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diff --git a/Jauslin_Milan_2022.tex b/Jauslin_Milan_2022.tex new file mode 100644 index 0000000..f0f8433 --- /dev/null +++ b/Jauslin_Milan_2022.tex @@ -0,0 +1,430 @@ +\documentclass{ian-presentation} + +\usepackage[hidelinks]{hyperref} +\usepackage{graphicx} +\usepackage{array} +\usepackage{xcolor} + + +\definecolor{ipurple}{HTML}{4B0082} +\definecolor{iyellow}{HTML}{DAA520} +\definecolor{igreen}{HTML}{32CD32} +\definecolor{iblue}{HTML}{4169E1} +\definecolor{ired}{HTML}{DC143C} + +\definecolor{highlight}{HTML}{328932} +\definecolor{highlight}{HTML}{981414} + +\begin{document} +\pagestyle{empty} +\hbox{}\vfil +\bf\Large +\hfil An effective equation to study Bose gases\par +\smallskip +\hfil at all densities\par +\vfil +\large +\hfil Ian Jauslin +\normalsize +\vfil +\hfil\rm joint with {\bf Eric A. Carlen}, {\bf Markus Holzmann}, {\bf Elliott H. Lieb}\par +\vfil +arXiv:{\tt\ \parbox[b]{3cm}{ + \href{https://arxiv.org/abs/1912.04987}{1912.04987}\par + \href{https://arxiv.org/abs/2010.13882}{2010.13882}\par + \href{https://arxiv.org/abs/2011.10869}{2011.10869}\par + \href{https://arxiv.org/abs/2202.07637}{2202.07637} +}} +\hfill{\tt \href{http://ian.jauslin.org}{http://ian.jauslin.org}} +\eject + +\setcounter{page}1 +\pagestyle{plain} + +\title{Bose-Einstein condensation} +\begin{itemize} +\item System of many Bosons, e.g. {\color{highlight}Helium} atoms, {\color{highlight}Rubidium} atoms, etc... +\item {\color{highlight}Bose-Einstein condensate}: most particles are in the same quantum state. +\item Related to the phenomena of {\color{highlight}superfluidity} (flow with zero viscocity) and {\color{highlight}superconductivity} (currents with zero resistance). +\item Predicted theoretically in {\color{highlight}1924-1925}, experimentally observed in {\color{highlight}1995}. +\item Mathematical understanding: still {\color{highlight}no proof} of the existence of a condensate (at finite density, in the presence of interactions and in the continuum). +\end{itemize} +\vfill +\eject + +\title{Repulsive Bose gas} +\begin{itemize} + \item Potential: {\color{highlight}$v(r)\geqslant 0$} and {\color{highlight}$v\in L_1(\mathbb R^3)$}, Hamiltonian: + $$ + H_N:= + -\frac12\sum_{i=1}^N\Delta_i + +\sum_{1\leqslant i<j\leqslant N}v(|x_i-x_j|) + $$ + \vskip-5pt + \item Ground state: $\psi_0$, energy $E_0$. + \item Observables in the {\color{highlight}thermodynamic limit}: ground state energy per particle and condensate fraction: $P_i$: projection onto condensate state + $$ + e_0:=\lim_{\displaystyle\mathop{\scriptstyle V,N\to\infty}_{{\color{highlight}\frac NV=\rho}}}\frac{E_0}N + ,\quad + \eta_0:=\lim_{\displaystyle\mathop{\scriptstyle V,N\to\infty}_{{\color{highlight}\frac NV=\rho}}}\frac1N\sum_{i=1}^N\left<\psi_0\right|P_i\left|\psi_0\right> + . + $$ +\end{itemize} +\vfill +\eject + +\title{Low density} +\begin{itemize} + \item Bogolyubov theory: {\color{highlight}approximation scheme} that reduces the problem to an effective {\color{highlight}1-particle problem}. + \item Predictions \href{https://doi.org/10.1103/PhysRev.106.1135}{[Lee, Huang, Yang, 1957]}: + \begin{itemize} + \item Energy: + $$ + {\color{highlight}e_0=2\pi\rho a\left(1+\frac{128}{15\sqrt\pi}\sqrt{\rho a^3}+o(\sqrt\rho)\right)} + $$ + \vskip-10pt + \item Condensate fraction: + $$ + {\color{highlight}1-\eta_0\sim\frac{8\sqrt{\rho a^3}}{3\sqrt\pi}} + $$ + \end{itemize} +\end{itemize} +\vfill +\eject + +\title{Low density} +\begin{itemize} + \item Energy asymptotics: {\color{highlight} proved}: + \href{https://doi.org/10.1103/PhysRevLett.80.2504}{[Lieb, Yngvason, 1998]}, + \href{https://doi.org/10.1007/s10955-009-9792-3}{[Yau, Yin, 2009]}, + \href{https://doi.org/10.4007/annals.2020.192.3.5}{[Fournais, Solovej, 2020]}. + + \item Condensate fraction: {\color{highlight}still open} in the theormodynamic limit, but there are proofs of condensation in the Gross-Pitaevskii regime (ultra-dilute): + \href{https://doi.org/10.1103/PhysRevLett.88.170409}{[Lieb, Seiringer, 2002]}, + \href{https://doi.org/10.1007/s00220-017-3016-5}{[Boccato, Brennecke, Cenatiempo, Schlein, 2018]}. + +\end{itemize} +\vfill +\eject + +\title{High density} +\begin{itemize} + \item [Bogolyubov, 1947]: if $\hat v\geqslant 0$. + $$ + {\color{highlight}e_0\sim\frac\rho2\int v} + $$ + {\color{highlight}Hartree} (mean field) energy. + \item {\color{highlight}Proved} in \href{https://doi.org/10.1103/PhysRev.130.2518}{[Lieb, 1963]}. + \item Condensate fraction + $$ + \eta\to1 + $$ + {\color{highlight}open}. +\end{itemize} +\vfill +\eject + +\title{Energy as a function of density} +For $v(x)=e^{-|x|}$: + +\hfil\includegraphics[height=5.5cm]{erho_lowhigh.pdf} +\vfill +\eject + +\addtocounter{page}{-1} +\title{Energy as a function of density} +For $v(x)=e^{-|x|}$: + +\hfil\includegraphics[height=5.5cm]{erho_effective.pdf} +\vfill +\eject + +\title{Derivation of the equation} +\begin{itemize} + \item \href{https://doi.org/10.1103/PhysRev.130.2518}{[Lieb, 1963]}. + \item Integrate $H_N\psi_0=E_0\psi_0$: + $$ + \int dx_1\cdots dx_N\ + \left( + -\frac12\sum_{i=1}^N\Delta_i\psi_0 + +\sum_{1\leqslant i<j\leqslant N} v(x_i-x_j)\psi_0 + \right) + =E_0\int dx_1\cdots dx_N\ \psi_0 + $$ + \item Therefore, + $$ + \frac{N(N-1)}2\int dx_1dx_2\ v(x_1-x_2)\frac{\int dx_3\cdots dx_N\ \psi_0}{\int dx_1\cdots dx_N\ \psi_0} + =E_0 + $$ +\end{itemize} +\vfill +\eject + +\title{Derivation of the equation} +\begin{itemize} + \item Thus, + $$ + \frac{E_0}N=\frac{N-1}{2V}\int dx\ v(x)g_2(0,x) + $$ + \item {\color{highlight}$\psi_0\geqslant 0$}, so it can be thought of as a probability distribution. + \item $g_n$: {\color{highlight}correlation functions} of $V^{-N}\psi_0$ + $$ + g_n(x_1,\cdots,x_n):=\frac{V^n\int dx_{n+1}\cdots dx_N\ \psi_0(x_1,\cdots,x_N)}{\int dx_1\cdots dx_N\ \psi_0(x_1,\cdots,x_N)} + $$ +\end{itemize} +\vfill +\eject + +\title{Hierarchy} +\vskip-10pt +\begin{itemize} + \item Equation for $g_2$: integrate $H_N\psi_0=E_0\psi_0$ with respect to $x_3,\cdots,x_N$: + $$ + \begin{array}{>\displaystyle l} + -\frac12(\Delta_x+\Delta_y) g_2(x,y) + +\frac{N-2}V\int dz\ (v(x-z)+v(y-z))g_3(x,y,z) + \\[0.5cm]\hfill + +v(x-y)g_2(x,y) + +\frac{(N-2)(N-3)}{2V^2}\int dzdt\ v(z-t)g_4(x,y,z,t) + =E_0g_2(x,y) + \end{array} + $$ + \item Factorization {\color{highlight}assumption}: + $$ + g_3(x_1,x_2,x_3)=g_2(x_1,x_2)g_2(x_1,x_3)g_2(x_2,x_3) + $$ + $$ + g_4(x_1,x_2,x_3,x_4)=\prod_{i<j}(g_2(x_i,x_j)+O(V^{-1})) + $$ +\end{itemize} +\vfill +\eject + +\title{{\color{ipurple}Big equation}} +\begin{itemize} +\item In the thermodynamic limit, if ${\color{highlight}u(x):=1-g_2(0,x)}$, + $$ + -\Delta u(x) + = + (1-u(x))\left(v(x)-2\rho K(x)+\rho^2 L(x)\right) + $$ + $$ + K:= + u\ast S + ,\quad + S(y):=(1-u(y))v(y) + $$ + $$ + L:= + u\ast u\ast S + -2u\ast(u(u\ast S)) + +\frac12 + \int dydz\ u(y)u(z-x)u(z)u(y-x)S(z-y) + . + $$ + + \item {\color{ipurple}``Big'' equation}: + $$ + L\approx + u\ast u\ast S + -2u\ast (u(u\ast S)) + $$ +\end{itemize} +\vfill +\eject + +\title{{\color{iblue}Simple equation}} +\vskip-10pt +\begin{itemize} + \item Further approximate $S(x)\approx\frac{2e}\rho\delta(x)$ and $u\ll 1$. + \item Simple equation + $$ + {\color{iblue}-\Delta u(x)=(1-u(x))v(x)- 4eu(x)+2e\rho\ u\ast u(x)} + $$ + $$ + {\color{iblue}e=\frac\rho2\int dx\ (1-u(x))v(x)} + $$ + \item {\bf Theorem 1}: + If $v(x)\geqslant 0$ and $v\in L_1\cap L_2(\mathbb R^3)$, then the {\color{iblue}simple equation} has an {\color{highlight}integrable solution} (proved constructively), with $0\leqslant u\leqslant 1$. +\end{itemize} +\vfill +\eject + +\title{Energy for the {\color{iblue}simple equation}} +\vskip-10pt +\begin{itemize} + \item {\bf Theorem 2}: + $$ + \frac{e}{\rho}\mathop{\longrightarrow}_{\rho\to\infty}\frac12\int dx\ v(x) + $$ + (note that there is no condition that $\hat v\geqslant 0$). + This coincides with the {\color{highlight}Hartree energy}. + \item {\bf Theorem 3}: + $$ + e=2\pi\rho a\left(1+\frac{128}{15\sqrt\pi}\sqrt{\rho a^3}+o(\sqrt\rho)\right) + $$ + This coincides with the {\color{highlight}Lee-Huang-Yang prediction}. +\end{itemize} +\vfill +\eject + +\title{Energy} +$v(x)=e^{-|x|}$, Blue: {\color{iblue}simple equation}; purple: {\color{ipurple}big equation}; red: {\color{ired}Monte Carlo} + +\hfil\includegraphics[height=5.5cm]{erho_fulleq.pdf} +\vfill +\eject + +\title{Energy} +$v(x)=e^{-|x|}$, Blue: {\color{iblue}simple equation}; red: {\color{ired}Jastrow}; purple: {\color{ipurple}big equation} + +\hfil\includegraphics[height=5.5cm]{cmp_energy1.pdf} +\vfill +\eject + +\title{Condensate fraction} +\begin{itemize} + \item Add a parameter $\mu$ to the Hamiltonian: + $$ + H_N(\mu):= + -\frac12\sum_{i=1}^N\Delta_i + +\sum_{1\leqslant i<j\leqslant N}v(x_i-x_j) + {\color{highlight}-\mu\sum_{i=1}^NP_i} + $$ + \item Projection onto condensate wavefunction: $P_i$. + \item Condensate fraction: + $$ + {\color{highlight}\eta_0}:=\frac1N\left<\psi_0\right|\sum_{i=1}^NP_i\left|\psi_0\right> + =-\frac1N\partial_\mu \left<\psi_0\right|H_N(\mu)\left|\psi_0\right>|_{\mu_0} + \equiv + {\color{highlight}-\partial_\mu e_0(\mu)|_{\mu=0}} + $$ +\end{itemize} +\vfill +\eject + +\title{Condensate fraction} +\begin{itemize} + \item {\bf Theorem 4}: + For the {\color{iblue}simple equation}, as $\rho\to0$ + $$ + 1-\eta\sim\frac{8\sqrt{\rho a^3}}{3\sqrt\pi} + $$ + which coincides with {\color{highlight}Bogolyubov's prediction}. +\end{itemize} +\vfill +\eject + +\title{Condensate fraction} +$v(x)=e^{-|x|}$, Blue: {\color{iblue}simple equation}; purple: {\color{ipurple}big equation}; red: {\color{ired}Monte Carlo} + +\hfil\includegraphics[height=5.5cm]{condensate.pdf} +\vfill +\eject + +\title{Two point correlation function} +$v(x)=16e^{-|x|}$, Blue: {\color{iblue}simple equation}; purple: {\color{ipurple}big equation}; red: {\color{ired}Monte Carlo} + +\hfil\includegraphics[height=5.5cm]{correlation.pdf} +\vfill +\eject + +\title{Summary and outlook} +\begin{itemize} + \item Two {\color{highlight}effective equations}: the {\color{ipurple}big equation} and the {\color{iblue}simple equation}, which are {\color{highlight}non-linear 1-particle equations}. + \item Reproduce the known results for both {\color{highlight}small and large densities}. + \item Their derivation is {\color{highlight}different from Bogolyubov theory}, so they may give new insights onto studying the Bose gas in these asymptotic regimes. + \item The {\color{ipurple}big equation} is {\color{highlight}quantitatively accurate} at intermediate densities. + \item This opens up the possibility of studying the physics of the {\color{highlight}Bose gas at intermediate densities}. +\end{itemize} +\vfill +\eject + +\title{Open problems} +\vfill +\begin{itemize} + \item {\color{highlight}Uniqueness} of the solution of the {\color{iblue}simple equation} (done for small and large $\rho$). + \vfill + + \item LHY as an {\color{highlight}upper bound} at low density using the {\color{iblue}simple equation} to construct an Ansatz. + \vfill + + \item {\color{highlight}Existence} (and uniqueness) of the solution of the {\color{ipurple}big equation}. + +\end{itemize} +\vfill +\eject + +\title{The uniqueness problem} + $$ + -\Delta u(x)=(1-u(x))v(x)- 4eu(x)+2e\rho\ u\ast u(x) + ,\quad + e=\frac\rho2\int dx\ (1-u(x))v(x) + $$ +\begin{itemize} + \item Change the point of view: {\color{highlight}fix $e>0$}, and compute $\rho$ and $u$. + + \item {\color{highlight}Iteration}: $u_0=0$, + $$ + (-\Delta+4e+v)u_n=v+2e\rho_{n-1}u_{n-1}\ast u_{n-1} + ,\quad + \rho_n:=\frac{2e}{\int dx\ (1-u_n(x))v(x)} + . + $$ +\end{itemize} +\vfill +\eject + +\title{The uniqueness problem} +\begin{itemize} + \item {\bf Lemma}: $u_n(x)$ is an {\color{highlight}increasing} sequence, and is {\color{highlight}bounded} $u_n(x)\leqslant 1$. + It converges to a function $u$, which is the {\color{highlight}unique} integrable solution of the equation {\color{highlight}with $e$ fixed}. + + \item {\bf Lemma}: $e\mapsto\rho(e)$ is {\color{highlight}continuous}, and $\rho(0)=0$ and $\rho(\infty)=\infty$, which allows us to compute solutions for the problem at fixed $\rho$. + + \item We thus have a {\color{highlight}restricted} notion of uniqueness. + The full uniqueness would follow from a proof that $e\mapsto\rho(r)$ is {\color{highlight}monotone increasing} (which must be true for the physics to make sense). +\end{itemize} +\vfill +\eject + +\title{Upper bound at low density} +\begin{itemize} + \item \href{https://doi.org/10.1007/s10955-009-9792-3}{[Yau, Yin, 2009]}: proof for {\color{highlight}weak, smooth}, rapidly decaying potentials. + \item \href{https://arxiv.org/abs/2101.06222}{[Basti, Cenatiempo, Schlein, 2021]}: extended for {\color{highlight}$L_3$} (and compactly supported) potentials (excludes hard-core interactions). + \item {\color{iblue}Simple Equation}: our analysis holds for the hard-core, so if one could find a good {\color{highlight}Ansatz} from it, one might get an upper bound for the energy in this case. + \item Idea for Ansatz? (Jastrow, Dyson-Jastrow?). +\end{itemize} +\vfill +\eject + +\title{Upper bound at low density: Jastrow function} +\begin{itemize} + \item Idea: + $$ + \psi=\prod_{i<j}e^{-u(x_i-x_j)} + $$ + + \item Why this: $\rho\ll1$, and {\color{highlight}if $\rho\|u\|_1\ll1$}, + $$ + g_2\sim1-u + . + $$ + + \item Again, {\color{highlight}if $\rho\|u\|_1\ll1$}, we would be able to compute the energy of $\psi$ using a cluster expansion! + + \item However, {\color{highlight}$\|u\|_1=\frac1\rho$}! +\end{itemize} +\vfill +\eject + +\title{Existence for the {\color{ipurple}Big Equation}} +\begin{itemize} + \item Numerical method: {\color{highlight}Newton algorithm}. + + \item For the existence of a solution, it would suffice to prove that the Newton algorithm has a {\color{highlight}Basin of attraction}. (Kantorovich-like theorem?) + + \item Such a result, applied to the {\color{iblue}Simple Equation}, would imply the {\color{highlight}uniqueness} of a solution (provided we have convergence in an appropriate norm). +\end{itemize} + +\end{document} diff --git a/Makefile b/Makefile new file mode 100644 index 0000000..94f61ff --- /dev/null +++ b/Makefile @@ -0,0 +1,47 @@ +PROJECTNAME=$(basename $(wildcard *.tex)) +LIBS=$(notdir $(wildcard libs/*)) +FIGS=$(notdir $(wildcard figs/*.fig)) + +PDFS=$(addsuffix .pdf, $(PROJECTNAME)) +SYNCTEXS=$(addsuffix .synctex.gz, $(PROJECTNAME)) + +all: $(PROJECTNAME) + +$(PROJECTNAME): $(LIBS) $(FIGS) + pdflatex -file-line-error $@.tex + pdflatex -synctex=1 $@.tex + +$(SYNCTEXS): $(LIBS) $(FIGS) + pdflatex -synctex=1 $(patsubst %.synctex.gz, %.tex, $@) + +$(LIBS): + ln -fs libs/$@ ./ + + +figs: $(FIGS) + +$(FIGS): + make -C figs/$@ + for pdf in $$(find figs/$@/ -name '*.pdf'); do ln -fs "$$pdf" ./ ; done + + +clean-aux: clean-figs-aux + rm -f $(addsuffix .aux, $(PROJECTNAME)) + rm -f $(addsuffix .log, $(PROJECTNAME)) + rm -f $(addsuffix .out, $(PROJECTNAME)) + +clean-libs: + rm -f $(LIBS) + +clean-figs: + $(foreach fig,$(addprefix figs/, $(FIGS)), make -C $(fig) clean; ) + rm -f $(notdir $(wildcard figs/*.fig/*.pdf)) + +clean-figs-aux: + $(foreach fig,$(addprefix figs/, $(FIGS)), make -C $(fig) clean-aux; ) + + +clean-tex: + rm -f $(PDFS) $(SYNCTEXS) + +clean: clean-aux clean-tex clean-libs clean-figs @@ -0,0 +1,33 @@ +This directory contains the source files to typeset the presentation, and +generate the figures. This can be accomplished by running + make + +This document uses a custom class file, located in the 'libs' directory, which +defines a number of commands. + + +* Dependencies: + + pdflatex + TeXlive packages: + amsfonts + array + graphics + hyperref + latex + pgf + standalone + GNU make + gnuplot + +* Files: + + Jauslin_Milan_2022.tex: + main LaTeX file + + libs: + custom LaTeX class file + + figs: + source code for the figures + diff --git a/figs/condensate.fig/Makefile b/figs/condensate.fig/Makefile new file mode 100644 index 0000000..c45de65 --- /dev/null +++ b/figs/condensate.fig/Makefile @@ -0,0 +1,34 @@ +PROJECTNAME=condensate + +PDFS=$(addsuffix .pdf, $(PROJECTNAME)) +DATS= simpleq.dat bigeq.dat + +all: $(PDFS) + +$(PDFS): $(DATS) + gnuplot $(patsubst %.pdf, %.gnuplot, $@) > $(patsubst %.pdf, %.tikz.tex, $@) + pdflatex -jobname $(basename $@) -file-line-error $(patsubst %.pdf, %.tikz.tex, $@) + +simpleq.dat: + julia $(SIMPLEQ)/main.jl -p "tolerance=1e-11;order=100;maxiter=100;v_a=1" -M simpleq condensate_fraction > $@ +bigeq.dat: + julia -p 8 $(SIMPLEQ)/main.jl -p "eq=bigeq;N=12;P=8;v_a=1" -M medeq condensate_fraction > $@ + +install: $(PDFS) + cp $^ $(INSTALLDIR)/ + +$(LIBS): + ln -fs libs/$@ ./ + +clean-libs: + rm -f $(LIBS) + +clean-aux: + rm -f $(addsuffix .aux, $(PROJECTNAME)) + rm -f $(addsuffix .log, $(PROJECTNAME)) + rm -f $(addsuffix .tex, $(PROJECTNAME)) + +clean-tex: + rm -f $(PDFS) + +clean: clean-libs clean-aux clean-tex diff --git a/figs/condensate.fig/bigeq.dat b/figs/condensate.fig/bigeq.dat new file mode 100644 index 0000000..e48cbc3 --- /dev/null +++ b/figs/condensate.fig/bigeq.dat @@ -0,0 +1,100 @@ + 1.000000000000000e-06 1.942109602248065e-03 1.702970665674168e-12 + 1.202264434617413e-06 2.144142093189251e-03 1.178808810520995e-13 + 1.445439770745928e-06 2.370859341242408e-03 1.192336354552407e-12 + 1.737800828749376e-06 2.623985546948715e-03 4.076932518598860e-12 + 2.089296130854041e-06 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+unset mxtics + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 8,6 standalone + +set key off + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 2 +set style line 2 linetype rgbcolor "#DC143C" linewidth 2 +set style line 3 linetype rgbcolor "#32CD32" linewidth 2 +set style line 4 linetype rgbcolor "#4B0082" linewidth 2 +set style line 5 linetype rgbcolor "#DAA520" linewidth 2 + +set pointsize 0.6 + +set label at 0.000005,0.91 "Bogolyubov" textcolor "#32CD32" + +set logscale x + +a=1.25435641059 + +plot "simpleq.dat" u 1:(1-$2) w l ls 1, \ + "bigeq.dat" u 1:(1-$2) w l ls 4 , \ + 1-8/(3*sqrt(pi))*sqrt(x*a**3) linestyle 3 dashtype "." ,\ + "holzmann_2019-12-25.dat" u 1:(1-$3) ls 2 diff --git a/figs/condensate.fig/condensate.pdf b/figs/condensate.fig/condensate.pdf Binary files differnew file mode 100644 index 0000000..9e965a4 --- /dev/null +++ b/figs/condensate.fig/condensate.pdf diff --git a/figs/condensate.fig/condensate.tikz.tex b/figs/condensate.fig/condensate.tikz.tex new file mode 100644 index 0000000..4f7da70 --- /dev/null +++ b/figs/condensate.fig/condensate.tikz.tex @@ -0,0 +1,142 @@ +\documentclass[10pt]{article} +\usepackage[T1]{fontenc} +\usepackage{textcomp} + +\usepackage[utf8x]{inputenc} +\SetUnicodeOption{mathletters} + +\usepackage{gnuplot-lua-tikz} +\pagestyle{empty} +\usepackage[active,tightpage]{preview} +\PreviewEnvironment{tikzpicture} +\setlength\PreviewBorder{\gpbboxborder} +\begin{document} + +\begin{tikzpicture}[gnuplot] +%% generated with GNUPLOT 5.4p2 (Lua 5.4; terminal rev. 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+%% coordinates of the plot area +\gpdefrectangularnode{gp plot 1}{\pgfpoint{1.748cm}{0.985cm}}{\pgfpoint{7.447cm}{5.691cm}} +\end{tikzpicture} +%% gnuplot variables +\end{document} diff --git a/figs/condensate.fig/holzmann_2019-12-25.dat b/figs/condensate.fig/holzmann_2019-12-25.dat new file mode 100644 index 0000000..96689cb --- /dev/null +++ b/figs/condensate.fig/holzmann_2019-12-25.dat @@ -0,0 +1,11 @@ +## data from M. Holzmann, 2019-09-22 +# rho E0 n0 +1e-6 7.902e-6 +1e-4 8.3441e-4 0.0171 +1e-3 9.13384e-3 0.0481 +1e-2 1.061073e-1 0.0871 +1e-1 1.19182e+0 0.0851 +1e-0 1.24302e+1 0.0587 +1e+1 1.25442e+2 0.0319 +5e+1 6.28032e+2 0.021 + diff --git a/figs/condensate.fig/simpleq.dat b/figs/condensate.fig/simpleq.dat new file mode 100644 index 0000000..348121c --- /dev/null +++ b/figs/condensate.fig/simpleq.dat @@ -0,0 +1,100 @@ + 1.000000000000000e-06 2.095081711925015e-03 + 1.202264434617413e-06 2.295235280091131e-03 + 1.445439770745928e-06 2.514296186738034e-03 + 1.737800828749376e-06 2.754005992218143e-03 + 2.089296130854041e-06 3.016257261240048e-03 + 2.511886431509582e-06 3.303104592145314e-03 + 3.019951720402019e-06 3.616775975726918e-03 + 3.630780547701017e-06 3.959684344305409e-03 + 4.365158322401657e-06 4.334439155646415e-03 + 5.248074602497723e-06 4.743857767750661e-03 + 6.309573444801930e-06 5.190976310677877e-03 + 7.585775750291836e-06 5.679059686385030e-03 + 9.120108393559096e-06 6.211610171947045e-03 + 1.096478196143185e-05 6.792374027485015e-03 + 1.318256738556407e-05 7.425345312781278e-03 + 1.584893192461114e-05 8.114765932045185e-03 + 1.905460717963248e-05 8.865120699464721e-03 + 2.290867652767775e-05 9.681125931789915e-03 + 2.754228703338163e-05 1.056770975064344e-02 + 3.311311214825908e-05 1.152998189333092e-02 + 3.981071705534969e-05 1.257319039145271e-02 + 4.786300923226380e-05 1.370266197723624e-02 + 5.754399373371566e-05 1.492372253381352e-02 + 6.918309709189363e-05 1.624159332185176e-02 + 8.317637711026709e-05 1.766125812610249e-02 + 1.000000000000000e-04 1.918729591875359e-02 + 1.202264434617413e-04 2.082367319967555e-02 + 1.445439770745928e-04 2.257348995912804e-02 + 1.737800828749376e-04 2.443867336254203e-02 + 2.089296130854039e-04 2.641961398528058e-02 + 2.511886431509580e-04 2.851474099050601e-02 + 3.019951720402016e-04 3.072003537104471e-02 + 3.630780547701014e-04 3.302848464372067e-02 + 4.365158322401661e-04 3.542948859291789e-02 + 5.248074602497728e-04 3.790823417663501e-02 + 6.309573444801930e-04 4.044506877087432e-02 + 7.585775750291835e-04 4.301491450154334e-02 + 9.120108393559096e-04 4.558678199565728e-02 + 1.096478196143185e-03 4.812345827946150e-02 + 1.318256738556408e-03 5.058145864328128e-02 + 1.584893192461114e-03 5.291134289200051e-02 + 1.905460717963246e-03 5.505849827399160e-02 + 2.290867652767772e-03 5.696447960043553e-02 + 2.754228703338166e-03 5.856896678930269e-02 + 3.311311214825911e-03 