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authorNorbert Preining <norbert@preining.info>2019-09-02 13:46:59 +0900
committerNorbert Preining <norbert@preining.info>2019-09-02 13:46:59 +0900
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tree60335e10d2f4354b0674ec22d7b53f0f8abee672 /support/biblio/EXAMPLES
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-rw-r--r--support/biblio/EXAMPLES/2sorts/2sorts.tex169
-rw-r--r--support/biblio/EXAMPLES/2sorts/2sorts_formats.tex217
-rwxr-xr-xsupport/biblio/EXAMPLES/2sorts/libtex32
-rw-r--r--support/biblio/EXAMPLES/2sorts/refers.db1186
-rw-r--r--support/biblio/EXAMPLES/hairy/hairy.tex895
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diff --git a/support/biblio/EXAMPLES/2sorts/2sorts.tex b/support/biblio/EXAMPLES/2sorts/2sorts.tex
new file mode 100644
index 0000000000..c53a0a2b64
--- /dev/null
+++ b/support/biblio/EXAMPLES/2sorts/2sorts.tex
@@ -0,0 +1,169 @@
+\documentstyle[aps,manuscript]{revtex}
+
+\title{Comb copolymer brush with chemically different side chains}
+\date{\today}
+%-----------------------------------------------
+
+\newcommand{\vA}{v_{AA}}
+\newcommand{\vB}{v_{BB}}
+\newcommand{\vAB}{v_{AB}}
+\newcommand{\vx}{v}
+\newcommand{\mnu}{\nu}
+\newcommand{\khi}{\chi}
+\newcommand{\dd}{\partial}
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+
+\begin{document}
+
+\maketitle
+%--------------------------------------------------
+
+\begin{abstract}
+An investigation of side chain microphase separation
+within a single comb copolymer molecule containing chemically different
+$A$ and $B$ side chains has been carried out. Expressions for the
+transition point $\chi_{AB}^*$ in a
+good ($\chi_{AB}^* \sim N^{-3/8}$),
+marginal ($\chi_{AB}^* \sim N^{-1/2}$),
+$\theta$ ($\chi_{AB}^* \sim N^{-2/3}$),
+and poor ($\chi_{AB}^* \sim N^{-1}$)
+solvent are derived
+both by a mean field calculation and by scaling arguments.
+Properties of the system below and above the transition point are
+described.
+Some unusual ``bow-like'' conformations are predicted for a single
+molecule in the microphase separated state in a good solvent.
+\end{abstract}
+%--------------------------------------------------
+\section{Introduction}
+
+The conformational characteristics of individual comb copolymers with a
+high grafting density of side chains in solution has been addressed in a
+series of theoretical papers
+\cite{Birshtein,WangSafran,Fredrickson,Rouault1,3dFlex,3dRigid,Potemkin,2dComb}
+to begin with the original work of
+Birshtein et al \cite{Birshtein}.
+Irrespective of the solvent quality, be it a good
+solvent or a $\theta$-solvent, all theories predict a cylindrical
+brush-like structure for sufficiently long side chains. The pertinent
+parameters are the side chain grafting density, the side chain length,
+the intrinsic stiffness of the backbone and the side chains (the
+respective Kuhn segments) and the solvent quality with respect to the
+side chains and the backbone. The conformation is characterized by a
+number of quantities, the persistence length of the comb copolymer brush
+being most important. For sufficiently long side chains the persistence
+length is predicted to exceed the backbone length, thus resulting in a
+characteristic cylindrical "bottle-brush" structure. Subsequent computer
+simulations using a freely jointed hard sphere model essentially
+confirmed this picture
+\cite{Mika4,BrinkeIkkala,Rouault2,Mika1,Mika3,Mika2}.
+
+The experimental investigation of comb copolymers with a high grafting
+density has assumed large proportions after the successful
+polymerization of macromonomers, yielding degrees of polymerization
+significantly exceeding the length of the macromonomer itself, by
+Tsukahara and coworkers
+\cite{Tsukahara2,Tsukahara3,Schmidt,Tsukahara0}.
+Besides polymerization of macromonomers
+alternative routes have been developed recently using grafting from a
+macroinitiator prepared by either atom-transfer radical polymerization
+\cite{Beers1}
+or by living cationic polymerization
+\cite{Schappacher}.
+Using atom transfer
+radical polymerization molecular brushes with block copolymer side
+chains have been prepared as well.
+
+The experimental characterization of the comb copolymer brush
+conformation in dilute solution is a highly nontrivial issue. It was
+achieved recently by Schmidt and co-workers
+\cite{Borner1,Wintermantel1,Wintermantel2,Wintermantel3,DziezokSheiko,Sheiko,GerleRoos,FischerGerleSchmidt}
+using a combination
+of light scattering experiments and theoretical modeling. Since the high
+grafting density is supposed to lead to a stiff molecular structure, the
+modeling has been based on the Kratky-Porod worm-like chain model.
+For high molar mass polymacromonomers based on methacryloyl
+end-functionalized oligo methacrylates ($M_n = 2410~g/mole$) in the good
+solvent THF, the Kuhn statistical segment length, which is twice the
+persistence length, turned out to be $120~nm$. For polymacromonomers
+($M_n = 3624~g/mole$) consisting of polystyrene main and side chains this
+value was $190~nm$ in the good solvent toluene and $120~nm$ in the
+"$\theta$-solvent" cyclohexane.
+
+At the same time one of the most challenging problems in
+the polymer physics is a description of a microphase
+formation in copolymer systems.
+Theoretically, self-organization in block copolymer systems has
+attracted
+a lot of attention during the last decades and a fairly complete picture
+has emerged for the
+relatively simple diblock copolymers.
+\cite{Helfand1,Semenov,Leibler,FredricksonHelfand}
+As a consequence, the interest gradually shifts towards more
+complicated architectures such as comb or graft copolymers
+\cite{Dobrynin1,Cruz1,Foster1,WernerFredrickson,Nap1}.
+The discussion of structure formation in comb copolymers using the weak
+segregation limit has been presented in some detail. Compared to diblock
+copolymers the description is only slightly complicated by the fact that
+the single chain correlation functions are more involved. Phase diagrams
+of various comb copolymer systems have been published. Although
+different in details, the general trends are the same as for diblock
+copolymers. Of course, rather than the overall chain length, it is the
+length of the "repeat unit" that determines the order-disorder
+transition temperature as well as the characteristic length scale of the
+ordered structures.
+
+The application of the weak segregation approach, however, requires a
+relatively low
+grafting density such that the distance between two
+consecutive grafting points along the backbone is at least of the order
+of the Flory radius of the side chains. If the grafting density of comb
+copolymers is very high, the structure in the melt will usually involve
+segregation between individual molecules. Even if the incompatibility
+between backbone and side chains is high, the high grafting density may
+well prevent segregation of several backbones. Furthermore, a high
+grafting density combined with long side chains implies the volume
+fraction of the backbone to be of the order of 0.1 or lower, not
+necessarily the most interesting part of the melt phase diagram.
+
+Still, microphase separation may occur provided chemically different
+side chains are used. In this case unfavorable interaction between the
+side chains may lead to a micro domain
+structure within a single molecule. The present paper is devoted to this
+subject.
+The main objective is to identify conditions for "microphase separation"
+of side chains of two
+different types within a single comb copolymer molecule under different
+solvent conditions.
+
+The paper is organized as follows. The next section describes the
+self-consistent field approach to a molecule with a straight
+backbone and chemically different side chains. We show the possibility
+of side chain separation
+within the molecule and discuss the limits of the theory's
+applicability.
+The subsequent section is devoted to possible unusual behavior
+of comb copolymer molecules with a flexible backbone and
+microphase separated side chains. Then all results are summarized and
+discussed in the last section.
+
+%-------------------------------------------
+\section{Useful literature (not from the article)}
+Very interesting and useful books on this subject (polymers) are
+\cite{bookdeGennesScalingConcepts,GrosKhokh,bookCloizeaux} or more specific
+books devoted to peculiarities if comb copolymers behavior
+\cite{bookPlate,bookMcArdle}.
