diff options
author | Ian Jauslin <jauslin@ias.edu> | 2018-10-12 20:24:46 +0000 |
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committer | Ian Jauslin <jauslin@ias.edu> | 2018-10-16 02:48:17 +0000 |
commit | 0425ca56937e60d194c475c29b3f145c0bac30bc (patch) | |
tree | a4eb663632a766f1a43d99bc5c676caa83d6d47c /figs/plots.fig |
Initial commitv0.0
Diffstat (limited to 'figs/plots.fig')
-rw-r--r-- | figs/plots.fig/FN_base.jl | 170 | ||||
-rw-r--r-- | figs/plots.fig/Makefile | 36 | ||||
-rw-r--r-- | figs/plots.fig/current_density.jl | 60 | ||||
-rw-r--r-- | figs/plots.fig/currents-4.gnuplot | 43 | ||||
-rw-r--r-- | figs/plots.fig/currents-8.gnuplot | 43 | ||||
-rw-r--r-- | figs/plots.fig/density-4.gnuplot | 44 | ||||
-rw-r--r-- | figs/plots.fig/density-8.gnuplot | 44 | ||||
-rw-r--r-- | figs/plots.fig/integrated_current-4.gnuplot | 43 | ||||
-rw-r--r-- | figs/plots.fig/integrated_current-8.gnuplot | 43 |
9 files changed, 526 insertions, 0 deletions
diff --git a/figs/plots.fig/FN_base.jl b/figs/plots.fig/FN_base.jl new file mode 100644 index 0000000..cff6d8e --- /dev/null +++ b/figs/plots.fig/FN_base.jl @@ -0,0 +1,170 @@ +# fractional power with an arbitrary branch cut +function pow(x,a,cut) + if(angle(x)/cut<=1) + return(abs(x)^a*exp(1im*angle(x)*a)) + else + return(abs(x)^a*exp(1im*(angle(x)-sign(cut)*2*pi)*a)) + end +end + +# asymptotic airy functions +# specify a branch cut for the fractional power +function airyai_asym(x,cut) + if(abs(real(pow(x,3/2,cut)))<airy_threshold) + return(exp(2/3*pow(x,3/2,cut))*airyai(x)) + else + ret=0 + for n in 0:airy_order + ret+=gamma(n+5/6)*gamma(n+1/6)*(-3/4)^n/(4*pi^(3/2)*factorial(n)*pow(x,3*n/2+1/4,cut)) + end + return ret + end +end +function airyaiprime_asym(x,cut) + if(abs(real(pow(x,3/2,cut)))<airy_threshold) + return(exp(2/3*pow(x,3/2,cut))*airyaiprime(x)) + else + ret=0 + for n in 0:airy_order + ret+=gamma(n+5/6)*gamma(n+1/6)*(-3/4)^n/(4*pi^(3/2)*factorial(n))*(-1/pow(x,3*n/2-1/4,cut)-(3/2*n+1/4)/pow(x,3*n/2+5/4,cut)) + end + return ret + end +end + +# solutions of (-\Delta+U-ip)phi=0 +# assume that p has an infinitesimal real part (and adjust the branch cuts appropriately) +function phi(p,x,E,U) + return(airyai_asym(2^(1/3)*exp(-1im*pi/3)*(E^(1/3)*x-E^(-2/3)*(U-1im*p)),pi)) +end +function dphi(p,x,E,U) + return(2^(1/3)*exp(-1im*pi/3)*E^(1/3)*airyaiprime_asym(2^(1/3)*exp(-1im*pi/3)*(E^(1/3)*x-E^(-2/3)*(U-1im*p)),pi)) +end +function eta(p,x,E,U) + return(exp(-1im*pi/3)*airyai_asym(-2^(1/3)*(E^(1/3)*x-E^(-2/3)*(U-1im*p)),pi/2)) +end +function deta(p,x,E,U) + return(-2^(1/3)*exp(-1im*pi/3)*E^(1/3)*airyaiprime_asym(-2^(1/3)*(E^(1/3)*x-E^(-2/3)*(U-1im*p)),pi/2)) +end + +# Laplace transform of psi +# assume that p has an infinitesimal real part (and adjust the branch cuts appropriately) +# for example, (1im*p-U)^(3/2) becomes pow(1im*p-U,3/2,-pi/2) because when 1im*p is real negative, its square