Commit fab7734d by Matthieu Schaller

### Use a standard sigmoid as a long-range cut-off function for periodic gravity.

parent 560f13d2
 ... ... @@ -67,16 +67,36 @@ phi_newton = 1. / r phit_newton = 1. / k**2 def smoothstep(x): #S_2(x) ret = 6*x**5 - 15*x**4 + 10*x**3#3*x**2 - 2*x**3 ret = 6*x**5 - 15*x**4 + 10*x**3 #ret = 3*x**2 - 2*x**3 ret[x < 0] = 0. ret[x > 1] = 1. return ret def sigmoid(x): return 1. / (1. + exp(-x)) #return x / sqrt(1. + x**2) # Correcction in real space def swift_corr(x): #return 2. * smoothstep(x/4. + 1./2.) - 1. #return sigmoid(4. * x) return 2 * sigmoid( 4 * x ) - 1 figure() x = linspace(-4, 4, 100) plot(x, special.erf(x), '-', color=colors[0]) plot(x, swift_corr(x), '-', color=colors[1]) plot(x, x, '-', color=colors[2]) ylim(-1.1, 1.1) xlim(-4.1, 4.1) savefig("temp.pdf") # Correction in real space corr_short_gadget2 = special.erf(r / (2.*r_s)) corr_long_gadget2 = exp(-k**2*r_s**2) corr_short_swift = smoothstep(r / (2.*r_s)) corr_long_swift = 0.5 * (90 * r_s * k * np.cos(k * r_s)**2 + (r_s**2 * k**2 - 3) * np.sin(2*r_s*k))/ (r_s**5 * k**7) corr_short_swift = swift_corr(r / (2.*r_s)) #corr_long_swift = (-15. / 1024.) * (12. * r_s * k * cos(4. * r_s * k) + (16. * r_s**2 * k**2 - 3.) * sin(4. * r_s * k)) / (k**5 * r_s**5) corr_long_swift = k * r_s * math.pi / (2. * sinh(0.5 * math.pi * r_s * k)) # Shortrange term phi_short_gadget2 = (1. / r ) * (1. - corr_short_gadget2) ... ... @@ -105,17 +125,19 @@ ylabel("$\\varphi_s(r)$", labelpad=-3) legend(loc="upper right", frameon=True, handletextpad=0.1, handlelength=3.2, fontsize=8) # Correction subplot(312, xscale="log", yscale="linear") subplot(312, xscale="log", yscale="log") #plot(r_rs, np.ones(np.size(r)), '--', lw=1.4, color=colors[0]) plot(r_rs, 1. - corr_short_gadget2, '-', lw=1.4, color=colors[2]) plot(r_rs, 1. - corr_short_swift, '-', lw=1.4, color=colors[3]) plot(r_rs, np.zeros(np.size(r)), 'k--', alpha=0.5, lw=0.5) #plot(r_rs, np.zeros(np.size(r)), 'k--', alpha=0.5, lw=0.5) plot(r_rs, np.ones(np.size(r)), 'k--', alpha=0.5, lw=0.5) plot(r_rs, np.ones(np.size(r))*0.01, 'k--', alpha=0.5, lw=0.5) plot([1., 1.], [-1e5, 1e5], 'k-', alpha=0.5, lw=0.5) yticks([1e-2, 1e-1, 1], ["$0.01$", "$0.1$", "$1$"]) xlim(1.1*r_min/r_s, 0.9*r_max/r_s) ylim(-0.1, 1.1) ylabel("$\\chi_s(r)$", labelpad=2) ylim(3e-3, 1.5) ylabel("$\\chi_s(r)$", labelpad=-3) subplot(313, xscale="log", yscale="log") ... ... @@ -150,13 +172,14 @@ subplot(211, xscale="log", yscale="log") plot(k_rs, phit_newton, '--', lw=1.4, label="${\\rm Newtonian}$", color=colors[0]) plot(k_rs, phit_long_gadget2, '-', lw=1.4, label="${\\rm Gadget}$", color=colors[2]) plot(k_rs, phit_long_swift, '-', lw=1.4, label="${\\rm SWIFT}$", color=colors[3]) plot(k_rs, -phit_long_swift, ':', lw=1.4, color=colors[3]) plot([1., 1.], [1e-5, 1e5], 'k-', alpha=0.5, lw=0.5) legend(loc="lower left", frameon=True, handletextpad=0.1, handlelength=3.2, fontsize=8) xlim(1.1*r_min/ r_s, 0.9*r_max / r_s) ylim(1.1/r_max**2, 0.9/r_min**2) ylabel("$\\tilde\\varphi_l(k)$", labelpad=-3) ylabel("$\\tilde{\\varphi_l}(k)$", labelpad=-3) subplot(212, xscale="log", yscale="log") ... ... @@ -165,12 +188,13 @@ subplot(212, xscale="log", yscale="log") plot(k_rs, phit_newton * k**2, '--', lw=1.4, label="${\\rm Newtonian}$", color=colors[0]) plot(k_rs, phit_long_gadget2 * k**2, '-', lw=1.4, label="${\\rm Gadget}$", color=colors[2]) plot(k_rs, phit_long_swift * k**2, '-', lw=1.4, label="${\\rm SWIFT}$", color=colors[3]) plot(k_rs, -phit_long_swift * k**2, ':', lw=1.4, label="${\\rm SWIFT}$", color=colors[3]) plot([1., 1.], [1e-5, 1e5], 'k-', alpha=0.5, lw=0.5) plot(r_rs, np.ones(np.size(r))*0.01, 'k--', alpha=0.5, lw=0.5) xlim(1.1*r_min/ r_s, 0.9*r_max / r_s) ylim(3e-3, 1.5) ylabel("$k^2 \\times \\tilde\\varphi_l(k)$", labelpad=-3) ylabel("$k^2 \\times \\tilde{\\varphi_l}(k)$", labelpad=-3) yticks([1e-2, 1e-1, 1], ["$0.01$", "$0.1$", "$1$"]) xlabel("$k \\times r_s$", labelpad=0) ... ...
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