+Still unpublished works, like \cite{FischerSchmidt}, can be very helpful too.
+
+Thesis \cite{thesisHyvarinen} is a good reading too!
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{references}
+
+
+\end{references}
+
+
+
+
+
+\end{document} \ No newline at end of file
diff --git a/support/biblio/EXAMPLES/2sorts/2sorts_formats.tex b/support/biblio/EXAMPLES/2sorts/2sorts_formats.tex
new file mode 100644
index 0000000000..d95505135d
--- /dev/null
+++ b/support/biblio/EXAMPLES/2sorts/2sorts_formats.tex
@@ -0,0 +1,217 @@
+%% This is an example of a TeX file with formats
+%% included into the header of the document.
+%% To run it you have to do something like:
+%% biblio.pl -o 2sorts_formats.1.tex -d refers.db 2sorts_formats.tex
+%% or
+%% biblio.pl -o 2sorts_formats.1.tex -d refers.db --nobibitem --uselist 2sorts_formats.tex
+%% if you want a really well formatted citation list
+%% and then
+%% latex 2sorts_formats.1.tex
+%% to get 2sorts_formats.1.dvi
+
+%%------------------------------------------------------
+
+%% this is copyed from the template for Macromolecules
+%% no ordering of the references is needed. Otherwise add line
+%% '%ordering= AUTHORL'
+
+%begin{biblio}
+
+%cite_format={(%s)}
+%ref_format=${^{%s}}$
+
+%% normal article:
+% ARTICLE [$AUTHOR0P~L,~F~M; $ {\it $JOURNAL$} {\bf $YEAR$}, {\it $VOL$}, $PAGE$.]
+
+%% article which is submitted or accepted
+% ARTICLE0[$AUTHOR0P~L,~F~M; $ {\it $JOURNAL$} $STATE$.]
+
+%% normal book
+% BOOK [$AUTHOR0P~L,~F~M; $ {\it $TITLE$}; $PUBL$: $PLACE$, $YEAR$.]
+
+%% article in a book AUTHORE, AUTHORG and AUTHORH - last, first
+%% and middle names of the editor
+% EDBOOK [$AUTHOR0P~L,~F~M; $ in {\it $BOOKTITLE$}, edited by $AUTHOR0I~E,~G~H;$; $PUBL$: $PLACE$, $YEAR$.]
+
+%% article in a book without editor
+% INBOOK [$AUTHOR0P~L,~F~M; $ in {\it $BOOKTITLE$}, p.$PAGE$ $PUBL$: $PLACE$, $YEAR$.]
+
+% EPRINT [$AUTHOR0P~L,~F~M; $ in {\it $BOOKTITLE$} $INFO$, $YEAR$.]
+
+%% Thesis
+% THESIS [$AUTHOR0P~L,~F~M; $ {\it $SORT$}; $UNIV$: $PLACE$, $YEAR$.]
+
+%end{biblio}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%REAL DOCUMENT STARTS HERE!!!!
+
+\documentstyle[aps,manuscript]{revtex}
+
+\title{Comb copolymer brush with chemically different side chains}
+\date{\today}
+%-----------------------------------------------
+
+\newcommand{\vA}{v_{AA}}
+\newcommand{\vB}{v_{BB}}
+\newcommand{\vAB}{v_{AB}}
+\newcommand{\vx}{v}
+\newcommand{\mnu}{\nu}
+\newcommand{\khi}{\chi}
+\newcommand{\dd}{\partial}
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+
+\begin{document}
+
+\maketitle
+%--------------------------------------------------
+
+\begin{abstract}
+An investigation of side chain microphase separation
+within a single comb copolymer molecule containing chemically different
+$A$ and $B$ side chains has been carried out. Expressions for the
+transition point $\chi_{AB}^*$ in a
+good ($\chi_{AB}^* \sim N^{-3/8}$),
+marginal ($\chi_{AB}^* \sim N^{-1/2}$),
+$\theta$ ($\chi_{AB}^* \sim N^{-2/3}$),
+and poor ($\chi_{AB}^* \sim N^{-1}$)
+solvent are derived
+both by a mean field calculation and by scaling arguments.
+Properties of the system below and above the transition point are
+described.
+Some unusual ``bow-like'' conformations are predicted for a single
+molecule in the microphase separated state in a good solvent.
+\end{abstract}
+%--------------------------------------------------
+\section{Introduction}
+
+The conformational characteristics of individual comb copolymers with a
+high grafting density of side chains in solution has been addressed in a
+series of theoretical papers
+\cite{Birshtein,WangSafran,Fredrickson,Rouault1,3dFlex,3dRigid,Potemkin,2dComb}
+to begin with the original work of
+Birshtein et al \cite{Birshtein}.
+Irrespective of the solvent quality, be it a good
+solvent or a $\theta$-solvent, all theories predict a cylindrical
+brush-like structure for sufficiently long side chains. The pertinent
+parameters are the side chain grafting density, the side chain length,
+the intrinsic stiffness of the backbone and the side chains (the
+respective Kuhn segments) and the solvent quality with respect to the
+side chains and the backbone. The conformation is characterized by a
+number of quantities, the persistence length of the comb copolymer brush
+being most important. For sufficiently long side chains the persistence
+length is predicted to exceed the backbone length, thus resulting in a
+characteristic cylindrical "bottle-brush" structure. Subsequent computer
+simulations using a freely jointed hard sphere model essentially
+confirmed this picture
+\cite{Mika4,BrinkeIkkala,Rouault2,Mika1,Mika3,Mika2}.
+
+The experimental investigation of comb copolymers with a high grafting
+density has assumed large proportions after the successful
+polymerization of macromonomers, yielding degrees of polymerization
+significantly exceeding the length of the macromonomer itself, by
+Tsukahara and coworkers
+\cite{Tsukahara2,Tsukahara3,Schmidt,Tsukahara0}.
+Besides polymerization of macromonomers
+alternative routes have been developed recently using grafting from a
+macroinitiator prepared by either atom-transfer radical polymerization
+\cite{Beers1}
+or by living cationic polymerization
+\cite{Schappacher}.
+Using atom transfer
+radical polymerization molecular brushes with block copolymer side
+chains have been prepared as well.
+
+The experimental characterization of the comb copolymer brush
+conformation in dilute solution is a highly nontrivial issue. It was
+achieved recently by Schmidt and co-workers
+\cite{Borner1,Wintermantel1,Wintermantel2,Wintermantel3,DziezokSheiko,Sheiko,GerleRoos,FischerGerleSchmidt}
+using a combination
+of light scattering experiments and theoretical modeling. Since the high
+grafting density is supposed to lead to a stiff molecular structure, the
+modeling has been based on the Kratky-Porod worm-like chain model.
+For high molar mass polymacromonomers based on methacryloyl
+end-functionalized oligo methacrylates ($M_n = 2410~g/mole$) in the good
+solvent THF, the Kuhn statistical segment length, which is twice the
+persistence length, turned out to be $120~nm$. For polymacromonomers
+($M_n = 3624~g/mole$) consisting of polystyrene main and side chains this
+value was $190~nm$ in the good solvent toluene and $120~nm$ in the
+"$\theta$-solvent" cyclohexane.
+
+At the same time one of the most challenging problems in
+the polymer physics is a description of a microphase
+formation in copolymer systems.
+Theoretically, self-organization in block copolymer systems has
+attracted
+a lot of attention during the last decades and a fairly complete picture
+has emerged for the
+relatively simple diblock copolymers.
+\cite{Helfand1,Semenov,Leibler,FredricksonHelfand}
+As a consequence, the interest gradually shifts towards more
+complicated architectures such as comb or graft copolymers
+\cite{Dobrynin1,Cruz1,Foster1,WernerFredrickson,Nap1}.
+The discussion of structure formation in comb copolymers using the weak
+segregation limit has been presented in some detail. Compared to diblock
+copolymers the description is only slightly complicated by the fact that
+the single chain correlation functions are more involved. Phase diagrams
+of various comb copolymer systems have been published. Although
+different in details, the general trends are the same as for diblock
+copolymers. Of course, rather than the overall chain length, it is the
+length of the "repeat unit" that determines the order-disorder
+transition temperature as well as the characteristic length scale of the
+ordered structures.