root should be imaginary positive +function f(p,x,k0,E,U) + T=2im*k0/(1im*k0-sqrt(2*U-k0*k0)) + R=T-1 + + if x>=0 + C2=-2im*T/(pow(-2im*p,1/2,pi/2)*phi(p,0,E,U)-dphi(p,0,E,U))*((sqrt(2*U-k0*k0)+pow(-2im*p,1/2,pi/2))/(-2im*p+k0*k0)-2im*(2*E)^(-1/3)*pi*quadgk(y -> (pow(-2im*p,1/2,pi/2)*eta(p,0,E,U)-deta(p,0,E,U))*phi(p,y,E,U)*exp(-sqrt(2*U-k0*k0)*y)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*y+E^(-2/3)*(1im*p-U),3/2,-pi/2)-E^(-1)*pow(1im*p-U,3/2,-pi/2))),0,Inf)[1]) + FT=4*(2*E)^(-1/3)*pi*(quadgk(y -> phi(p,x,E,U)*eta(p,y,E,U)*exp(-sqrt(2*U-k0*k0)*y)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*x+E^(-2/3)*(1im*p-U),3/2,-pi/2)-pow(E^(1/3)*y+E^(-2/3)*(1im*p-U),3/2,-pi/2))),0,x)[1]+quadgk(y -> eta(p,x,E,U)*phi(p,y,E,U)*exp(-sqrt(2*U-k0*k0)*y)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*y+E^(-2/3)*(1im*p-U),3/2,-pi/2)-pow(E^(1/3)*x+E^(-2/3)*(1im*p-U),3/2,-pi/2))),x,Inf)[1]) + main=C2*phi(p,x,E,U)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*x+E^(-2/3)*(1im*p-U),3/2,-pi/2)-E^(-1)*pow(1im*p-U,3/2,-pi/2)))+T*FT + + # subtract the contribution of the pole, which will be added back in after the integration + pole=psi_pole(x,k0,E,U)/(p+1im*k0*k0/2) + return(main-pole) + else + C1=-2im*T*((sqrt(2*U-k0*k0)*phi(p,0,E,U)+dphi(p,0,E,U))/(-2im*p+k0*k0)/(pow(-2im*p,1/2,pi/2)*phi(p,0,E,U)-dphi(p,0,E,U))+quadgk(y -> phi(p,y,E,U)/(pow(-2im*p,1/2,pi/2)*phi(p,0,E,U)-dphi(p,0,E,U))*exp(-sqrt(2*U-k0*k0)*y)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*y+E^(-2/3)*(1im*p-U),3/2,-pi/2)-E^(-1)*pow(1im*p-U,3/2,-pi/2))),0,Inf)[1]) + FI=-2im*exp(1im*k0*x)/(-2im*p+k0*k0) + FR=-2im*exp(-1im*k0*x)/(-2im*p+k0*k0) + main=C1*exp(pow(-2im*p,1/2,pi/2)*x)+FI+R*FR + + # subtract the contribution of the pole, which will be added back in after the integration + pole=psi_pole(x,k0,E,U)/(p+1im*k0*k0/2) + return(main-pole) + end +end +# its derivative +function df(p,x,k0,E,U) + T=2im*k0/(1im*k0-sqrt(2*U-k0*k0)) + R=T-1 + + if x>=0 + C2=-2im*T/(pow(-2im*p,1/2,pi/2)*phi(p,0,E,U)-dphi(p,0,E,U))*((sqrt(2*U-k0*k0)+pow(-2im*p,1/2,pi/2))/(-2im*p+k0*k0)-2im*(2*E)^(-1/3)*pi*quadgk(y -> (pow(-2im*p,1/2,pi/2)*eta(p,0,E,U)-deta(p,0,E,U))*phi(p,y,E,U)*exp(-sqrt(2*U-k0*k0)*y)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*y+E^(-2/3)*(1im*p-U),3/2,-pi/2)-E^(-1)*pow(1im*p-U,3/2,-pi/2))),0,Inf)[1]) + dFT=4*(2*E)^(-1/3)*pi*(quadgk(y -> dphi(p,x,E,U)*eta(p,y,E,U)*exp(-sqrt(2*U-k0*k0)*y)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*x+E^(-2/3)*(1im*p-U),3/2,-pi/2)-pow(E^(1/3)*y+E^(-2/3)*(1im*p-U),3/2,-pi/2))),0,x)[1]+quadgk(y -> deta(p,x,E,U)*phi(p,y,E,U)*exp(-sqrt(2*U-k0*k0)*y)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*y+E^(-2/3)*(1im*p-U),3/2,-pi/2)-pow(E^(1/3)*x+E^(-2/3)*(1im*p-U),3/2,-pi/2))),x,Inf)[1]) + main=C2*dphi(p,x,E,U)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*x+E^(-2/3)*(1im*p-U),3/2,-pi/2)-E^(-1)*pow(1im*p-U,3/2,-pi/2)))+T*dFT + + # subtract the contribution of the pole, which will be added back in after the integration + pole=dpsi_pole(x,k0,E,U)/(p+1im*k0*k0/2) + return(main-pole) + else + C1=-2im*T*((sqrt(2*U-k0*k0)*phi(p,0,E,U)+dphi(p,0,E,U))/(-2im*p+k0*k0)/(pow(-2im*p,1/2,pi/2)*phi(p,0,E,U)-dphi(p,0,E,U))+quadgk(y -> phi(p,y,E,U)/(pow(-2im*p,1/2,pi/2)*phi(p,0,E,U)-dphi(p,0,E,U))*exp(-sqrt(2*U-k0*k0)*y)*exp(sqrt(2)*2im/3*(pow(E^(1/3)*y+E^(-2/3)*(1im*p-U),3/2,-pi/2)-E^(-1)*pow(1im*p-U,3/2,-pi/2))),0,Inf)[1]) + dFI=2*k0*exp(1im*k0*x)/(-2im*p+k0*k0) + dFR=-2*k0*exp(-1im*k0*x)/(-2im*p+k0*k0) + main=C1*pow(-2im*p,1/2,pi/2)*exp(pow(-2im*p,1/2,pi/2)*x)+dFI+R*dFR + + # subtract the contribution of the pole, which will be added back in after the integration + pole=dpsi_pole(x,k0,E,U)/(p+1im*k0*k0/2) + return(main-pole) + end +end + +# psi (returns t,psi(x,t)) +function psi(x,k0,E,U,p_npoints,p_cutoff) + fft=fourier_fft(f,x,k0,E,U,p_npoints,p_cutoff) + # add the contribution of the pole + for i in 1:p_npoints + fft[2][i]=fft[2][i]+psi_pole(x,k0,E,U)*exp(-1im*k0*k0/2*fft[1][i]) + end + return(fft) +end +# its derivative +function dpsi(x,k0,E,U,p_npoints,p_cutoff) + fft=fourier_fft(df,x,k0,E,U,p_npoints,p_cutoff) + # add the contribution of the pole + for i in 1:p_npoints + fft[2][i]=fft[2][i]+dpsi_pole(x,k0,E,U)*exp(-1im*k0*k0/2*fft[1][i]) + end + return(fft) +end + +# compute Fourier transform by sampling and fft +function fourier_fft(A,x,k0,E,U,p_npoints,p_cutoff) + fun=zeros(Complex{Float64},p_npoints) + times=zeros(p_npoints) + + # prepare fft + for i in 1:p_npoints + fun[i]=p_cutoff/pi*A(1im*(-p_cutoff+2*p_cutoff*(i-1)/p_npoints),x,k0,E,U) + times[i]=(i-1)*pi/p_cutoff + end + + ifft!(fun) + + # correct the phase + for i in 2:2:p_npoints + fun[i]=-fun[i] + end + return([times,fun]) +end + +# asymptotic value of psi +function psi_pole(x,k0,E,U) + if x>=0 + return(1im*phi(-1im*k0*k0/2,x,E,U)*2*k0/(1im*k0*phi(-1im*k0*k0/2,0,E,U)+dphi(-1im*k0*k0/2,0,E,U))*exp(sqrt(2)*2im/3*(pow(E^(1/3)*x+E^(-2/3)*(k0*k0/2-U),3/2,-pi/2)-E^(-1)*pow(k0*k0/2-U,3/2,-pi/2)))) + else + return((1im*k0*phi(-1im*k0*k0/2,0,E,U)-dphi(-1im*k0*k0/2,0,E,U))/(1im*k0*phi(-1im*k0*k0/2,0,E,U)+dphi(-1im*k0*k0/2,0,E,U))*exp(-1im*k0*x)+exp(1im*k0*x)) + end +end +function dpsi_pole(x,k0,E,U) + if x>=0 + return(1im*dphi(-1im*k0*k0/2,x,E,U)*2*k0/(1im*k0*phi(-1im*k0*k0/2,0,E,U)+dphi(-1im*k0*k0/2,0,E,U))*exp(sqrt(2)*2im/3*(pow(E^(1/3)*x+E^(-2/3)*(k0*k0/2-U),3/2,-pi/2)-E^(-1)*pow(k0*k0/2-U,3/2,-pi/2)))) + else + return(-1im*k0*(1im*k0*phi(-1im*k0*k0/2,0,E,U)-dphi(-1im*k0*k0/2,0,E,U))/(1im*k0*phi(-1im*k0*k0/2,0,E,U)+dphi(-1im*k0*k0/2,0,E,U))*exp(-1im*k0*x)+1im*k0*exp(1im*k0*x)) + end +end + +# current +function J(ps,dps) + return(2*imag(conj(ps)*dps)) +end + +# complete computation of the current +function current(x,k0,E,U,p_npoints,p_cutoff) + ps=psi(x,k0,E,U,p_npoints,p_cutoff) + dps=dpsi(x,k0,E,U,p_npoints,p_cutoff) + Js=zeros(Complex{Float64},p_npoints) + for