\relax \bibstyle{woc} \citation{BaBar,BaBarc} \citation{cmd2} \citation{cleo} \babel@aux{english}{} \@writefile{toc}{\contentsline {section}{\numberline {1}Introduction}{1}} \newlabel{Introd}{{1}{1}} \citation{cmd3} \citation{vepp2000000} \citation{csi} \citation{GEANT4} \citation{rmc} \citation{gener} \citation{compton,compton1} \@writefile{toc}{\contentsline {section}{\numberline {2}CMD-3 detector and data set}{2}} \newlabel{CMD3}{{2}{2}} \@writefile{toc}{\contentsline {section}{\numberline {3}Event Selection}{2}} \newlabel{evntselection}{{3}{2}} \citation{gener} \@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces (left) Ionization losses vs. momentum for positive tracks for data at $E_{c.m.} = 1.5$ GeV. The lines show the acceptance for signal pions. (right) The spectrum of $\chi ^2_{5C}$ for the \ensuremath {\rm e^+ e^- \to 2\pi ^0 \pi ^+\pi ^-}events. }}{3}} \newlabel{dedxp}{{1}{3}} \@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces (left) The $\gamma _3 \gamma _4$ mass spectrum for \ensuremath {\rm e^+ e^- \to 2\pi ^0 \pi ^+\pi ^-}~ events at $E_{c.m.} = 1.5$ GeV. (right) The difference of the total reconstructed energy of pions and $\sqrt {s} = E_{c.m.}$ for \ensuremath {\rm e^+ e^- \to 2\pi ^+ 2\pi ^-}~ events at $E_{c.m.} = 1.5$ GeV.}}{3}} \newlabel{lmgg_750_2011}{{2}{3}} \citation{cmd2} \citation{PDG} \@writefile{toc}{\contentsline {section}{\numberline {4}Amplitude analysis}{4}} \@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces Cross sections calculated for different components of the matrix element. The total cross section of the process \ensuremath {\rm e^+ e^- \to 2\pi ^0 \pi ^+\pi ^-}~, measured in this analysis (filled circles).}}{5}} \newlabel{cross_sections}{{3}{5}} \@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces The data-MC comparison of the $\pi ^+ \pi ^- \pi ^0$, $\pi ^+ \pi ^-$, $\pi ^0 \pi ^0$ and $\pi ^{\pm }\pi ^{0}$ mass spectra for the process \ensuremath {\rm e^+ e^- \to 2\pi ^0 \pi ^+\pi ^-}~ in the energy ranges $\sqrt {s} = 1.7 \div 1.8$ GeV (top) and $\sqrt {s} = 1.9 \div 2.01$ GeV (bottom).}}{5}} \newlabel{2pi2pi01819}{{4}{5}} \@writefile{toc}{\contentsline {section}{\numberline {5}Systematic and model uncertainty}{5}} \bibcite{BaBar}{{1}{}{{}}{{}}} \bibcite{BaBarc}{{2}{}{{}}{{}}} \bibcite{cmd2}{{3}{}{{}}{{}}} \bibcite{cleo}{{4}{}{{}}{{}}} \@writefile{lof}{\contentsline {figure}{\numberline {5}{\ignorespaces The data-MC comparison of the squared matrix element $|M|^2$ and $\pi ^+ \pi ^-$, $2\pi ^{\pm } \pi ^{\mp }$ and $\pi ^{\pm }\pi ^{\pm }$ mass spectra for the process \ensuremath {\rm e^+ e^- \to 2\pi ^+ 2\pi ^-}~ for the energy ranges $\sqrt {s} = 1.9 \div 2.01$ GeV.}}{6}} \newlabel{4pic192}{{5}{6}} \@writefile{toc}{\contentsline {section}{\numberline {6}Summary}{6}} \bibcite{cmd3}{{5}{}{{}}{{}}} \bibcite{vepp2000000}{{6}{}{{}}{{}}} \bibcite{csi}{{7}{}{{}}{{}}} \bibcite{GEANT4}{{8}{}{{}}{{}}} \bibcite{rmc}{{9}{}{{}}{{}}} \bibcite{gener}{{10}{}{{}}{{}}} \bibcite{compton}{{11}{}{{}}{{}}} \bibcite{compton1}{{12}{}{{}}{{}}} \bibcite{PDG}{{13}{}{{}}{{}}} \providecommand\NAT@force@numbers{}\NAT@force@numbers