+
+The application of the weak segregation approach, however, requires a
+relatively low
+grafting density such that the distance between two
+consecutive grafting points along the backbone is at least of the order
+of the Flory radius of the side chains. If the grafting density of comb
+copolymers is very high, the structure in the melt will usually involve
+segregation between individual molecules. Even if the incompatibility
+between backbone and side chains is high, the high grafting density may
+well prevent segregation of several backbones. Furthermore, a high
+grafting density combined with long side chains implies the volume
+fraction of the backbone to be of the order of 0.1 or lower, not
+necessarily the most interesting part of the melt phase diagram.
+
+Still, microphase separation may occur provided chemically different
+side chains are used. In this case unfavorable interaction between the
+side chains may lead to a micro domain
+structure within a single molecule. The present paper is devoted to this
+subject.
+The main objective is to identify conditions for "microphase separation"
+of side chains of two
+different types within a single comb copolymer molecule under different
+solvent conditions.
+
+The paper is organized as follows. The next section describes the
+self-consistent field approach to a molecule with a straight
+backbone and chemically different side chains. We show the possibility
+of side chain separation
+within the molecule and discuss the limits of the theory's
+applicability.
+The subsequent section is devoted to possible unusual behavior
+of comb copolymer molecules with a flexible backbone and
+microphase separated side chains. Then all results are summarized and
+discussed in the last section.
+
+%-------------------------------------------
+\section{Useful literature (not from the article)}
+Very interesting and useful books on this subject (polymers) are
+\cite{bookdeGennesScalingConcepts,GrosKhokh,bookCloizeaux} or more specific
+books devoted to peculiarities if comb copolymers behavior
+\cite{bookPlate,bookMcArdle}.
+Still unpublished works, like \cite{FischerSchmidt}, can be very helpful too.
+
+Thesis \cite{thesisHyvarinen} is a good reading too!
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{references}
+
+
+\end{references}
+
+
+
+
+
+\end{document} \ No newline at end of file
diff --git a/support/biblio/EXAMPLES/2sorts/libtex b/support/biblio/EXAMPLES/2sorts/libtex
new file mode 100755
index 0000000000..c33c392115
--- /dev/null
+++ b/support/biblio/EXAMPLES/2sorts/libtex
@@ -0,0 +1,32 @@
+JOURNAL="physreve"
+PREFIX="../../"
+
+VLEVEL="1" #verbosity level
+PROJECT="2sorts"
+REFS="refers.db"
+FORMATS=$PREFIX"formats/"$JOURNAL
+
+
+
+SUFFIX=".1"
+
+OUTTEX="$PROJECT$SUFFIX.tex"
+OUTDVI="$PROJECT$SUFFIX.dvi"
+TEXFILE="$PROJECT.tex"
+DVIFILE="$PROJECT.dvi"
+
+
+echo $OUTTEX
+
+if [ $JOURNAL = "physreve" ]
+then
+ "$PREFIX"biblio.pl -v $VLEVEL -o $OUTTEX -d $REFS -f $FORMATS $TEXFILE
+else
+ "$PREFIX"biblio.pl -v $VLEVEL -o $OUTTEX -d $REFS -f $FORMATS --nobibitem --uselist $TEXFILE
+fi
+
+
+latex $OUTTEX
+latex $OUTTEX
+mv $OUTDVI $DVIFILE
+#rm *.aux *.log *~ \ No newline at end of file
diff --git a/support/biblio/EXAMPLES/2sorts/refers.db b/support/biblio/EXAMPLES/2sorts/refers.db
new file mode 100644
index 0000000000..fb2654ac9e
--- /dev/null
+++ b/support/biblio/EXAMPLES/2sorts/refers.db
@@ -0,0 +1,1186 @@
+LABEL = thesisHyvarinen
+TYPE = thesis
+AUTHORL = Hyv\"arinen
+AUTHORF = S.
+SORT = Licentiate Thesis
+UNIV = University of Helsinki
+PLACE = Helsinki
+YEAR = 1997
+TITLE =
+URL =
+----------
+LABEL = Brinke4
+TYPE = edbook
+AUTHORP = |ten
+AUTHORL = Ikkala|Brinke
+AUTHORF = O.|G.
+BOOKTITLE= Handbook of Advanced Electronic and Photonic Materials and Devices, Part 8 Conducting Polymers
+AUTHORI =
+AUTHORE = Nalwa
+AUTHORG = Hari
+AUTHORH = Singh
+PAGE = 185
+PUBL = Academic Press
+PLACE =
+YEAR = 2000
+----------
+LABEL = bookMcArdle
+TYPE = edbook
+AUTHORL = Warner
+AUTHORF = M.
+AUTHORM =
+TITLE = The physical principles of side chain polymer liquid crystals
+BOOKTITLE= Side Chain Liquid Crystal Polymers
+AUTHORI =
+AUTHORE = McArdle
+AUTHORG = C.
+AUTHORH = B.
+PUBL = Blackie
+PLACE = Glasgow and London
+YEAR = 1989
+PAGE = 7
+EPAGE = 29
+----------
+LABEL = bookdeGennesLiqCryst
+TYPE = book
+AUTHORP = de
+AUTHORL = Gennes
+AUTHORF = P.-G.
+AUTHORM =
+TITLE = The Physics of Liquid Crystals
+PUBL = Clarendon Press
+PLACE = Oxford
+YEAR = 1974
+----------
+LABEL = bookdeGennesScalingConcepts
+TYPE = book
+AUTHORP = de
+AUTHORL = Gennes
+AUTHORF = P.-G.
+AUTHORM =
+TITLE = Scaling Concepts in Polymer Physics
+PUBL = Cornell University Press
+PLACE = Ithaca
+YEAR = 1985
+PAGES = 325
+----------
+LABEL = bookPlate
+TYPE = book
+AUTHORL = Plate|Shibaev
+AUTHORF = N. |V.
+AUTHORM = A. |P.
+TITLE = Comb-Shaped Polymers and Liquid Crystals
+PUBL = Plenum Press
+PLACE = New York and London
+YEAR = 1987
+PAGES = 415
+----------
+LABEL = GrosKhokh
+TYPE = book
+AUTHORL = Grosberg|Khokhlov
+AUTHORF = A. |A.
+AUTHORM = Yu. |R.
+TITLE = Statistical Physics of Macromolecules
+PUBL = American Institute of Physics
+PLACE = New York
+YEAR = 1994
+----------
+LABEL = Landau
+TYPE = book
+AUTHORL = Landau|Lifshits
+AUTHORF = L |E.
+AUTHORM = D. |M.
+TITLE = Statistical Physics
+PUBL = Pergamon
+PLACE = Oxford
+YEAR = 1980
+----------
+LABEL = bookLipatovNesterov
+TYPE = book
+AUTHORL = Lipatov|Nesterov
+AUTHORF = Y. |A.
+AUTHORM = S. |E.
+TITLE = Thermodynamics of Polymer Blends
+PUBL = Technomic
+PLACE = Lancaster, Basel
+YEAR = 1997
+----------
+LABEL = bookCloizeaux
+TYPE = book
+AUTHORP = des
+AUTHORL = Cloizeaux|Jannink
+AUTHORF = J. |G.
+TITLE = Polymers in Solutions: Their modelling and Structure
+PUBL = Clarendon Press
+PLACE = Oxford
+YEAR = 1990
+PAGES = 896
+----------
+LABEL = LifshitzGrosbergKhokhlov1
+TYPE = article
+AUTHORL = Lifshitz|Grosberg|Khokhlov
+AUTHORF = I. |A. |A.
+AUTHORM = M. |Yu. |R.
+JOURNAL = Rev. Mod. Phys.
