I'm tryng to write an entire chapter vertically aligned. I found the following solution:
\begingroup%
\makeatletter%
\let\clearpage\relax%
\vspace*{\fill}%
\vspace*{\dimexpr-50\p@-\baselineskip}
\chapter*{\centering\normalsize{Abstract}}
\noindent
\begin{quote}
text 1
\end{quote}
\vspace*{\fill}%
\endgroup
The solution worked fine for me until I start a \newpage
and try to write another vertically aligned chapter. In this case, the second chapter is not vertically aligned.
Could someone help me?
Here, the full code
\documentclass[a4paper,12pt,twoside,openright]{book}
\usepackage[utf8]{inputenc}
\usepackage[T1]{fontenc}
\usepackage[lighttt]{lmodern}
\usepackage[a4paper,top=2.50cm,bottom=2.50cm,left=2.50cm,right=2.50cm]{geometry}
\usepackage{textcomp}
\usepackage{setspace}
\onehalfspacing
\usepackage{fancyhdr}
\setlength{\headheight}{18pt}%
\fancypagestyle{main}{%
\renewcommand{\headrulewidth}{.4pt}% Header rule
\renewcommand{\footrulewidth}{0pt}% No Footer rule
\fancyhf{}% Clear header/footer
\fancyhead[LE]{\itshape\nouppercase\leftmark}
\fancyhead[RO]{\itshape\nouppercase\rightmark}
\fancyhead[RE,LO]{\thepage}%
}
\fancypagestyle{plain}{%
\fancyhf{} % clear all header and footer fields
\fancyfoot[R]{\thepage}
\fancyhead{}
\renewcommand{\headrulewidth}{0pt}
\renewcommand{\footrulewidth}{0pt}
}
\raggedbottom
\usepackage{titlesec}
\titleformat{name=\chapter}[display]
{\Large\ttfamily}
{{\chaptertitlename} \thechapter}
{2ex}
{\bfseries\filcenter\Huge
}
\titleformat{\section}[block]
{\ttfamily\bfseries\boldmath\Large}
{\thesection}{1em}{}
\titleformat{\subsection}[block]
{\ttfamily\bfseries\large}
{\thesubsection}{1em}{}
\titlespacing{\chapter}{0pt}{-10pt}{40pt}
\newenvironment{changemargin}[2]{%
\begin{list}{}{%
\setlength{\topsep}{0pt}%
\setlength{\leftmargin}{#1}%
\setlength{\rightmargin}{#2}%
\setlength{\listparindent}{\parindent}%
\setlength{\itemindent}{\parindent}%
\setlength{\parsep}{\parskip}%
}%
\item[]}{\end{list}}
\begin{document}
\begingroup%
\makeatletter%
\let\clearpage\relax%
\vspace*{\fill}%
\vspace*{\dimexpr-50\p@-\baselineskip}
\chapter*{\centering\normalsize{Abstract}}
\noindent
\begin{quote}
A problem of non-relativistic quantum mechanics treated using regularization and renormalization is presented. The main aim of this thesis is to study regularization and renormalization techniques in general and applying them first to a classical electromagnetism problem and then to compute the bound state energy of a single quantum particle subjected to a two-dimensional $\delta$-function potential, which results to be divergent if computed naively. The naive computation is performed both solving directly the Schr\"odinger equation and using the theory of propagators, that is briefly studied in the central part of the thesis. The regularization techniques used are the cutoff regularization and the dimensional one. An effective field theory approach, where the potential is regularized through the real space scheme, is also presented. After regularization has been performed, the potential is renormalized re-defining the coupling constant and the running of the renormalized coupling constant, i.e. the renormalization group equation, is found.
\end{quote}
\vspace*{\fill}%
\endgroup
\newpage
\begingroup%
\makeatletter%
\let\clearpage\relax%
\vspace*{\fill}%
\vspace*{\dimexpr-50\p@-\baselineskip}
\chapter*{\centering\normalsize{Sommario}}
\noindent
\begin{quote}
A problem of non-relativistic quantum mechanics treated using regularization and renormalization is presented. The main aim of this thesis is to study regularization and renormalization techniques in general and applying them first to a classical electromagnetism problem and then to compute the bound state energy of a single quantum particle subjected to a two-dimensional $\delta$-function potential, which results to be divergent if computed naively. The naive computation is performed both solving directly the Schr\"odinger equation and using the theory of propagators, that is briefly studied in the central part of the thesis. The regularization techniques used are the cutoff regularization and the dimensional one. An effective field theory approach, where the potential is regularized through the real space scheme, is also presented. After regularization has been performed, the potential is renormalized re-defining the coupling constant and the running of the renormalized coupling constant, i.e. the renormalization group equation, is found.
\end{quote}
\vspace*{\fill}%
\endgroup
\end{document}
Here a picture of the output wanted (only the first part works)
kantlipsum
package to better explain it