5.981234782238041e-02 + 3.981071705534973e-03 6.063886048364867e-02 + 4.786300923226385e-03 6.100013371714988e-02 + 5.754399373371567e-03 6.085886970213172e-02 + 6.918309709189363e-03 6.019231791545348e-02 + 8.317637711026709e-03 5.899513433487237e-02 + 1.000000000000000e-02 5.728121486315967e-02 + 1.202264434617413e-02 5.508415858187780e-02 + 1.445439770745928e-02 5.245615721904299e-02 + 1.737800828749376e-02 4.946530746709376e-02 + 2.089296130854041e-02 4.619156855992348e-02 + 2.511886431509582e-02 4.272179185226004e-02 + 3.019951720402019e-02 3.914438480508303e-02 + 3.630780547701010e-02 3.554420649152192e-02 + 4.365158322401656e-02 3.199821953636445e-02 + 5.248074602497723e-02 2.857226663349834e-02 + 6.309573444801930e-02 2.531914059520501e-02 + 7.585775750291836e-02 2.227792229852985e-02 + 9.120108393559097e-02 1.947440831436047e-02 + 1.096478196143185e-01 1.692235880228233e-02 + 1.318256738556407e-01 1.462526717442258e-02 + 1.584893192461114e-01 1.257837345877809e-02 + 1.905460717963248e-01 1.077069465848733e-02 + 2.290867652767775e-01 9.186909564013418e-03 + 2.754228703338169e-01 7.808998508205012e-03 + 3.311311214825908e-01 6.617591964706389e-03 + 3.981071705534969e-01 5.593022042416338e-03 + 4.786300923226380e-01 4.716097668760250e-03 + 5.754399373371566e-01 3.968639441621027e-03 + 6.918309709189363e-01 3.333816454742892e-03 + 8.317637711026709e-01 2.796327604398189e-03 + 1.000000000000000e+00 2.342466331442259e-03 + 1.202264434617413e+00 1.960102269258443e-03 + 1.445439770745928e+00 1.638607138480099e-03 + 1.737800828749376e+00 1.368746272215081e-03 + 2.089296130854041e+00 1.142551829784601e-03 + 2.511886431509582e+00 9.531892670181336e-04 + 3.019951720402019e+00 7.948250154423670e-04 + 3.630780547701010e+00 6.625005224425910e-04 + 4.365158322401657e+00 5.520157121243856e-04 + 5.248074602497723e+00 4.598234179345307e-04 + 6.309573444801930e+00 3.829352915009887e-04 + 7.585775750291836e+00 3.188389988971121e-04 + 9.120108393559097e+00 2.654260840747906e-04 + 1.096478196143185e+01 2.209296357978901e-04 + 1.318256738556407e+01 1.838707817059403e-04 + 1.584893192461114e+01 1.530130079086820e-04 + 1.905460717963248e+01 1.273233330370514e-04 + 2.290867652767775e+01 1.059394293104648e-04 + 2.754228703338169e+01 8.814186420712528e-05 + 3.311311214825908e+01 7.333072418003886e-05 + 3.981071705534969e+01 6.100596972384632e-05 + 4.786300923226381e+01 5.075095479639026e-05 + 5.754399373371567e+01 4.221862079919067e-05 + 6.918309709189363e+01 3.511994492291246e-05 + 8.317637711026708e+01 2.921428437169262e-05 diff --git a/figs/condensate16.fig/.energy16.gnuplot.swp b/figs/condensate16.fig/.energy16.gnuplot.swp Binary files differnew file mode 100644 index 0000000..d23db08 --- /dev/null +++ b/figs/condensate16.fig/.energy16.gnuplot.swp diff --git a/figs/condensate16.fig/2020-05-22+16.dat b/figs/condensate16.fig/2020-05-22+16.dat new file mode 100644 index 0000000..c28285d --- /dev/null +++ b/figs/condensate16.fig/2020-05-22+16.dat @@ -0,0 +1,7 @@ +# rho E0 n0 + 1e-3 0.05195 0.61 + 5e-3 0.449 0.40 + 1e-2 1.1335 0.34 + 2e-2 2.748 0.33 + 1e-1 17.797 0.43 + 1e+0 197.35 0.70 diff --git a/figs/condensate16.fig/Makefile b/figs/condensate16.fig/Makefile new file mode 100644 index 0000000..d44f73c --- /dev/null +++ b/figs/condensate16.fig/Makefile @@ -0,0 +1,35 @@ +PROJECTNAME=condensate16 + +SIMPLEQ=~/Work/Research/2018+bose_gas/cmp/simpleq + +DATS=simpleq16.dat medeq16.dat +PDFS=$(addsuffix .pdf, $(PROJECTNAME)) +TEXS=$(addsuffix .tikz.tex, $(PROJECTNAME)) + +all: $(PDFS) + +$(PDFS): $(DATS) + gnuplot $(patsubst %.pdf, %.gnuplot, $@) > $(patsubst %.pdf, %.tikz.tex, $@) + pdflatex -jobname $(basename $@) -file-line-error $(patsubst %.pdf, %.tikz.tex, $@) + +simpleq16.dat: + julia $(SIMPLEQ)/main.jl -p "tolerance=1e-11;order=100;maxiter=100;v_a=16" -M simpleq condensate_fraction > $@ +medeq16.dat: + julia -p 8 $(SIMPLEQ)/main.jl -p "aK=1;aL1=1;aL2=1;aL3=0;bK=1;bL1=1;bL2=1;gK=1;gL2=1;gL3=0;N=12;P=8;v_a=16" -M medeq condensate_fraction > $@ + + +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 $(DATS) + +clean-tex: + rm -f $(PDFS) + +clean: clean-aux clean-tex diff --git a/figs/condensate16.fig/condensate16.gnuplot b/figs/condensate16.fig/condensate16.gnuplot new file mode 100644 index 0000000..e94eb1a --- /dev/null +++ b/figs/condensate16.fig/condensate16.gnuplot @@ -0,0 +1,34 @@ +set ylabel "$\\eta$" norotate offset -1,0 +set xlabel "$\\rho$" + +set xtics 1e-6, 100, 100 +set xtics add ("$10^{-6}$" 0.000001, "$10^{-4}$" 0.0001, "$10^{-2}$" 0.01, "$1$" 1.0, "$10^2$" 100) +unset mxtics + +#set ytics 0.6, 0.1 +set mytics 2 + +set xrange [0.000001:100] + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 8,6 standalone + +set key off + + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 2 +set style line 2 linetype rgbcolor "#DC143C" linewidth 2 +set style line 3 linetype rgbcolor "#32CD32" linewidth 2 +set style line 4 linetype rgbcolor "#4B0082" linewidth 2 +set style line 5 linetype rgbcolor "#DAA520" linewidth 2 + +set pointsize 1 + +set logscale x + +plot \ + "simpleq16.dat" using 1:($3<1e-5 ? 1-$2 : 1/0) with lines ls 1 ,\ + "medeq16.dat" using 1:($3<1e-5 ? 1-$2 : 1/0) with lines ls 4 ,\ + "2020-05-22+16.dat" using 1:3 with points ls 2 + diff --git a/figs/condensate16.fig/condensate16.pdf b/figs/condensate16.fig/condensate16.pdf Binary files differnew file mode 100644 index 0000000..0cc97fd --- /dev/null +++ b/figs/condensate16.fig/condensate16.pdf diff --git a/figs/condensate16.fig/medeq16.dat b/figs/condensate16.fig/medeq16.dat new file mode 100644 index 0000000..16ef72d --- /dev/null +++ b/figs/condensate16.fig/medeq16.dat @@ -0,0 +1,100 @@ + 1.000000000000000e-06 1.166000749536307e-02 1.397500557749096e-14 + 1.202264434617413e-06 1.294150659557208e-02 1.638378932477403e-14 + 1.445439770745928e-06 1.433395863576837e-02 2.068669778175053e-14 + 1.737800828749376e-06 1.585523520080719e-02 9.413457244472722e-15 + 2.089296130854041e-06 1.752468227078358e-02 2.147730951610164e-14 + 2.511886431509582e-06 1.936219857512355e-02 5.079185685242370e-14 + 3.019951720402019e-06 2.138821025238190e-02 4.890613903920614e-14 + 3.630780547701017e-06 2.362406333962305e-02 3.239855276438957e-14 + 4.365158322401657e-06 2.609258293662487e-02 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$(PROJECTNAME)) +TEXS=$(addsuffix .tikz.tex, $(PROJECTNAME)) + +all: $(PDFS) + +$(PDFS): $(DATS) + gnuplot $(patsubst %.pdf, %.gnuplot, $@) > $(patsubst %.pdf, %.tikz.tex, $@) + pdflatex -jobname $(basename $@) -file-line-error $(patsubst %.pdf, %.tikz.tex, $@) + +simpleq.dat: + julia $(SIMPLEQ)/main.jl -p "rho=2e-2;minlrho=-6;nlrho=60;eq=simpleq;N=12;P=8;xmax=10" -M medeq 2pt-simpleq > $@ +mueq.dat: + julia $(SIMPLEQ)/main.jl -p "rho=2e-2;minlrho=-6;nlrho=60;eq=mueq;N=12;P=8;xmax=10" -M medeq 2pt > $@ +bigeq.dat: + julia $(SIMPLEQ)/main.jl -p "rho=2e-2;minlrho=-6;nlrho=60;v_a=16;eq=bigeq;N=12;P=8;xmax=10" -M medeq 2pt > $@ + +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 $(DATS) + +clean-tex: + rm -f $(PDFS) + +clean: clean-aux clean-tex diff --git a/figs/correlation.fig/bigeq.dat b/figs/correlation.fig/bigeq.dat new file mode 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offset -1,0 +set xlabel "$|\\mathbf x|$" + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 