+VOL = 50
+PAGE = 683
+EPAGE = 713
+YEAR = 1978
+TITLE = Some problems of the statistical physics of polymer chains with volume interaction
+URL = RevModPhys_LifshitsGrosbergKhokhlov1978.pdf
+----------
+LABEL = Vasilevskaya
+TYPE = article
+AUTHORP = | | | |ten
+AUTHORL = Vasilevskaya|Klochkov|Khalatur|Khokhlov|Brinke
+AUTHORF = V. |A. |P. |A. |G.
+AUTHORM = V. |A. |G. |R. |
+TITLE = Microphase separation within comb-like copolymer with attractive side-chains: computer simulations
+JOURNAL = Macromol. Theory and Simul.
+VOL = 10
+PAGE = 389
+EPAGE = 394
+YEAR = 2001
+URL = vasilevskaya_attractive.pdf
+----------
+LABEL = Helfand1
+TYPE = article
+AUTHORL = Helfand|Wasserman
+AUTHORF = E. |Z.
+AUTHORM = |R.
+TITLE =
+JOURNAL = Macromolecules
+VOL = 9
+PAGE = 879
+YEAR = 1976
+----------
+LABEL = Tsukahara0
+TYPE = edbook
+AUTHORL = Tsukahara
+AUTHORF = Y.
+BOOKTITLE=Macromolecular Design: Concept and Practice
+AUTHORI =
+AUTHORE = Mishra
+AUTHORG = M.
+AUTHORH =
+PAGE = 161
+EPAGE = 227
+PUBL = Polymer Frontiers International Inc.
+PLACE = New York
+YEAR = 1993
+----------
+LABEL = Schmidt
+TYPE = article
+AUTHORL = Tsukahara|Tsutsumi|Yamashita|Shimada
+AUTHORF = Y. |K. |S. |S.
+TITLE =
+JOURNAL = Macromolecules
+VOL = 23
+PAGE = 5201
+YEAR = 1990
+----------
+LABEL = Tsukahara2
+TYPE = article
+AUTHORL = Tsukahara|Mizuno|Segawa|Yamashita
+AUTHORF = Y. |K. |A. |Y.
+TITLE =
+JOURNAL = Macromolecules
+VOL = 22
+PAGE = 1546
+EPAGE = 1552
+YEAR = 1989
+----------
+LABEL = Tsukahara3
+TYPE = article
+AUTHORL = Tsukahara|Tsutsumi|Yamashita
+AUTHORF = Y. |K. |Y.
+TITLE =
+JOURNAL = Macromolecules
+VOL = 22
+PAGE = 2869
+EPAGE = 2871
+YEAR = 1989
+----------
+LABEL = Ballauff
+TYPE = article
+AUTHORL = Ballauff
+AUTHORF = M.
+AUTHORM =
+TITLE =
+JOURNAL = Angew. Chem. Int. Ed. Engl.
+VOL = 28
+PAGE = 253
+YEAR = 1989
+----------
+LABEL = Antonietti
+TYPE = article
+AUTHORL = Antonietti|Henke|Th\"unemann
+AUTHORF = M. |S. |A.
+AUTHORM = | |F.
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+VOL = 55
+PAGE = 1241
+EPAGE = 1310
+TITLE = Phase transitions in lyotropic colloidal and polymer liquid crystals
+URL = rp920803.pdf
+----------
+LABEL = WangSafran
+TYPE = article
+AUTHORL = Wang |Safran
+AUTHORF = Z.-G.|S.
+AUTHORM = |A.
+JOURNAL = J. Chem. Phys.
+YEAR = 1988
+VOL = 89
+PAGE = 5323
+EPAGE = 5328
+TITLE = Size distribution for aggregates of associating polymers. II. Linear packing
+URL =
+----------
+LABEL = BrinkeIkkala
+TYPE = article
+AUTHORP = ten
+AUTHORL = Brinke|Ikkala
+AUTHORF = G. |O.
+AUTHORM =
+JOURNAL = TRIP
+YEAR = 1997
+VOL = 5
+PAGE = 213
+EPAGE = 217
+TITLE =
+URL =
+----------
+LABEL = Beers1
+TYPE = article
+AUTHORP =
+AUTHORL = Beers|Scott|Mattyjaszewski|Sheiko|M\"oller
+AUTHORF = K. |G. |K. |S. |M.
+AUTHORM = L. |G. | |S. |
+JOURNAL = Macromolecules
+YEAR = 1998
+VOL = 31
+PAGE = 9413
+EPAGE = 9415
+TITLE = The Synthesis of Densely Grafted Copolymers by Atom Transfer Radical Polymerization
+URL = ma981402i.pdf
+----------
+LABEL = Borner1
+TYPE = article
+AUTHORP =
+AUTHORL = B\"orner|Beers|Matyjaszewski|Sheiko|M\"oller
+AUTHORF = H. |K. |K. |S. |M.
+AUTHORM = G. | | |S. |
+JOURNAL = Macromolecules
+YEAR = 2001
+VOL = 34
+PAGE = 4375
+EPAGE = 4383
+TITLE = Synthesis of Molecular Brushes with Block Copolymer Side Chains Using Atom Transfer Radical Polymerization
+URL = ma010001r.pdf
+----------
+LABEL = Schappacher
+TYPE = article
+AUTHORP =
+AUTHORL = Schappacher|Billaud|Paulo|Deffieux
+AUTHORF = M. |C. |C. |A.
+AUTHORM =
+JOURNAL = Macromol. Chem. Phys.
+YEAR = 1999
+VOL = 200
+PAGE = 2377
+EPAGE = 2386
+TITLE = Synthesis, dimensions and solution properties of linear and macrocyclic poly(chloroethyl vinyl ether)-g-polystyrene comblike polymers
+URL = schappacher.pdf
+----------
+LABEL = Wintermantel1
+TYPE = article
+AUTHORP =
+AUTHORL = Wintermantel|Schmidt|Tsukahara|Kajiwara|Kohjiya
+AUTHORF = M.|M.|Y.|K.|S.
+AUTHORM =
+JOURNAL = Macromol. Rapid. Commun.
+YEAR = 1994
+VOL = 15
+PAGE = 279
+EPAGE = 284
+TITLE =
+URL =
+----------
+LABEL = Wintermantel2
+TYPE = article
+AUTHORP =
+AUTHORL = Wintermantel|Fischer|Gerle|Ries|Schmidt|Kajiwara|Urakawa|Wataoka
+AUTHORF = M.|K.|M.|R.|M.|K.|H.|I.
+AUTHORM =
+JOURNAL = Angew Chem. Int. Ed. Engl.
+YEAR = 1995
+VOL = 34
+PAGE = 1472
+EPAGE = 1474
+TITLE =
+URL =
+----------
+LABEL = Wintermantel3
+TYPE = article
+AUTHORP =
+AUTHORL = Wintermantel|Gerle|Fischer|Schmidt|Wataoka|Urakawa|Kajiwara|Tsukahara
+AUTHORF = M.|M.|K.|M.|I.|H.|K.|Y.
+AUTHORM =
+JOURNAL = Macromolecules
+YEAR = 1996
+VOL = 29
+PAGE = 978
+EPAGE = 983
+TITLE = Molecular Bottlebrushes
+URL = ma950227s.pdf
+----------
+LABEL = GerleRoos
+TYPE = article
+AUTHORP =
+AUTHORL = Gerle|Fischer|Roos|M\"uller|Schmidt|Sheiko|Prokhorova|M\"oller
+AUTHORF = M. |K. |S. |A. |M. |S. |S. |M.
+AUTHORM = | | |H.~E. | |S.
+JOURNAL = Macromolecules
+YEAR = 1999
+VOL = 32
+PAGE = 2629
+EPAGE = 2637
+TITLE = Main Chain Conformation and Anomalous Elution Behavior of Cylindrical Brushes As Revealed by GPC/MALLS, Light Scattering, and SFM
+URL = ma9816463.pdf
+----------
+LABEL = FischerGerleSchmidt
+TYPE = article
+AUTHORP =
+AUTHORL = Fischer|Gerle|Schmidt
+AUTHORF = K.|M.|M.