i in 1:p_npoints + Js[i]=J(ps[2][i],dps[2][i]) + end + return(Js) +end diff --git a/figs/plots.fig/Makefile b/figs/plots.fig/Makefile new file mode 100644 index 0000000..d9fdf82 --- /dev/null +++ b/figs/plots.fig/Makefile @@ -0,0 +1,36 @@ +PROJECTNAME=currents-4 currents-8 density-4 density-8 integrated_current-4 integrated_current-8 + +PDFS=$(addsuffix .pdf, $(PROJECTNAME)) +TEXS=$(addsuffix .tikz.tex, $(PROJECTNAME)) + +all: $(PDFS) + +currents-4.pdf density-4.pdf integrated_current-4.pdf: current_density-4.dat + gnuplot $(patsubst %.pdf, %.gnuplot, $@) > $(patsubst %.pdf, %.tikz.tex, $@) + pdflatex -jobname $(basename $@) -file-line-error $(patsubst %.pdf, %.tikz.tex, $@) + +currents-8.pdf density-8.pdf integrated_current-8.pdf: current_density-8.dat + gnuplot $(patsubst %.pdf, %.gnuplot, $@) > $(patsubst %.pdf, %.tikz.tex, $@) + pdflatex -jobname $(basename $@) -file-line-error $(patsubst %.pdf, %.tikz.tex, $@) + +current_density-4.dat: + julia current_density.jl 4 > $@ +current_density-8.dat: + julia current_density.jl 8 > $@ + +install: $(PDFS) + cp $^ $(INSTALLDIR)/ + +clean-aux: + rm -f $(addsuffix .tikz.tex, $(PROJECTNAME)) + rm -f $(addsuffix .aux, $(PROJECTNAME)) + rm -f $(addsuffix .log, $(PROJECTNAME)) + +clean-dat: + rm -f current_density-4.dat + rm -f current_density-8.dat + +clean-tex: + rm -f $(PDFS) + +clean: clean-dat clean-aux clean-tex diff --git a/figs/plots.fig/current_density.jl b/figs/plots.fig/current_density.jl new file mode 100644 index 0000000..9ec85f6 --- /dev/null +++ b/figs/plots.fig/current_density.jl @@ -0,0 +1,60 @@ +using QuadGK +using FastGaussQuadrature +using SpecialFunctions +using FFTW + +# numerical values +hbar=6.58e-16 # eV.s +m=9.11e-31 # kg +Un=9 # eV +En=parse(Float64,ARGS[1])*1e9 # V/m +Kn=4.5 # eV + +# dimensionless quantities +U=1 +E=En*hbar/(Un^1.5*m^0.5)*sqrt(1.60e-19) +k0=sqrt(2*Kn/Un) + +# cutoffs +p_cutoff=20*k0 +p_npoints=4096 + +# airy approximations +airy_threshold=30 +airy_order=5 + +# order for Gauss-Legendre quadrature +order=10 + +# compute at these points +X=[(2*U-k0*k0)/(2*E),10*(2*U-k0*k0)/(2*E)] + +include("FN_base.jl") + +# compute the weights and abcissa for gauss-legendre quadratures +gl_data=gausslegendre(order) + +ps=Array{Array{Array{Complex{Float64}}}}(undef,length(X)) +dps=Array{Array{Array{Complex{Float64}}}}(undef,length(X)) +intJ=Array{Array{Complex{Float64}}}(undef,length(X)) +for i in 1:length(X) + # wave function + ps[i]=psi(X[i],k0,E,U,p_npoints,p_cutoff) + dps[i]=dpsi(X[i],k0,E,U,p_npoints,p_cutoff) + + # integrated current + intJ[i]=zeros(Complex{Float64},p_npoints) + for l in 1:order + eval=current(X[i],k0/2*(gl_data[1][l]+1),E,U,p_npoints,p_cutoff) + for j in 1:length(eval) + intJ[i][j]=intJ[i][j]+k0/2*gl_data[2][l]*eval[j] + end + end +end + +for j in 1:p_npoints + for i in 