8,6 standalone + +unset key + + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 2 +set style line 2 linetype rgbcolor "#DC143C" linewidth 1 +set style line 3 linetype rgbcolor "#32CD32" linewidth 2 +set style line 4 linetype rgbcolor "#4B0082" linewidth 2 +set style line 5 linetype rgbcolor "#DAA520" linewidth 2 +set style line 6 linetype rgbcolor "#555500" linewidth 2 + +set pointsize 0.5 + +rho=2e-2 + +plot \ + "simpleq.dat" using 1:($2/rho**2) with lines ls 1,\ + "bigeq.dat" using 1:($2/rho**2) with lines ls 4,\ + "2020-08-27+correlation.dat" using 1:2 ls 2 + diff --git a/figs/correlation.fig/correlation.pdf b/figs/correlation.fig/correlation.pdf Binary files differnew file mode 100644 index 0000000..9014dbf --- /dev/null +++ b/figs/correlation.fig/correlation.pdf diff --git a/figs/correlation.fig/mueq.dat b/figs/correlation.fig/mueq.dat new file 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3.998197942978559e-04 + 8.900000000000000e+00 3.998946829458393e-04 + 9.000000000000000e+00 3.999714677968415e-04 + 9.100000000000000e+00 4.000305881360316e-04 + 9.199999999999999e+00 4.000410500051843e-04 + 9.300000000000001e+00 4.000014391187070e-04 + 9.400000000000000e+00 3.999330105526194e-04 + 9.500000000000000e+00 3.998492973740165e-04 + 9.600000000000000e+00 3.997874738537067e-04 + 9.699999999999999e+00 3.997749691406509e-04 + 9.800000000000001e+00 3.998043912261032e-04 + 9.900000000000000e+00 3.998519077270098e-04 + 1.000000000000000e+01 3.998904866755104e-04 diff --git a/figs/energy.fig/Makefile b/figs/energy.fig/Makefile new file mode 100644 index 0000000..e8d3f12 --- /dev/null +++ b/figs/energy.fig/Makefile @@ -0,0 +1,28 @@ +PROJECTNAME=erho_effective erho_fulleq erho_lowhigh + +PDFS=$(addsuffix .pdf, $(PROJECTNAME)) + +all: $(PDFS) + +$(PDFS): + gnuplot $(patsubst %.pdf, %.gnuplot, $@) > $(patsubst %.pdf, %.tex, $@) + pdflatex -file-line-error $(patsubst %.pdf, %.tex, $@) + +install: $(PDFS) + cp $^ $(INSTALLDIR)/ + +$(LIBS): + ln -fs libs/$@ ./ + +clean-libs: + rm -f $(LIBS) + +clean-aux: + rm -f $(addsuffix .aux, $(PROJECTNAME)) + rm -f $(addsuffix .log, $(PROJECTNAME)) + rm -f $(addsuffix .tex, $(PROJECTNAME)) + +clean-tex: + rm -f $(PDFS) + +clean: clean-libs clean-aux clean-tex diff --git a/figs/energy.fig/erho.dat b/figs/energy.fig/erho.dat new file mode 100644 index 0000000..837439f --- /dev/null +++ b/figs/energy.fig/erho.dat @@ -0,0 +1,104 @@ + # v(x)=exp(-|x|), order=100, tolerance=1e-14 + # + # rho energy + # + 1.00000000e-06 7.93445832e-06 + 1.20226443e-06 9.54545091e-06 + 1.44543977e-06 1.14842358e-05 + 1.73780083e-06 1.38177301e-05 + 2.08929613e-06 1.66265809e-05 + 2.51188643e-06 2.00080034e-05 + 3.01995172e-06 2.40792133e-05 + 3.63078055e-06 2.89815779e-05 + 4.36515832e-06 3.48856405e-05 + 5.24807460e-06 4.19972045e-05 + 6.30957344e-06 5.05647046e-05 + 7.58577575e-06 6.08881446e-05 + 9.12010839e-06 7.33299394e-05 + 1.09647820e-05 8.83280780e-05 + 1.31825674e-05 1.06412115e-04 + 1.58489319e-05 1.28222614e-04 + 1.90546072e-05 1.54534805e-04 + 2.29086765e-05 1.86287394e-04 + 2.75422870e-05 2.24617677e-04 + 3.31131121e-05 2.70904370e-04 + 3.98107171e-05 3.26819905e-04 + 4.78630092e-05 3.94394317e-04 + 5.75439937e-05 4.76093386e-04 + 6.91830971e-05 5.74914264e-04 + 8.31763771e-05 6.94502595e-04 + 1.00000000e-04 8.39296065e-04 + 1.20226443e-04 1.01470042e-03 + 1.44543977e-04 1.22730542e-03 + 1.73780083e-04 1.48514988e-03 + 2.08929613e-04 1.79804690e-03 + 2.51188643e-04 2.17798310e-03 + 3.01995172e-04 2.63960836e-03 + 3.63078055e-04 3.20083623e-03 + 4.36515832e-04 3.88357954e-03 + 5.24807460e-04 4.71465030e-03 + 6.30957344e-04 5.72685888e-03 + 7.58577575e-04 6.96035420e-03 + 9.12010839e-04 8.46425370e-03 + 1.09647820e-03 1.02986208e-02 + 1.31825674e-03 1.25368572e-02 + 1.58489319e-03 1.52685874e-02 + 1.90546072e-03 1.86031268e-02 + 2.29086765e-03 2.26736380e-02 + 2.75422870e-03 2.76420977e-02 + 3.31131121e-03 3.37052167e-02 + 3.98107171e-03 4.11014850e-02 + 4.78630092e-03 5.01195435e-02 + 5.75439937e-03 6.11081308e-02 + 6.91830971e-03 7.44879092e-02 + 8.31763771e-03 9.07655413e-02 + 1.00000000e-02 1.10550483e-01 + 1.20226443e-02 1.34575061e-01 + 1.44543977e-02 1.63718539e-01 + 1.73780083e-02 1.99036030e-01 + 2.08929613e-02 2.41793284e-01 + 2.51188643e-02 2.93508614e-01 + 3.01995172e-02 3.56003446e-01 + 3.63078055e-02 4.31463277e-01 + 4.36515832e-02 5.22511186e-01 + 5.24807460e-02 6.32296416e-01 + 6.30957344e-02 7.64601077e-01 + 7.58577575e-02 9.23968602e-01 + 9.12010839e-02 1.11585830e+00 + 1.09647820e-01 1.34683126e+00 + 1.31825674e-01 1.62477387e+00 + 1.58489319e-01 1.95916654e+00 + 1.90546072e-01 2.36140673e+00 + 2.29086765e-01 2.84519724e+00 + 2.75422870e-01 3.42701297e+00 + 3.31131121e-01 4.12666196e+00 + 3.98107171e-01 4.96795983e+00 + 4.78630092e-01 5.97954056e+00 + 5.75439937e-01 7.19583118e+00 + 6.91830971e-01 8.65822353e+00 + 8.31763771e-01 1.04164830e+01 + 1.00000000e+00 1.25304420e+01 + 1.20226443e+00 1.50720365e+01 + 1.44543977e+00 1.81277534e+01 + 1.73780083e+00 2.18015742e+01 + 2.08929613e+00 2.62185132e+01 + 2.51188643e+00 3.15288712e+01 + 3.01995172e+00 3.79133506e+01 + 3.63078055e+00 4.55892039e+01 + 4.36515832e+00 5.48176270e+01 + 5.24807460e+00 6.59126465e+01 + 6.30957344e+00 7.92518063e+01 + 7.58577575e+00 9.52890139e+01 + 9.12010839e+00 1.14569987e+02 + 1.09647820e+01 1.37750822e+02 + 1.31825674e+01 1.65620322e+02 + 1.58489319e+01 1.99126836e+02 + 1.90546072e+01 2.39410530e+02 + 2.29086765e+01 2.87842186e+02 + 2.75422870e+01 3.46069846e+02 + 3.31131121e+01 4.16074894e+02 + 3.98107171e+01 5.00239474e+02 + 4.78630092e+01 6.01427558e+02 + 5.75439937e+01 7.23082394e+02 + 6.91830971e+01 8.69343678e+02 + 8.31763771e+01 1.04518842e+03 diff --git a/figs/energy.fig/erho_effective.gnuplot b/figs/energy.fig/erho_effective.gnuplot new file mode 100644 index 0000000..f26252e --- /dev/null +++ b/figs/energy.fig/erho_effective.gnuplot @@ -0,0 +1,38 @@ +set ylabel "$\\displaystyle\\frac{e}{\\rho}$" norotate offset -1,0 +set xlabel "$\\rho$" + +set xtics 1e-6, 100, 100 +set xtics add ("$10^{-6}$" 0.000001, "$10^{-4}$" 0.0001, "$10^{-2}$" 0.01, "$1$" 1.0, "$10^2$" 100) +unset mxtics + +set ytics 8,1 +set mytics 2 + +set xrange [0.000001:100] +set yrange [7.5:13.5] + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 8,6 standalone + +set key off + + +# 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 1 + +set logscale x + +a=1.25435641059 + +set label at 0.0001,2*pi*a*1.03 "LHY" textcolor "#DAA520" +set label at 0.1,4.1*pi "Hartree" textcolor "#32CD32" + +plot "erho.dat" using 1:($2/$1) with lines linestyle 1 ,\ + 2*pi*a*(1+128/15/sqrt(pi)*sqrt(x*a**3)) linestyle 5 dashtype "." ,\ + 4*pi linestyle 3 dashtype "." diff --git a/figs/energy.fig/erho_effective.pdf b/figs/energy.fig/erho_effective.pdf Binary files differnew file mode 100644 index 0000000..351ba36 --- /dev/null +++ b/figs/energy.fig/erho_effective.pdf diff --git a/figs/energy.fig/erho_fulleq.dat b/figs/energy.fig/erho_fulleq.dat new file mode 100644 index 0000000..351d1b9 --- /dev/null +++ b/figs/energy.fig/erho_fulleq.dat @@ -0,0 +1,100 @@ + 1.000000000000000e-06 7.943042518656766e-06 0 + 1.202264434617413e-06 9.550219866068997e-06 0 + 1.445439770745928e-06 1.148608224097378e-05 1 + 1.737800828749376e-06 1.381647407426905e-05 1 + 2.089296130854041e-06 