+AUTHORM =
+JOURNAL = Proc. ACS PMSE Anaheim
+YEAR = 1999
+VOL = 30
+PAGE = 133
+EPAGE = 134
+TITLE =
+URL =
+----------
+LABEL = FischerSchmidt
+TYPE = article0
+AUTHORP =
+AUTHORL = Fischer|Schmidt
+AUTHORF = K.|M.|M.
+AUTHORM =
+JOURNAL = Macromol Rapid Commun
+YEAR = 2001
+VOL =
+PAGE =
+EPAGE =
+TITLE =
+URL =
+STATE = in press
+----------
+LABEL = Sheiko2
+TYPE = article
+AUTHORP =
+AUTHORL = Sheiko
+AUTHORF = S.
+AUTHORM = S.
+JOURNAL = Advances Polym. Sci.
+YEAR = 2000
+VOL = 151
+PAGE = 61
+EPAGE = 174
+TITLE =
+URL =
+----------
+%LABEL=kukuku
+%TYPE=preprint
+%AUTHORL=kukuauth
+%TITLE=Microphase separation within comb-like copolymer with attractive side-chains: computer simulations1
+%JOURNAL= Macromol. Theory and Simul1.
+%YEAR =1995
+%VOL =4
+%----------
+EOF
+
+
+
+
+
+
+
+
diff --git a/support/biblio/EXAMPLES/hairy/hairy.tex b/support/biblio/EXAMPLES/hairy/hairy.tex
new file mode 100644
index 0000000000..0c3a89d23c
--- /dev/null
+++ b/support/biblio/EXAMPLES/hairy/hairy.tex
@@ -0,0 +1,895 @@
+\documentstyle[aps,preprint]{revtex}
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+
+\newcommand{\lbl}[1]{\label{#1}}
+\newcommand{\reff}[1]{eq~\ref{#1}}
+
+
+\newcommand{\be}[1]{ \begin{equation} \lbl{#1} }
+\newcommand{\ee}{\end{equation}}
+
+\newcommand{\bea}[1]{ \begin{eqnarray} \lbl{#1} }
+\newcommand{\eea}{\end{eqnarray}}
+
+\newcommand{\dd}{\partial}
+
+\newcommand{\vk}{\bf k}
+\newcommand{\vb}{\bf b}
+
+
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\begin{document}
+
+\title{Phase equilibria in associating rodlike and flexible chains}
+
+\date{\today}
+
+\author{R. Stepanyan$^{\dagger}$,
+ A. Subbotin$^{\dagger ,\sharp}$,
+ O. Ikkala$^{\ddagger}$,
+ G. ten Brinke$^{\dagger}$}
+
+\address{$^{\dagger }$
+Department of Polymer Science and Material Science Center,\\
+University of Groningen, Nijenborgh 4, 9747 AG Groningen, The Netherlands;}
+
+\address{$^{\sharp }$
+Institute of Petrochemical Synthesis, Russian Academy of\\
+Sciences, Moscow 119991, Russia;}
+
+\address{$^{\ddagger }$
+Department of Engineering Physics and Mathematics, \\
+Helsinki University of Technology, P.O. Box 2200,\\
+FIN-02015 HUT, Espoo, Finland}
+
+\date{\today}
+
+\maketitle
+
+\begin{abstract}
+Abstract goes here
+\end{abstract}
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\newpage
+
+\section{Introduction}
+
+Introduction......
+
+\cite{MB1091,BF525,bookdeGennesScalingConcepts,Leibler}.
+%-----------------------------------------------------------------
+
+\section{The model and the free energy of the reference system}
+
+Let us consider a melt consisting of rigid rods of length $L$ and diameter
+$d$ and flexible coils consisting of $N$ beads of volume $\nu$ and statistical
+segment of length $a$. The coil size is $R_c = a \sqrt{N}$. We will assume that
+each rod contains $M$ associating groups (an average distance between two
+succesive groups is $b=L/M \ll R_c$) which can form bonds with the
+associating end of the coil (FIGURE). It is assumed that each coil has only one
+associating end. The energy of association between rod and coil equals
+to $-\epsilon $. The concentration of rods in the melt is $c$ and their volume
+fraction is $f=(\pi /4)Ld^2c$.
+
+The interactions between rods and coils can be introduced in the
+following way. It is well known that rods and polymer coils in the
+molten state are practically incompartible and separate on the nematic phase
+consisting of rods and isotropic phase consisting of the flexible
+polymers \cite{Flory:MML:11:1138,AbeBallauff}.
+Let us consider the interface between the nematic and isotropic phases
+(FIGURE fig.1)
+which is assumed to be sharp so that the polymer segments can not
+penetrate into the nematic phase, and introduce the interfacial tension
+$\gamma$ corresponding to planar orientation of rods at the interface
+($k_B \equiv 1$)
+%
+\be{eq0}
+\gamma =(w+sT)/d^2
+\ee
+%
+where $w$ is the energetic part of the surface energy and $s$ is the
+entropic part
+(here $T$ is temperature, ??we will also assume that $s \sim 1$??).
+According to the defenition \reff{eq0} if a rod penetrates into the polymer
+melt its energy loss approximatly equals
+%
+\be{eq01}
+\mu _r\simeq 2Ld\gamma =\frac{2L}d\left( w+sT\right)
+\ee
+The free energy of the isotropic phase with small amount of rigid rods
+therefore is given by
+
+\be{eq02}
+{\cal F}_I^{*} =
+T V c
+\ln \left( \frac{f}{e} \right) +
+T V \frac{1-f}{N\nu}
+\ln \left( \frac{1-f}{e} \right) +
+V c \frac{2L}{d} \left( w+sT \right)
+\ee
+%
+Here we omitted interaction between the rods. $V$ is the volume of the
+system. In \reff{eq02} the first two terms imply the translational
+energy of the rods and coils correspondingly and the last term is the energy of
+rods.
+
+The coils can also penetrate into the nematic phase where they become
+stretched. In order to write the free energy of the nematic phase with small
+amount of coils we introduce a chemical potential of the coil in the
+nematic phase $\mu _c$ which includes both energetic and entropic
+parts and limits to infinity,
+
+\be{eq05}
+\mu _c/T\rightarrow \infty
+\ee
+for arbitrary $T$. As we will see below it means that the coils
+practically do not penetrate in the nematic phase.
+
+The free energy of the nematic phase contains also a term connected with
+orientational ordering of rods. The last one can be estimated as
+\cite{KhokhlovTBOA,SemenovKhokhlov}
+$T \ln ( 4 \pi /\Omega )$,
+where $\Omega$ is the characteristic fluctuation angle,
+$\Omega \simeq 2\pi (d/L)^2$. Thus the free energy is given by
+%
+\be{eq03}
+{\cal F}_N^{*}=
+T V c \ln \left( \frac{f}{e} \right) +
+T V \frac{1-f}{N\nu}
+\ln \left( \frac{1-f}e \right) +
+2 T V c \ln \left( \frac{L}{d} \right) +
+V \frac{1-f}{N\nu} \mu _c
+\ee
+The phase equilibrium between the nematic and isotropic phases can be found
+in a usuall way by equating the chemical potentials and osmotic pressures in
+both phases.
+%
+\begin{eqnarray}
+\mu_I^{*} & = & \mu _N^{*}; \quad
+\mu _{I,N}^{*} = \frac{1}{V} \frac{\dd {\cal F}_{I,N}^{*}}{\dd c}
+ \nonumber\\
+%
+P_I &=&P_N; \quad
+P_{I,N}=\frac{1}{V}
+\left(
+ c \, \frac{\dd {\cal F}_{I,N}^{*}}{\dd c} - {\cal F}_{I,N}^{*}
+\right)
+\lbl{eq04}
+\end{eqnarray}
+Considering limit \reff{eq05}, solution of these equations is given by
+%
+\be{eq06}
+f_N \simeq 1,\quad
+f_I \simeq
+ \left( \frac{L}{d} \right) ^2
+ \exp \left( -\frac{2L}{d}\left( \frac wT+s \right)
+ \right) \ll 1
+\ee
+
+\section{Nematic-isotropic liquid phase coexistence: effect of association}
+%
+In this section we study the influence of association between rods and
+coils on the macrophase separation described above.