1:length(X) + print(real(ps[i][1][j])*hbar/Un*1e15,' ',abs(ps[i][2][j])^2,' ',J(ps[i][2][j],dps[i][2][j])/(2*k0),' ',real(intJ[i][j]/k0^2),' ') + end + print('\n') +end diff --git a/figs/plots.fig/currents-4.gnuplot b/figs/plots.fig/currents-4.gnuplot new file mode 100644 index 0000000..1e9dba9 --- /dev/null +++ b/figs/plots.fig/currents-4.gnuplot @@ -0,0 +1,43 @@ +## can also set the following options +set title "$E=4\\ \\mathrm{V}\\cdot\\mathrm{nm}^{-1}$" +set ylabel "$\\displaystyle\\frac j{2k}$" norotate +set xlabel "$t$ (fs)" +# +## start ticks at 0, then every x +#set xtics 0,x +#set ytics 0,x +## puts 4 minor tics between tics (5 intervals, i.e. every 0.01) +set mxtics 5 +set mytics 5 + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 12.5,8.75 standalone + +set key spacing 1.5 + +# 3=1+2 draw bottom and left sides of the box +set border 3 +# don't show tics on opposite sides +set xtics nomirror +set ytics nomirror + +# My colors +## 4169E1 (pastel blue) +## DC143C (bright red) +## 32CD32 (bright green) +## 4B0082 (deep purple) +## DAA520 (ochre) + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 3 +set style line 2 linetype rgbcolor "#DC143C" linewidth 3 +set style line 3 linetype rgbcolor "#32CD32" linewidth 3 +set style line 4 linetype rgbcolor "#4B0082" linewidth 3 +set style line 5 linetype rgbcolor "#DAA520" linewidth 3 + +set pointsize 0.6 + +set xrange [:12] + +plot "current_density-4.dat" using 1:3 every ::1 with lines linestyle 1 title "$x=x_0$",\ + "current_density-4.dat" using 5:7 every ::1 with lines linestyle 2 title "$x=10x_0$" diff --git a/figs/plots.fig/currents-8.gnuplot b/figs/plots.fig/currents-8.gnuplot new file mode 100644 index 0000000..62448f7 --- /dev/null +++ b/figs/plots.fig/currents-8.gnuplot @@ -0,0 +1,43 @@ +## can also set the following options +set title "$E=8\\ \\mathrm{V}\\cdot\\mathrm{nm}^{-1}$" +set ylabel "$\\displaystyle\\frac j{2k}$" norotate +set xlabel "$t$ (fs)" +# +## start ticks at 0, then every x +#set xtics 0,x +#set ytics 0,x +## puts 4 minor tics between tics (5 intervals, i.e. every 0.01) +set mxtics 5 +set mytics 5 + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 12.5,8.75 standalone + +set key spacing 1.5 + +# 3=1+2 draw bottom and left sides of the box +set border 3 +# don't show tics on opposite sides +set xtics nomirror +set ytics nomirror + +# My colors +## 4169E1 (pastel blue) +## DC143C (bright red) +## 32CD32 (bright green) +## 4B0082 (deep purple) +## DAA520 (ochre) + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 3 +set style line 2 linetype rgbcolor "#DC143C" linewidth 3 +set style line 3 linetype rgbcolor "#32CD32" linewidth 3 +set style line 4 linetype rgbcolor "#4B0082" linewidth 3 +set style line 5 linetype rgbcolor "#DAA520" linewidth 3 + +set pointsize 0.6 + +set xrange [:12] + +plot "current_density-8.dat" using 1:3 every ::1 with lines linestyle 1 title "$x=x_0$",\ + "current_density-8.dat" using 5:7 every ::1 with lines linestyle 2 title "$x=10x_0$" diff --git a/figs/plots.fig/density-4.gnuplot b/figs/plots.fig/density-4.gnuplot new file mode 100644 index 0000000..8139a7a --- /dev/null +++ b/figs/plots.fig/density-4.gnuplot @@ -0,0 +1,44 @@ +## can also set the following options +set title "$E=4\\ \\mathrm{V}\\cdot\\mathrm{nm}^{-1}$" +set ylabel "$|\\psi|^2$" norotate +set xlabel "$t$ (fs)" +# +## start ticks at 0, then every x +#set xtics 0,x +#set ytics 0,x +## puts 4 minor tics between tics (5 intervals, i.e. every 0.01) +set mxtics 5 +set mytics 5 + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 12.5,8.75 standalone + +set key spacing 1.5 + +# 3=1+2 draw bottom and left sides of the box +set border 3 +# don't show tics on opposite sides +set xtics nomirror +set ytics nomirror + +# My colors +## 4169E1 (pastel blue) +## DC143C (bright red) +## 32CD32 (bright green) +## 4B0082 (deep purple) +## DAA520 (ochre) + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 3 +set style line 2 linetype rgbcolor "#DC143C" linewidth 3 +set style line 3 linetype rgbcolor "#32CD32" linewidth 3 +set style line 4 linetype rgbcolor "#4B0082" linewidth 3 +set style line 5 linetype rgbcolor "#DAA520" linewidth 3 + +set pointsize 0.6 + +set xrange [:12] + +plot \ + "current_density-4.dat" using 1:2 every ::1 with lines linestyle 1 title "$x=x_0$",\ + "current_density-4.dat" using 5:6 every ::1 with lines linestyle 2 title "$x=10x_0$" diff --git a/figs/plots.fig/density-8.gnuplot b/figs/plots.fig/density-8.gnuplot new file mode 100644 index 0000000..f107ff6 --- /dev/null +++ b/figs/plots.fig/density-8.gnuplot @@ -0,0 +1,44 @@ +## can also set the following options +set title "$E=8\\ \\mathrm{V}\\cdot\\mathrm{nm}^{-1}$" +set ylabel "$|\\psi|^2$" norotate +set xlabel "$t$ (fs)" +# +## start ticks at 0, then every x +#set xtics 0,x +#set ytics 0,x +## puts 4 minor tics between tics (5 intervals, i.e. every 0.01) +set mxtics 5 +set mytics 5 + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 12.5,8.75 standalone + +set key spacing 1.5 + +# 3=1+2 draw bottom and left sides of the box +set border 3 +# don't show tics on opposite sides +set xtics nomirror +set ytics nomirror + +# My colors +## 4169E1 (pastel blue) +## DC143C (bright red) +## 32CD32 (bright green) +## 4B0082 (deep purple) +## DAA520 (ochre) + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 3 +set style line 2 linetype rgbcolor "#DC143C" linewidth 3 +set style line 3 linetype rgbcolor "#32CD32" linewidth 3 +set style line 4 linetype rgbcolor "#4B0082" linewidth 3 +set style line 5 linetype rgbcolor "#DAA520" linewidth 3 + +set pointsize 0.6 + +set xrange [:12] + +plot \ + "current_density-8.dat" using 1:2 every ::1 with lines linestyle 1 title "$x=x_0$",\ + "current_density-8.dat" using 5:6 every ::1 with lines linestyle 2 title "$x=10x_0$" diff --git a/figs/plots.fig/integrated_current-4.gnuplot b/figs/plots.fig/integrated_current-4.gnuplot new file mode 100644 index 0000000..7e9dd6b --- /dev/null +++ b/figs/plots.fig/integrated_current-4.gnuplot @@ -0,0 +1,43 @@ +## can also set the following options +set title "$E=4\\ \\mathrm{V}\\cdot\\mathrm{nm}^{-1}$" +set ylabel "$\\displaystyle\\frac J{k^2}$" norotate +set xlabel "$t$ (fs)" +# +## start ticks at 0, then every x +#set xtics 0,x +#set ytics 0,x +## puts 4 minor tics between tics (5 intervals, i.e. every 0.01) +set mxtics 5 +set mytics 5 + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 12.5,8.75 standalone + +set key spacing 1.5 + +# 3=1+2 draw bottom and left sides of the box +set border 3 +# don't show tics on opposite sides +set xtics nomirror +set ytics nomirror + +# My colors +## 4169E1 (pastel blue) +## DC143C (bright red) +## 32CD32 (bright green) +## 4B0082 (deep purple) +## DAA520 (ochre) + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 3 +set style line 2 linetype rgbcolor "#DC143C" linewidth 3 +set style line 3 linetype rgbcolor "#32CD32" linewidth 3 +set style line 4 linetype rgbcolor "#4B0082" linewidth 3 +set style line 5 linetype rgbcolor "#DAA520" linewidth 3 + +set pointsize 0.6 + +set xrange [:12] + +plot "current_density-4.dat" using 1:4 every ::1 with lines linestyle 1 title "$x=x_0$",\ + "current_density-4.dat" using 5:8 every ::1 with lines linestyle 2 title "$x=10x_0$" diff --git a/figs/plots.fig/integrated_current-8.gnuplot b/figs/plots.fig/integrated_current-8.gnuplot new file mode 100644 index 0000000..3d5d501 --- /dev/null +++ b/figs/plots.fig/integrated_current-8.gnuplot @@ -0,0 +1,43 @@ +## can also set the following options +set title "$E=4\\ \\mathrm{V}\\cdot\\mathrm{nm}^{-1}$" +set ylabel "$\\displaystyle\\frac J{k^2}$" norotate +set xlabel "$t$ (fs)" +# +## start ticks at 0, then every x +#set xtics 0,x +#set ytics 0,x +## puts 4 minor tics between tics (5 intervals, i.e. every 0.01) +set mxtics 5 +set mytics 5 + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 12.5,8.75 standalone + +set key spacing 1.5 + +# 3=1+2 draw bottom and left sides of the box +set border 3 +# don't show tics on opposite sides +set xtics nomirror +set ytics nomirror + +# My colors +## 4169E1 (pastel blue) +## DC143C (bright red) +## 32CD32 (bright green) +## 4B0082 (deep purple) +## DAA520 (ochre) + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 3 +set style line 2 linetype rgbcolor "#DC143C" linewidth 3 +set style line 3 linetype rgbcolor "#32CD32" linewidth 3 +set style line 4 linetype rgbcolor "#4B0082" linewidth 3 +set style line 5 linetype rgbcolor "#DAA520" linewidth 3 + +set pointsize 0.6 + +set xrange [:12] + +plot "current_density-8.dat" using 1:4 every ::1 with lines linestyle 1 title "$x=x_0$",\ + "current_density-8.dat" using 5:8 every ::1 with lines linestyle 2 title "$x=10x_0$" |