1.662160583174429e-05 0 + 2.511886431509582e-06 2.000065135391551e-05 0 + 3.019951720402019e-06 2.406839054942614e-05 0 + 3.630780547701017e-06 2.896662133595565e-05 1 + 4.365158322401657e-06 3.486570260772683e-05 1 + 5.248074602497723e-06 4.197087478032896e-05 1 + 6.309573444801930e-06 5.052956242205629e-05 1 + 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7.113784322007290e+00 1 + 6.918309709189363e-01 8.570243441380599e+00 1 + 8.317637711026709e-01 1.032245608693097e+01 1 + 1.000000000000000e+00 1.243026753303222e+01 1 + 1.202264434617413e+00 1.496562561057760e+01 1 + 1.445439770745928e+00 1.801502869576436e+01 1 + 1.737800828749376e+00 2.168246883802093e+01 1 + 2.089296130854041e+00 2.609297014699965e+01 1 + 2.511886431509582e+00 3.139684282320142e+01 1 + 3.019951720402019e+00 3.777479758723231e+01 1 + 3.630780547701010e+00 4.544409456028400e+01 1 + 4.365158322401657e+00 5.466593586138625e+01 1 + 5.248074602497723e+00 6.575435350738108e+01 1 + 6.309573444801930e+00 7.908689506783082e+01 1 + 7.585775750291836e+00 9.511747067219883e+01 1 + 9.120108393559097e+00 1.143917984731058e+02 1 + 1.096478196143185e+01 1.375659740282897e+02 1 + 1.318256738556407e+01 1.654287952107530e+02 1 + 1.584893192461114e+01 1.989286012247062e+02 1 + 1.905460717963248e+01 2.392055363411829e+02 0 + 2.290867652767775e+01 2.876303621855438e+02 0 + 2.754228703338169e+01 3.458511552270688e+02 0 + 3.311311214825908e+01 4.158492765508882e+02 0 + 3.981071705534969e+01 5.000067330413117e+02 0 + 4.786300923226381e+01 6.011878314695363e+02 0 + 5.754399373371567e+01 7.228352310513908e+02 0 + 6.918309709189363e+01 8.690894472935229e+02 0 + 8.317637711026708e+01 1.044926046890143e+03 0 diff --git a/figs/energy.fig/erho_fulleq.gnuplot b/figs/energy.fig/erho_fulleq.gnuplot new file mode 100644 index 0000000..2927ead --- /dev/null +++ b/figs/energy.fig/erho_fulleq.gnuplot @@ -0,0 +1,37 @@ +set ylabel "$\\displaystyle\\frac{e}{\\rho}$" norotate offset -1,0 +set xlabel "$\\rho$" + +set xtics 1e-6, 100, 100 +set xtics add ("$10^{-6}$" 0.000001, "$10^{-4}$" 0.0001, "$10^{-2}$" 0.01, "$1$" 1.0, "$10^2$" 100) +unset mxtics + +set ytics 8,1 +set mytics 2 + +set xrange [0.000001:100] +set yrange [7.5:13.5] + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 8,6 standalone + +set key off + + +# 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 1 + +set logscale x + +a=1.25435641059 + +plot "erho.dat" using 1:($2/$1) with lines linestyle 1 ,\ + "erho_fulleq.dat" using 1:($2/$1) with lines linestyle 4 ,\ + 2*pi*a*(1+128/15/sqrt(pi)*sqrt(x*a**3)) linestyle 5 dashtype "." ,\ + 4*pi linestyle 3 dashtype "." ,\ + "holzmann_2019-12-25.dat" using 1:($2/$1) with points linestyle 2 diff --git a/figs/energy.fig/erho_fulleq.pdf b/figs/energy.fig/erho_fulleq.pdf Binary files differnew file mode 100644 index 0000000..3094403 --- /dev/null +++ b/figs/energy.fig/erho_fulleq.pdf diff --git a/figs/energy.fig/erho_lowhigh.gnuplot b/figs/energy.fig/erho_lowhigh.gnuplot new file mode 100644 index 0000000..9d2a590 --- /dev/null +++ b/figs/energy.fig/erho_lowhigh.gnuplot @@ -0,0 +1,37 @@ +set ylabel "$\\displaystyle\\frac{e}{\\rho}$" norotate offset -1,0 +set xlabel "$\\rho$" + +set xtics 1e-6, 100, 100 +set xtics add ("$10^{-6}$" 0.000001, "$10^{-4}$" 0.0001, "$10^{-2}$" 0.01, "$1$" 1.0, "$10^2$" 100) +unset mxtics + +set ytics 8,1 +set mytics 2 + +set xrange [0.000001:100] +set yrange [7.5:13.5] + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 8,6 standalone + +set key off + + +# 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 1 + +set logscale x + +a=1.25435641059 + +set label at 0.0001,2*pi*a*1.03 "LHY" textcolor "#DAA520" +set label at 0.1,4.1*pi "Hartree" textcolor "#32CD32" + +plot 2*pi*a*(1+128/15/sqrt(pi)*sqrt(x*a**3)) linestyle 5 dashtype "." ,\ + 4*pi linestyle 3 dashtype "." diff --git a/figs/energy.fig/erho_lowhigh.pdf b/figs/energy.fig/erho_lowhigh.pdf Binary files differnew file mode 100644 index 0000000..4872d49 --- /dev/null +++ b/figs/energy.fig/erho_lowhigh.pdf diff --git a/figs/energy.fig/holzmann_2019-12-25.dat b/figs/energy.fig/holzmann_2019-12-25.dat new file mode 100644 index 0000000..96689cb --- /dev/null +++ b/figs/energy.fig/holzmann_2019-12-25.dat @@ -0,0 +1,11 @@ +## data from M. Holzmann, 2019-09-22 +# rho E0 n0 +1e-6 7.902e-6 +1e-4 8.3441e-4 0.0171 +1e-3 9.13384e-3 0.0481 +1e-2 1.061073e-1 0.0871 +1e-1 1.19182e+0 0.0851 +1e-0 1.24302e+1 0.0587 +1e+1 1.25442e+2 0.0319 +5e+1 6.28032e+2 0.021 + diff --git a/figs/energy16.fig/2020-05-22+16.dat b/figs/energy16.fig/2020-05-22+16.dat new file mode 100644 index 0000000..c28285d --- /dev/null +++ b/figs/energy16.fig/2020-05-22+16.dat @@ -0,0 +1,7 @@ +# rho E0 n0 + 1e-3 0.05195 0.61 + 5e-3 0.449 0.40 + 1e-2 1.1335 0.34 + 2e-2 2.748 0.33 + 1e-1 17.797 0.43 + 1e+0 197.35 0.70 diff --git a/figs/energy16.fig/Makefile b/figs/energy16.fig/Makefile new file mode 100644 index 0000000..964a8c5 --- /dev/null +++ b/figs/energy16.fig/Makefile @@ -0,0 +1,35 @@ +PROJECTNAME=energy16 + +SIMPLEQ=~/Work/Research/2018+bose_gas/cmp/simpleq + +DATS=simpleq16.dat medeq16.dat +PDFS=$(addsuffix .pdf, $(PROJECTNAME)) +TEXS=$(addsuffix .tikz.tex, $(PROJECTNAME)) + +all: $(PDFS) + +$(PDFS): $(DATS) + gnuplot $(patsubst %.pdf, %.gnuplot, $@) > $(patsubst %.pdf, %.tikz.tex, $@) + pdflatex -jobname $(basename $@) -file-line-error $(patsubst %.pdf, %.tikz.tex, $@) + +simpleq16.dat: + julia $(SIMPLEQ)/main.jl -p "tolerance=1e-11;order=100;maxiter=100;v_a=16" -M simpleq energy_rho > $@ +medeq16.dat: + julia -p 8 $(SIMPLEQ)/main.jl -p "aK=1;aL1=1;aL2=1;aL3=0;bK=1;bL1=1;bL2=1;gK=1;gL2=1;gL3=0;N=12;P=8;v_a=16" -M medeq energy_rho > $@ + + +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 $(DATS) + +clean-tex: + rm -f $(PDFS) + +clean: clean-aux clean-tex diff --git a/figs/energy16.fig/energy16.gnuplot b/figs/energy16.fig/energy16.gnuplot new file mode 100644 index 0000000..dc996c5 --- /dev/null +++ b/figs/energy16.fig/energy16.gnuplot @@ -0,0 +1,34 @@ +set ylabel "$\\displaystyle\\frac{e}{\\rho}$" norotate offset -1,0 +set xlabel "$\\rho$" + +set xtics 1e-6, 100, 100 +set xtics add ("$10^{-6}$" 0.000001, "$10^{-4}$" 0.0001, "$10^{-2}$" 0.01, "$1$" 1.0, "$10^2$" 100) +unset mxtics + +#set ytics 0.6, 0.1 +set mytics 2 + +set xrange [0.000001:100] + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 8,6 standalone + +set key off + + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 2 +set style line 2 linetype rgbcolor "#DC143C" linewidth 2 +set style line 3 linetype rgbcolor "#32CD32" linewidth 2 +set style line 4 linetype rgbcolor "#4B0082" linewidth 2 +set style line 5 linetype rgbcolor "#DAA520" linewidth 2 + +set pointsize 1 + +set logscale x + +plot \ + "simpleq16.dat" using 1:($3<1e-5 ? ($2/$1) : 1/0) with lines ls 1 ,\ + "medeq16.dat" using 1:($3<1e-5 ? ($2/$1) : 1/0) with lines ls 4 ,\ + "2020-05-22+16.dat" using 1:($2/$1) with points ls 2 + diff --git a/figs/energy16.fig/energy16.pdf b/figs/energy16.fig/energy16.pdf Binary files differnew file mode 100644 index 0000000..0472d94 --- /dev/null +++ b/figs/energy16.fig/energy16.pdf diff --git a/figs/energy16.fig/medeq16.dat b/figs/energy16.fig/medeq16.dat new file mode 100644 index 0000000..b670ef5 --- /dev/null +++ b/figs/energy16.fig/medeq16.dat @@ -0,0 +1,100 @@ + 1.000000000000000e-06 