+We start from the free energy of association between
+rods and coils, ${\cal F}_{bond}$, assuming that they are
+ideal (without excluded volume). Let us introduce the probability of bond
+$p$. The total number of bonds in the system is $VMcp$ and
+equals to the number of associated coils.
+Therefore the number of free coils in the system is
+$(V/N\nu)(1-f-f\kappa pN)$, where $\kappa \equiv \nu/(\pi b d^2/4)$. The free
+energy of bonds can be written through the partition function $Z_{bond}$ as
+\cite{SemenovRubinstein1,Erukhimovich:Gel}
+%
+\be{eq3}
+{\cal F}_{bond}=-T\ln Z_{bond}
+\ee
+where
+%
+\be{eq4}
+Z_{bond} =
+ P_{comb}
+ \left( \frac{v_b}V \right)^{V M c p}
+ \exp \left( \frac{\epsilon \, V M c p}{T} \right)
+\ee
+and $P_{comb}$ is the number of different ways to bond rods and coils
+for a fixed probability of bond $p$; $v_b$ is a bond volume. If we denote
+the number of rods in the system as ${\cal N}_r=Vc$, and the number of coils
+as ${\cal N}_c=V(1-f)/N\nu$ then the number of ways to choose ${\cal N}_rMp$
+coils for bonds formation is a binomial coefficient
+%
+\be{eq5}
+C_{{\cal N}_c}^{{\cal N}_rMp}=\frac{{\cal N}_c!}{({\cal N}_rMp)!({\cal N}_c-%
+{\cal N}_rMp)!}
+\ee
+%
+On the other hand there are
+%
+\be{eq6}
+\frac{({\cal N}_rM)!}{({\cal N}_rM(1-p))!}
+\ee
+different ways to select ${\cal N}_rMp$ bonds from ${\cal N}_rM$
+associating groups. Therefore
+
+\be{eq7}
+P_{comb} = C_{{\cal N}_c}^{{\cal N}_rMp}
+ \frac{ ({\cal N}_rM)! }{ ({\cal N}_rM(1-p))! }
+\ee
+and the free energy of bonds is given by
+%
+\begin{eqnarray}
+{\cal F}_{bond} & = &
+VMcp
+\left[
+ T \ln \left( \frac{N\nu}{v_b} \right) - \epsilon
+\right] +
+TVcM
+\left[
+ p\ln p + (1-p) \ln (1-p)
+\right] \nonumber\\
+%
+ & & +
+TV \frac{\left( 1-f-f\kappa Np\right) }{N\nu}
+ \ln \left( \frac{1-f-f\kappa Np}{e} \right) -
+TV \frac{(1-f)}{N\nu}
+ \ln \left( \frac{1-f}{e} \right)
+\lbl{eq8}
+\end{eqnarray}
+
+Thus the free energy of the isotropic phase can be presented as the following
+%
+\be{eq9}
+{\cal F}_I = {\cal F}_I^{*} + {\cal F}_{bond} + {\cal F}_{el}
+\ee
+%
+where ${\cal F}_{el}$ is the elastic free energy of the side chains
+of the hairy
+rod when the density of association is high enough. We approximate it
+by \cite{3dFlex,2sorts}
+
+\be{eq10}
+{ \cal F}_{el}=
+\left[
+ \begin{array}{cl}
+ TVc\frac{3\kappa d^2}{32a^2}Mp^2\ln \left( \kappa Np\right) ,\quad &
+ p>\frac{1}{\kappa N} \\
+ 0, \quad &
+ \textrm{otherwise}
+ \end{array}
+\right.
+\ee
+Hence the final expression for the free energy of the isotropic phase is
+given by (per volume of one rod $(\pi /4)Ld^2)$
+%
+\begin{eqnarray}
+\frac{F_I(f,p)}T &=&
+ f\frac{2L}{d} \left( \frac wT+s \right)
+ +Mfp\left[ \ln \left( \frac{N\nu}{v_b}\right) -\frac \epsilon T \right]
+ +fM\left[ p\ln p+(1-p)\ln (1-p)\right] \nonumber\\
+&&
+ +f\ln \left( \frac fe \right)
+ +M \frac{\left( 1-f-f \kappa Np \right) }{N\kappa }
+ \ln \left( \frac{1-f-f\kappa Np}{e} \right) \nonumber\\
+&&
+ +f\frac{3\kappa d^2}{32a^2} Mp^2
+ \ln \left( \kappa Np \right) H\left( p-\frac 1{\kappa N}\right)
+\lbl{eq11}
+\end{eqnarray}
+%
+where
+%
+$$
+H(x)=
+\left[
+ \begin{array}{cl}
+ 1,\quad & x \geq 0 \\
+ 0,\quad & x < 0
+ \end{array}
+\right.
+$$
+is the Heavyside's function.
+Similarly, the free energy of the nematic phase is
+%
+\begin{eqnarray}
+\frac{F_N(f,p)}T &=&
+ 2 f \ln \left( \frac Ld \right)
+ +M\frac{1-f}{N\kappa }\frac{\mu _c}T
+ +Mfp\left[ \ln \left( \frac{N\nu}{v_b}\right)
+ -\frac \epsilon T\right]
+ +fM\left[ p\ln p+(1-p)\ln (1-p)\right] \nonumber\\
+&&
+ +f\ln \left( \frac fe\right)
+ +M\frac{\left( 1-f-f\kappa Np\right) }{ N\kappa }
+ \ln \left( \frac{1-f-f\kappa Np}e\right)
+\lbl{eq12}
+\end{eqnarray}
+%
+%
+The probability of bonding in both phases can be found from the minimization
+of the corresponding free energies
+%
+\be{eq13}
+\frac{\dd F_I}{\dd p}=0;
+\quad
+\frac{\dd F_N}{\dd p}=0
+\ee
+%
+and is given by ($N^* \equiv N \nu / v_b$)
+%
+\be{eq14}
+p= \frac{1}{2\kappa Nf}
+\left[
+ 1-f+\kappa Nf-\epsilon /(TN^{*})-
+ \sqrt{
+ \left(1-f+\kappa Nf-\epsilon /(TN^{*}) \right) ^2
+ -4\kappa Nf(1-f)
+ }
+\right]
+\ee
+for the nematic phase and for the isotropic phase when $p<\frac 1{\kappa N}$.
+%Here $N^{*}\equiv N\nu/v_b.$
+For $p>\frac 1{\kappa N}$ the probability of
+bonding in the isotropic phase obeys
+%
+\be{eq15}
+ \ln
+ \left[
+ \frac{ pN^{*}e^{-\epsilon /T} }
+ { \left( 1-p\right) \left(1-f_I-f_I\kappa Np\right) }
+ \right]
+ +\frac{3\kappa d^2p}{16a^2}\ln \left( \kappa Npe\right)
+ = 0
+\ee
+%
+and for a small volume fraction of rods, $f_I \ll 1$, is approximately given by
+%
+\be{eq24}
+p \simeq \frac 1{ 1 + N^{*} e^{-\epsilon^{*}/T}},
+\quad
+\epsilon ^{*} = \epsilon -
+ \frac{3\kappa d^2T}{32a^2} \,
+ \frac{1}{1+N^{*}e^{-\epsilon /T}}
+ \ln \left( \frac{\kappa N}{1+N^{*} e^{-\epsilon /T}} \right)
+\ee
+%
+Phase equilibrium between the isotropic and nematic phases can be found in a
+standard way from the equilibrium equations
+%
+\begin{eqnarray}
+\frac{\dd F_I}{\dd f_I} &=& \frac{\dd F_N}{\dd f_N}
+\nonumber \\
+f_I\frac{\dd F_I}{\dd f_I}-F_I &=& f_N\frac{\dd F_N}{\dd f_N}-F_N
+\lbl{eq16}
+\end{eqnarray}
+using eqs.~\ref{eq11},\ref{eq12} together with \reff{eq14} and \reff{eq24}.
