(prob, RK4(), p=(κ, p, E, Φ0, W0, B0, A0))
|
sol = solve(prob, RK4(), p=(κ, p, E, Φ0, W0, B0, A0))
|
||||||
return sol(r_max)[1]
|
return sol(r_max)[1]
|
||||||
end
|
end
|
||||||
|
|
||||||
"Find all bound energies between E_min (=0) and E_max (=mass) where
|
"Find all bound energies between E_min (=0) and E_max (=mass) where
|
||||||
the other parameters are the same from dirac!(...)."
|
the other parameters are the same from dirac!(...)."
|
||||||
function findEs(κ, p, Φ0, W0, B0, A0, r_max, r_min=r_max/1000, E_min=0, E_max=(p ? M_p : M_n))
|
function findEs(κ, p, Φ0, W0, B0, A0, r_max, E_min=0, E_max=(p ? M_p : M_n))
|
||||||
f(E) = boundaryValue(κ, p, E, Φ0, W0, B0, A0, r_max, r_min)
|
f(E) = boundaryValue(κ, p, E, Φ0, W0, B0, A0, r_max)
|
||||||
return find_zeros(f, (E_min, E_max))
|
return find_zeros(f, (E_min, E_max))
|
||||||
end
|
end
|
||||||
|
|
|
||||||
|
|
@ -18,10 +18,10 @@ A_interp = linear_interpolation(xs, As)
|
||||||
κ = -1
|
κ = -1
|
||||||
p = true
|
p = true
|
||||||
r_max = maximum(xs)
|
r_max = maximum(xs)
|
||||||
E_min = 850
|
E_min = 880
|
||||||
E_max = 939
|
E_max = 939
|
||||||
|
|
||||||
boundEs = findEs(κ, p, S_interp, V_interp, R_interp, A_interp, r_max, r_max/1000, E_min, E_max)
|
boundEs = findEs(κ, p, S_interp, V_interp, R_interp, A_interp, r_max, E_min, E_max)
|
||||||
println("bound E = $boundEs")
|
println("bound E = $boundEs")
|
||||||
|
|
||||||
Es = collect(E_min:0.5:E_max)
|
Es = collect(E_min:0.5:E_max)
|
||||||
|
|
|
||||||
Loading…
Reference in New Issue