2.554068644475559e-05 1.397500557749096e-14 + 1.202264434617413e-06 3.080347047701689e-05 1.638378932477403e-14 + 1.445439770745928e-06 3.716098929256974e-05 2.068669778175053e-14 + 1.737800828749376e-06 4.484410409494435e-05 9.413457244472722e-15 + 2.089296130854041e-06 5.413333030032436e-05 2.147730951610164e-14 + 2.511886431509582e-06 6.536981275090576e-05 5.079185685242370e-14 + 3.019951720402019e-06 7.896881202049198e-05 4.890613903920614e-14 + 3.630780547701017e-06 9.543630295201912e-05 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8.003831302911970e+03 8.573716686070972e-15 + 4.786300923226381e+01 9.622840695326604e+03 5.255692893479381e-14 + 5.754399373371567e+01 1.156931811166827e+04 5.412915990778012e-16 + 6.918309709189363e+01 1.390949868589013e+04 5.629397185139020e-14 + 8.317637711026708e+01 1.672301456399418e+04 8.852629630882290e-12 diff --git a/figs/energy_relative_error.fig/2020-10-15+energy.dat b/figs/energy_relative_error.fig/2020-10-15+energy.dat new file mode 100644 index 0000000..8a6566c --- /dev/null +++ b/figs/energy_relative_error.fig/2020-10-15+energy.dat @@ -0,0 +1,13 @@ +1e-6 7.90e-6 7.91e-6 +1e-4 8.344e-4 8.345e-4 0.017 0.018 8.355e-4 8.356e-4 0.015 0.016 +1e-3 9.1338e-3 9.1339e-3 0.048 0.049 9.142e-3 9.143e-3 0.045 0.046 +5e-3 5.0613e-2 5.0614e-2 0.080 0.081 5.0648e-2 5.0649e-2 0.070 0.071 +1e-2 1.06107e-1 1.06108e-1 0.087 0.088 1.0627e-1 1.0628e-1 0.073 0.074 +1.5e-2 1.6337e-1 1.6338e-1 0.090 0.091 1.6342e-1 1.6343e-1 0.088 0.089 +2e-2 2.2162e-1 2.2163e-1 0.093 0.094 2.2169e-1 2.2170e-1 0.090 0.091 +5e-2 5.8044e-1 5.8045e-1 0.091 0.092 5.8046e-1 5.8047e-1 0.091 0.092 +1e-1 1.1918e+0 1.1919e+0 0.088 0.089 1.1919e+0 1.1920e+0 0.085 0.086 +1e-0 1.2430e+1 1.2431e+1 0.058 0.059 1.245e+1 1.246e+1 0.05 0.06 +1e+1 1.2544e+2 1.2545e+2 0.031 0.032 +5e+1 6.2803e+2 6.2804e+2 0.02 0.03 + diff --git a/figs/energy_relative_error.fig/Makefile b/figs/energy_relative_error.fig/Makefile new file mode 100644 index 0000000..93e03f5 --- /dev/null +++ b/figs/energy_relative_error.fig/Makefile @@ -0,0 +1,51 @@ +PROJECTNAME=cmp_energy1 + +SIMPLEQ=~/Work/Research/2018+bose_gas/cmp/simpleq + +DATS= simpleq1.dat mueq1.dat bigeq1.dat +PDFS=$(addsuffix .pdf, $(PROJECTNAME)) +TEXS=$(addsuffix .tikz.tex, $(PROJECTNAME)) + +all: $(PDFS) + +$(PDFS): $(DATS) + gnuplot $(patsubst %.pdf, %.gnuplot, $@) > $(patsubst %.pdf, %.tikz.tex, $@) + pdflatex -jobname $(basename $@) -file-line-error $(patsubst %.pdf, %.tikz.tex, $@) + +bigeq1.dat: + for rho in 1e-6 1e-4 1e-3 5e-3 1e-2 1.5e-2 2e-2 5e-2 1e-1 1.0 1e1 5e1; do \ + echo -n $$rho " " >> $@-tmp ;\ + julia $(SIMPLEQ)/main.jl -p "N=12;P=8;J=10;maxiter=100;v_a=1;rho=$$rho;minlrho=-6;nlrho=50;eq=bigeq" -M medeq energy >> $@-tmp ;\ + done + paste $@-tmp 2020-10-15+energy.dat > $@ + rm $@-tmp +simpleq1.dat: + for lrho in -6 -4 -3 -2.3010299956639813 -2 -1.8239087409443189 -1.6989700043360187 -1.3010299956639813 -1 0 1 1.6989700043360187; do\ + julia $(SIMPLEQ)/main.jl -p "tolerance=1e-11;order=100;maxiter=100;v_a=1;minlrho=$$lrho;nlrho=1" -M simpleq energy_rho >> $@-tmp ;\ + done + paste $@-tmp 2020-10-15+energy.dat > $@ + rm $@-tmp +mueq1.dat: + for lrho in -6 -4 -3 -2.3010299956639813 -2 -1.8239087409443189 -1.6989700043360187 -1.3010299956639813 -1 0 1 1.6989700043360187; do\ + julia $(SIMPLEQ)/main.jl -p "tolerance=1e-11;order=100;maxiter=100;v_a=1;minlrho=$$lrho;nlrho=1" -M mueq energy_rho >> $@-tmp ;\ + done + paste $@-tmp 2020-10-15+energy.dat > $@ + rm $@-tmp + + +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 $(DATS) + rm -f Abar.dat + +clean-tex: + rm -f $(PDFS) + +clean: clean-aux clean-tex diff --git a/figs/energy_relative_error.fig/bigeq1.dat b/figs/energy_relative_error.fig/bigeq1.dat new file mode 100644 index 0000000..ccab7cc --- /dev/null +++ b/figs/energy_relative_error.fig/bigeq1.dat @@ -0,0 +1,13 @@ +1e-6 7.933345669932108e-06 1.702110068633820e-12 1e-6 7.90e-6 7.91e-6 +1e-4 8.349333596092273e-04 1.112527655484278e-13 1e-4 8.344e-4 8.345e-4 0.017 0.018 8.355e-4 8.356e-4 0.015 0.016 +1e-3 9.146316224214820e-03 2.077370190827862e-12 1e-3 9.1338e-3 9.1339e-3 0.048 0.049 9.142e-3 9.143e-3 0.045 0.046 +5e-3 5.063551121414726e-02 8.398015568932763e-12 5e-3 5.0613e-2 5.0614e-2 0.080 0.081 5.0648e-2 5.0649e-2 0.070 0.071 +1e-2 1.061166635113156e-01 5.017547334745932e-15 1e-2 1.06107e-1 1.06108e-1 0.087 0.088 1.0627e-1 1.0628e-1 0.073 0.074 +1.5e-2 1.633545333357252e-01 2.212732350724188e-15 1.5e-2 1.6337e-1 1.6338e-1 0.090 0.091 1.6342e-1 1.6343e-1 0.088 0.089 +2e-2 2.216006926766234e-01 4.554921896809050e-15 2e-2 2.2162e-1 2.2163e-1 0.093 0.094 2.2169e-1 2.2170e-1 0.090 0.091 +5e-2 5.805467427278628e-01 3.333614946727334e-15 5e-2 5.8044e-1 5.8045e-1 0.091 0.092 5.8046e-1 5.8047e-1 0.091 0.092 +1e-1 1.191928562890024e+00 2.450444415773880e-15 1e-1 1.1918e+0 1.1919e+0 0.088 0.089 1.1919e+0 1.1920e+0 0.085 0.086 +1.0 1.243051761633436e+01 3.791416729017179e-12 1e-0 1.2430e+1 1.2431e+1 0.058 0.059 1.245e+1 1.246e+1 0.05 0.06 +1e1 1.254476421597336e+02 2.677873467933947e-13 1e+1 1.2544e+2 1.2545e+2 0.031 0.032 +5e1 nan nan 5e+1 6.2803e+2 6.2804e+2 0.02 0.03 + diff --git a/figs/energy_relative_error.fig/cmp_energy1.gnuplot b/figs/energy_relative_error.fig/cmp_energy1.gnuplot new file mode 100644 index 0000000..c2b1afd --- /dev/null +++ b/figs/energy_relative_error.fig/cmp_energy1.gnuplot @@ -0,0 +1,37 @@ +set title "$v(\\mathbf x)=e^{-|\\mathbf x|}$" +set ylabel "energy relative error" offset +3 +set xlabel "$\\rho$" + +set xtics 1e-6, 100, 100 +set xtics add ("$10^{-6}$" 0.000001, "$10^{-4}$" 0.0001, "$10^{-2}$" 0.01, "$1$" 1.0, "$10^2$" 100) +unset mxtics +set xrange [1e-6:1e2] + +set ytics 1e-5, 10, 1e-1 +set ytics add ("$10^{-5}$" 1e-5, "$10^{-4}$" 1e-4, "$10^{-3}$" 1e-3, "$10^{-2}$" 1e-2, "$10^{-1}$" 1e-1) +set yrange [1e-5:1e-1] + +# default output canvas size: 12.5cm x 8.75cm +set term lua tikz size 8,6 standalone + +unset key + + +# set linestyle +set style line 1 linetype rgbcolor "#4169E1" linewidth 2 +set style line 2 linetype rgbcolor "#DC143C" linewidth 2 +set style line 3 linetype rgbcolor "#32CD32" linewidth 2 +set style line 4 linetype rgbcolor "#4B0082" linewidth 2 +set style line 5 linetype rgbcolor "#DAA520" linewidth 2 + +set pointsize 1 + +max(x,y)=(x>y ? x : y) + +set logscale xy + +plot \ + "simpleq1.dat" using 1:($3<1e-5 ? max(abs($2-$5)/$5,abs($2-$6)/$6) : 1/0) every ::1 with lp ls 1 ,\ + "bigeq1.dat" using 1:($3<1e-5 ? max(abs($2-$5)/$5,abs($2-$6)/$6) : 1/0) every ::1 with lp ls 4 ,\ + "2020-10-15+energy.dat" using 1:(max(max(abs($6-$2)/$2,abs($6-$3)/$3),max(abs($7-$2)/$2,abs($7-$3)/$3))) every ::1 with lp ls 2 + diff --git a/figs/energy_relative_error.fig/cmp_energy1.pdf b/figs/energy_relative_error.fig/cmp_energy1.pdf Binary files differnew file mode 100644 index 0000000..601b146 --- /dev/null +++ b/figs/energy_relative_error.fig/cmp_energy1.pdf diff --git a/figs/energy_relative_error.fig/mueq1.dat b/figs/energy_relative_error.fig/mueq1.dat new file mode 100644 index 0000000..6680ed3 --- /dev/null +++ b/figs/energy_relative_error.fig/mueq1.dat @@ -0,0 +1,13 @@ + 1.000000000000000e-06 7.934286257047026e-06 3.235575358862730e-14 1e-6 7.90e-6 7.91e-6 + 1.000000000000000e-04 8.377752370367244e-04 3.201262322514326e-14 1e-4 8.344e-4 8.345e-4 0.017 0.018 8.355e-4 