+When the probability of bonding in the
+isotropic phase $p_I<\frac 1{\kappa N}$
+(or equivalently $\frac{\epsilon}{T} < \ln \frac{\nu}{\kappa v_b}$),
+expression \reff{eq14} can be used giving the volume fraction of rods
+%
+\begin{eqnarray}
+f_N & \simeq & 1,
+ \nonumber\\
+f_I & \simeq &
+ \left( \frac Ld \right) ^2
+ \exp
+ \left(
+ -\frac{2L}{d}
+ \left( \frac wT+s\right)
+ +\frac M{1+N^{*}e^{-\epsilon /T}}
+ \left( \frac \epsilon T-\ln N^{*}\right)
+ \right) \ll 1
+\lbl{eq17}
+\end{eqnarray}
+%
+However, if
+$p_I>\frac 1{\kappa N}$
+(or $\frac \epsilon T>\ln \frac \nu{\kappa v_b}$),
+the volume fraction of rods in the nematic phase
+is still close to the unity whereas $f_I$ obeys the equation
+%
+\be{eq18}
+\ln f_I
+- Mp_I \ln \left( 1-f_I-f_I\kappa Np_I \right)
+\simeq
+2 \ln \left( \frac L d\right)
++ \frac M{N\kappa} - \frac{2Ls}{d}
+-Mp_I\ln N^{*}
++\frac{1}{T} \left( Mp_I\epsilon -\frac{2Lw}d \right)
+\ee
+where $p_I$ has to be determined from \reff{eq15}.
+Obviously, for $T \to 0$ $p_I \to 1$ and therefore the last term
+in eq.\ref{eq17} becomes dominant. Depending on its sign two
+characteristical assymptotics can be distinguished
+%
+\begin{eqnarray}
+f_I \to 0 \qquad\qquad\textrm{if }\quad M\epsilon <\frac{2Lw}d
+\nonumber\\
+f_I \to \frac 1{1+N\kappa } \quad\textrm{if }\quad M\epsilon >\frac{2Lw}d
+\label{eq19}
+\end{eqnarray}
+Thus for $\epsilon /w>2b/d$ rods and coils become partially compartible.
+This fact has a clear physical meaning. Negative sign of
+$-\epsilon + \frac{2Lw}{Md}$ corresponds to the negative ``total'' energy
+($\epsilon$-part plus $\gamma$-part)
+due to attaching of a coil to a rod, i.e. making it favorable to keep
+\emph{all} coils bonded (for $T\to 0$, of course).
+Further on we consider only the case $\epsilon /w>2b/d$,
+where a region of compatibility of rods and coils exists.
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+
+\section{Phase equilibria between nematic, isotropic liquid and microphases}
+
+There are two mechanisms of attraction between hairy rods, namely due to
+incompartibility of the rods and coils and due to nonhomogeneous
+distribution of the free polymer coils which is created by the hairy rods.
+These mechanisms ultimately result in formation hexagonal and lamellar
+structures in the blend. Moreover we can separate two different hexagonal
+phases. In one of the phases (we call it H1) the mechanism connected with
+nonhomogeneous distribution of the free polymers is dominant and the
+''cylinders'' contain only one rod per unit cell $(Q=1)$. In the second
+phase (H2) the surface term becomes important so that rods attract each
+other and the cylinders contain $Q>1$ rods per unit cell (fig.2FIGURE). With
+decreasing temperature the cylinders first adopts elipsoidal form and
+finally transform to the lamellar phase.
+
+\subsection{Separation of the hexagonal phase H1}
+
+Let us start with calculation of the interaction energy between the
+cylinders in the hexoganal phases (H1, H2). It is connected with
+nonhomogeneous distribution of the free polymer coils and is given by (per
+cylinder of unit length)
+
+\be{eq20}
+U_H(Q)=
+\frac{N\nu(Qp)^2}{2b}
+\left[
+ \frac 2{\sqrt{3} \, \ell ^2}
+ \sum_{\{ \vb \}}
+ \frac{h^2(\frac{a^2N{\vk}^2}6)}{g(\frac{a^2N{\vk}^2}6)}
+ -\frac 1{4\pi ^2}
+ \int d{\vk}\frac{h^2(\frac{a^2N{\vk}^2}6)}{g(\frac{a^2N{\vk}^2}6)}
+\right]
+\ee
+where $\ell $ is the period of the structure, $\{ \vb \}$ are the vectors
+of the reciprocal lattice,
+$$h(u) =\frac 1u\left( 1-e^{-u}\right) $$
+$$g(u) =\frac 2{u^2}\left( u-1+e^{-u}\right)$$
+
+After calculation of the sum and integral in eq.\ref{eq20} we find the
+interaction energy per volume $(\pi /4)Ld^2$
+
+\be{eq21}
+U_H(Q)=-\frac 3{32}\frac{\kappa MQp^2fd^2}{a^2N}
+ \left[
+ 3.457
+ +\ln \left( \frac{a^2Nf}{Qd^2}\right)
+ \right]
+\ee
+Thus the free energy of H1 phase is given by
+%
+\begin{eqnarray}
+\frac{F_{H1}}T &=&
+ f\frac{2L}{d} \left( \frac wT+s\right)
+- Mfp\left[ \frac \epsilon T - \ln N^{*} \right]
++ fM\left[ p\ln p+(1-p)\ln (1-p) \right]
++ 2f\ln \left( \frac Ld \right)
+\nonumber \\
+&&
++ M\frac{\left( 1-f-f\kappa Np\right) }{N\kappa }
+ \ln \left( \frac{1-f-f\kappa Np}e\right)
++ f\frac{3\kappa d^2}{32a^2}Mp^2\ln \left( \kappa Np\right)
+\nonumber \\
+&&
+- \frac{3}{32} \frac{\kappa Mp^2fd^2}{a^2N}
+ \left[ 3.457+\ln \left( \frac{a^2Nf}{d^2}\right) \right]
+\lbl{eq22}
+\end{eqnarray}
+Here we approximated the loss of the orientational energy of rod by the term
+$2Tf\ln \left( \frac Ld\right) $, and omitted the loss of it translational
+entropy because it is relatively small. Phase equilibrium between isotropic
+phase and H1 phase can be found from the equilibrium equations
+%
+\begin{eqnarray}
+ \frac{\dd F_I}{\dd f_I} =\frac{\dd F_{H1}}{\dd f_{H1}},
+ &\quad&
+ \frac{\dd F_I}{\dd p_I}=\frac{\dd F_{H1}}{\dd p_{H1}}=0
+\nonumber\\
+ f_I\frac{\dd F_I}{\dd f_I}-F_I
+ &=&
+ f_{H1}\frac{\dd F_{H1}}{\dd f_{H1}}-F_{H1}
+\lbl{eq23}
+\end{eqnarray}
+and the probability of bonding and the binodal lines are
+%
+\begin{eqnarray}
+ & p_1 \simeq & p_{H1}\simeq 1,
+\nonumber \\
+ & f_{H1}^{(1)} \simeq & \frac 3{16}\frac{d^2}{a^2 N},
+\nonumber \\
+ & f_I \simeq &
+ \left( \frac Ld\right) ^2
+ \exp \left( -\frac 3{16}\frac{d^2p^2\kappa M}{a^2}\right) \simeq 0
+\lbl{eq26}
+\end{eqnarray}
+
+Similarly the phase equilibrium between the nematic and H1 phases follow
+from equations
+%
+\begin{eqnarray}
+ \frac{\dd F_N}{\dd f_N} =\frac{\dd F_{H1}}{\dd f_{H1}},
+ &\quad&
+ \frac{\dd F_N}{\dd p_N}=\frac{\dd F_{H1}}{\dd p_{H1}}=0
+\nonumber\\
+ f_N\frac{\dd F_N}{\dd f_N}-F_N
+ &=&
+ f_{H1}\frac{\dd F_{H1}}{\dd f_{H1}}-F_{H1}
+\lbl{eq25}
+\end{eqnarray}
+%
+and solution is given by
+%
+\begin{eqnarray}
+& p_N \simeq &0, \quad p_{H1}\simeq 1, \nonumber \\
+& f_N \simeq &1, \nonumber\\
+& f_{H1}^{(2)} \simeq &\frac 1{1+\kappa N}
+ \left[
+ 1-\exp
+ \left(
+ -\frac{\epsilon}{T}
+ +\frac{2bw}{Td}
+ +\frac{2bs}d+\ln N^{*}
+ +\frac{3\kappa d^2}{32a^2}\ln \left( \kappa N\right)
+ \right)
+ \right]
+\lbl{eq251}
+\end{eqnarray}
+The critical temperature $(\epsilon /T)_c$ can be obtained from the
+intersection of the curves $f_{H1}^{(1)}$ and $f_{H1}^{(2)}$, and obeys the
+following equation
+%
+\be{eq27}
+(\epsilon /T)_c =
+ \frac{1}{1-\frac{2bw}{\epsilon d}}
+ \left( \frac{2bs}d+\ln
+ N^{*}+\frac{3\kappa d^2}{32a^2} \ln \left( \kappa N \right)
+ \right)
+\ee
+where the probability of bonding $p_c\simeq 1.$ Thus the hexagonal H1 phase
+is stable for $f_{H1}^{(1)}<f<f_{H1}^{(2)}$; for $f_I<f<f_{H1}^{(1)}$ the
+system separates on the isotropic and H1 phase and for $f_{H1}^{(1)}<f<f_N$
+it separates on the H1 and nematic phase.