8.356e-4 0.015 0.016 + 1.000000000000000e-03 9.227516472314044e-03 5.926882960328585e-12 1e-3 9.1338e-3 9.1339e-3 0.048 0.049 9.142e-3 9.143e-3 0.045 0.046 + 4.999999999999999e-03 5.110614907540598e-02 1.069784208067329e-14 5e-3 5.0613e-2 5.0614e-2 0.080 0.081 5.0648e-2 5.0649e-2 0.070 0.071 + 1.000000000000000e-02 1.069255387977072e-01 1.572627931557844e-14 1e-2 1.06107e-1 1.06108e-1 0.087 0.088 1.0627e-1 1.0628e-1 0.073 0.074 + 1.500000000000000e-02 1.643925118385577e-01 2.494863657028789e-14 1.5e-2 1.6337e-1 1.6338e-1 0.090 0.091 1.6342e-1 1.6343e-1 0.088 0.089 + 2.000000000000000e-02 2.228019992986293e-01 1.448625206361080e-14 2e-2 2.2162e-1 2.2163e-1 0.093 0.094 2.2169e-1 2.2170e-1 0.090 0.091 + 5.000000000000000e-02 5.821600306289594e-01 2.429130993459621e-14 5e-2 5.8044e-1 5.8045e-1 0.091 0.092 5.8046e-1 5.8047e-1 0.091 0.092 + 1.000000000000000e-01 1.193625606724180e+00 9.289627651289616e-14 1e-1 1.1918e+0 1.1919e+0 0.088 0.089 1.1919e+0 1.1920e+0 0.085 0.086 + 1.000000000000000e+00 1.243092200540192e+01 3.956891809887943e-12 1e-0 1.2430e+1 1.2431e+1 0.058 0.059 1.245e+1 1.246e+1 0.05 0.06 + 1.000000000000000e+01 1.254464788052155e+02 1.136222076562384e-14 1e+1 1.2544e+2 1.2545e+2 0.031 0.032 + 4.999999999999999e+01 6.280479158155819e+02 4.085062088184932e-15 5e+1 6.2803e+2 6.2804e+2 0.02 0.03 + diff --git a/figs/energy_relative_error.fig/simpleq1.dat b/figs/energy_relative_error.fig/simpleq1.dat new file mode 100644 index 0000000..0a9946c --- /dev/null +++ b/figs/energy_relative_error.fig/simpleq1.dat @@ -0,0 +1,13 @@ + 1.000000000000000e-06 7.934458317554763e-06 1.386474846476237e-14 1e-6 7.90e-6 7.91e-6 + 1.000000000000000e-04 8.392960650211980e-04 4.992772141681879e-14 1e-4 8.344e-4 8.345e-4 0.017 0.018 8.355e-4 8.356e-4 0.015 0.016 + 1.000000000000000e-03 9.335885024335848e-03 9.476600935679491e-12 1e-3 9.1338e-3 9.1339e-3 0.048 0.049 9.142e-3 9.143e-3 0.045 0.046 + 4.999999999999999e-03 5.253256909806337e-02 2.904203225041083e-14 5e-3 5.0613e-2 5.0614e-2 0.080 0.081 5.0648e-2 5.0649e-2 0.070 0.071 + 1.000000000000000e-02 1.105504827786785e-01 3.695967730970493e-14 1e-2 1.06107e-1 1.06108e-1 0.087 0.088 1.0627e-1 1.0628e-1 0.073 0.074 + 1.500000000000000e-02 1.702888708763101e-01 2.044316796426063e-14 1.5e-2 1.6337e-1 1.6338e-1 0.090 0.091 1.6342e-1 1.6343e-1 0.088 0.089 + 2.000000000000000e-02 2.309054339970606e-01 1.984104771646051e-14 2e-2 2.2162e-1 2.2163e-1 0.093 0.094 2.2169e-1 2.2170e-1 0.090 0.091 + 5.000000000000000e-02 6.014214358150070e-01 1.045253287889987e-14 5e-2 5.8044e-1 5.8045e-1 0.091 0.092 5.8046e-1 5.8047e-1 0.091 0.092 + 1.000000000000000e-01 1.226000446492040e+00 3.630493925691041e-15 1e-1 1.1918e+0 1.1919e+0 0.088 0.089 1.1919e+0 1.1920e+0 0.085 0.086 + 1.000000000000000e+00 1.253044200066420e+01 1.230015282154983e-13 1e-0 1.2430e+1 1.2431e+1 0.058 0.059 1.245e+1 1.246e+1 0.05 0.06 + 1.000000000000000e+01 1.256270224354739e+02 6.086298884133178e-15 1e+1 1.2544e+2 1.2545e+2 0.031 0.032 + 4.999999999999999e+01 6.282817756461592e+02 1.506690451671515e-15 5e+1 6.2803e+2 6.2804e+2 0.02 0.03 + diff --git a/libs/ian-presentation.cls b/libs/ian-presentation.cls new file mode 100644 index 0000000..91bd487 --- /dev/null +++ b/libs/ian-presentation.cls @@ -0,0 +1,187 @@ +%% +%% Ian's presentation class +%% + +%% TeX format +\NeedsTeXFormat{LaTeX2e}[1995/12/01] + +%% class name +\ProvidesClass{ian-presentation}[2017/09/29] + +\def\ian@defaultoptions{ + \pagestyle{plain} + \RequirePackage{color} + \RequirePackage{amssymb} +} + +%% paper dimensions +\setlength\paperheight{240pt} +\setlength\paperwidth{427pt} + +%% fonts +\input{size11.clo} +\DeclareOldFontCommand{\rm}{\normalfont\rmfamily}{\mathrm} +\DeclareOldFontCommand{\sf}{\normalfont\sffamily}{\mathsf} +\DeclareOldFontCommand{\tt}{\normalfont\ttfamily}{\mathtt} +\DeclareOldFontCommand{\bf}{\normalfont\bfseries}{\mathbf} +\DeclareOldFontCommand{\it}{\normalfont\itshape}{\mathit} + +%% text dimensions +\textheight=208pt +\textwidth=370pt +\hoffset=-1in +\voffset=-1in +\oddsidemargin=24pt +\evensidemargin=24pt +\topmargin=8pt +\headheight=0pt +\headsep=0pt +\marginparsep=0pt +\marginparwidth=0pt +\footskip=16pt + + +%% remove default skips +\parindent=0pt +\parskip=0pt +\baselineskip=0pt + +%% something is wrong with \thepage, redefine it +\gdef\thepage{\the\c@page} + +%% correct vertical alignment at the end of a document +\AtEndDocument{ + % save total slide count + \immediate\write\@auxout{\noexpand\gdef\noexpand\slidecount{\thepage}} + \vfill + \eject +} + + +%% footer +\def\ps@plain{ + \def\@oddhead{} + \def\@evenhead{\@oddhead} + \def\@oddfoot{\tiny\hfill\thepage/\safe\slidecount\hfill} + \def\@evenfoot{\@oddfoot} +} +\def\ps@empty{ + \def\@oddhead{} + \def\@evenhead{\@oddhead} + \def\@oddfoot{} + \def\@evenfoot{\@oddfoot} +} + + +%% title of slide +\def\title#1{ + \hfil{\bf\large #1}\par + \hfil\vrule width0.75\textwidth height0.3pt\par + \vskip5pt +} + + +%% hyperlinks +% hyperlinkcounter +\newcounter{lncount} +% hyperref anchor +\def\hrefanchor{% +\stepcounter{lncount}% +\hypertarget{ln.\thelncount}{}% +} + +%% define a command and write it to aux file +\def\outdef#1#2{% + % define command% + \expandafter\xdef\csname #1\endcsname{#2}% + % hyperlink number% + \expandafter\xdef\csname #1@hl\endcsname{\thelncount}% + % write command to aux% + \immediate\write\@auxout{\noexpand\expandafter\noexpand\gdef\noexpand\csname #1\endcsname{\csname #1\endcsname}}% + \immediate\write\@auxout{\noexpand\expandafter\noexpand\gdef\noexpand\csname #1@hl\endcsname{\thelncount}}% +} + +%% can call commands even when they are not defined +\def\safe#1{% + \ifdefined#1% + #1% + \else% + {\color{red}\bf?}% + \fi% +} + + +%% itemize +\newlength\itemizeskip +% left margin for items +\setlength\itemizeskip{20pt} +\newlength\itemizeseparator +% space between the item symbol and the text +\setlength\itemizeseparator{5pt} +% penalty preceding an itemize +\def\itemizepenalty{0} +% counter counting the itemize level +\newcounter{itemizecount} + +% item symbol +\def\itemizept#1{ + \ifnum#1=1 + \textbullet + \else + $\scriptstyle\blacktriangleright$ + \fi +} + +\newlength\current@itemizeskip +\setlength\current@itemizeskip{0pt} +\def\itemize{ + \par\penalty\itemizepenalty\medskip\penalty\itemizepenalty + \addtocounter{itemizecount}{1} + \addtolength\current@itemizeskip{\itemizeskip} + \leftskip\current@itemizeskip +} +\def\enditemize{ + \addtocounter{itemizecount}{-1} + \addtolength\current@itemizeskip{-\itemizeskip} + \par\leftskip\current@itemizeskip + \medskip +} +\newlength\itempt@total +\def\item{ + \settowidth\itempt@total{\itemizept\theitemizecount} + \addtolength\itempt@total{\itemizeseparator} + \par + \medskip + \hskip-\itempt@total\itemizept\theitemizecount\hskip\itemizeseparator +} + +%% enumerate +\newcounter{enumerate@count} +\def\enumerate{ + \setcounter{enumerate@count}0 + \let\olditem\item + \let\olditemizept\itemizept + \def\item{ + % counter + \stepcounter{enumerate@count} + % set header + \def\itemizept{\theenumerate@count.} + % hyperref anchor + \hrefanchor + % define tag (for \label) + \xdef\tag{\theenumerate@count} + \olditem + } + \itemize +} +\def\endenumerate{ + \enditemize + \let\item\olditem + \let\itemizept\olditemizept +} + + +%% end +\ian@defaultoptions + +\endinput |