+
+\subsection{Separation of the hexagonal phase H2}
+
+Let us follow along the binodal line $f_{H1}^{(1)}(T)$ decreasing the
+temperature. At some temperature H1 phase becomes unstable with respect to
+separation of the isotropic phase and the hexagonal H2 phase. The
+corresponding triple point can be obtained from the system of equations
+
+\begin{eqnarray}
+\frac{\dd F_I}{\dd f_I}
+=\frac{\dd F_{H1}}{\dd f_{H1}}
+=\frac{\dd F_{H2}}{\dd f_{H2}} \, ,
+\qquad
+\frac{\dd F_I}{\dd p_I}
+=\frac{\dd F_{H1}}{\dd p_{H1}}
+=\frac{\dd F_{H2}}{\dd p_{H2}}
+=0
+\nonumber \\
+f_I\frac{\dd F_I}{\dd f_I}-F_I
+=f_{H1}\frac{\dd F_{H1}}{\dd f_{H1}}-F_{H1}
+=f_{H2}\frac{\dd F_{H2}}{\dd f_{H2}}-F_{H2}
+\lbl{eq23a}
+\end{eqnarray}
+%
+where the free energy of the H2 phase for $Q<\sqrt{N}$ is given by
+%
+\begin{eqnarray}
+\frac{F_{H2}}T
+&=&
+ f\frac Ld\left( \frac wT+s\right) \left( 1+\frac 2Q\right)
+ +Mfp\left[ \ln N^{*}-\frac \epsilon T\right]
+ +fM\left[ p\ln p+(1-p)\ln (1-p)\right]
+\nonumber \\
+&&
+ +2f\ln \left( \frac Ld\right)
+ +M\frac{\left( 1-f-f\kappa Np\right) }{\kappa N}
+ \ln \left( \frac{1-f-f\kappa Np}e\right)
+ +f\frac{3d^2\kappa Q}{32a^2}Mp^2\ln \left( \kappa Np\right)
+\nonumber \\
+&&
+ -\frac 3{32}\frac{\kappa MQp^2fd^2}{a^2N}
+ \left[ 3.457+\ln \left( \frac{a^2Nf}{Qd^2}\right) \right]
+\lbl{eq28}
+\end{eqnarray}
+and the number of rods $Q$ in the cross-section of the cylinder can be
+calculated from the minimum condition $\dd F_{H2}/\dd Q=0$,
+%
+\be{eq28a}
+Q \simeq
+\sqrt{
+ \frac{64ba^2}{3\kappa p^2d^3 \ln \left( \kappa N \right) }
+ \left( \frac wT+s \right)
+}
+\ee
+Solution of the eqs.~\ref{eq23a} is given by
+%
+\begin{eqnarray}
+&& p_I \simeq p_{H1} \simeq p_{H2}\simeq 1 \nonumber \\
+&& Q_1 \simeq 2+\sqrt{2},
+\quad
+f_I\simeq 0,
+\quad
+f_{H1}^{(1)} \simeq \frac 3{16} \frac{d^2}{a^2N},
+\quad
+f_{H2}^{(1)} \simeq \frac 3{16}\frac{Q_1d^2}{a^2N}
+\lbl{eq28b}
+\end{eqnarray}
+and the critical temperature is
+
+\be{eq23e}
+\frac w{T_{c1}} \simeq -s+\frac{3\kappa d^3 Q_1^2}{64 b a^2}
+ \ln \left( \kappa N \right)
+\ee
+
+Similarly we the binodal line $f_{H1}^{(1)}(T)$ finishes at the triple point
+which can be found from the system of equations
+
+\begin{eqnarray}
+&&\frac{\dd F_N}{\dd f_N} =
+\frac{\dd F_{H1}}{\dd f_{H1}} =
+\frac{\dd F_{H2}}{\dd f_{H2}},
+\quad
+\frac{\dd F_N}{\dd p_N} =
+\frac{\dd F_{H1}}{\dd p_{H1}} =
+\frac{\dd F_{H2}}{\dd p_{H2}} =0
+\nonumber \\
+&&f_N\frac{\dd F_N}{\dd f_N}-F_N =
+f_{H1}\frac{\dd F_{H1}}{\dd f_{H1}}-F_{H1}=
+f_{H2}\frac{\dd F_{H2}}{\dd f_{H2}}-F_{H2}
+\lbl{eq23c}
+\end{eqnarray}
+%
+and is characterized by
+%
+\begin{eqnarray}
+&&
+p_N \simeq 0,
+\quad
+p_{H1} \simeq p_{H2} \simeq 1
+\nonumber\\
+&&
+Q_1^{^{\prime }} \simeq Q_1\simeq 2+\sqrt{2}, \quad f_N \simeq 1,
+\nonumber \\
+&&
+f_{H1}^{(2)}\simeq \frac 1{1+\kappa N}\left[ 1-\exp \left( -\frac \epsilon {%
+T_{c1}}+\frac{2bw}{T_{c1}d}+\frac{2bs}d+\ln N^{*}+\frac{3d^2\kappa }{32a^2}%
+\ln \left( \kappa N\right) \right) \right]
+\nonumber\\
+&&
+f_{H2}^{(2)}\simeq \frac 1{1+\kappa N}\left[ 1-\exp \left( -\frac \epsilon {%
+T_{c1}}+\left( \frac{2bw}{T_{c1}d}+\frac{2bs}d\right) \left( 1+\frac 2{Q_1}%
+\right) +\ln N^{*}+\frac{3d^2\kappa Q_1}{32a^2}\ln \left( \kappa N\right)
+\right) \right]
+%
+\lbl{eq23d}
+\end{eqnarray}
+
+In the first approximation the corresponding critical temperature coinside
+with the critical temperature \reff{eq23e}. Note, the small difference
+between these critical temperatures, which we do not consider here, result
+in a small area of phase separation between H1 and H2 phases.
+
+The phase equilibrium between the isotropic and the hexagonal H2 phase can
+be found based on the equations
+%
+\begin{eqnarray}
+&&
+ \frac{\dd F_I}{\dd f_I} =\frac{\dd F_{H2}}{\dd f_{H2}},
+ \quad
+ \frac{\dd F_I}{\dd p_I} = \frac{\dd F_{H2}}{\dd p_{H2}} =0
+\nonumber\\
+&&
+ f_I\frac{\dd F_I}{\dd f_I}-F_I = f_{H2}\frac{\dd F_{H2}}{\dd f_{H2}}-F_{H2}
+\lbl{eq231}
+\end{eqnarray}
+and for $1\ll Q<\sqrt{N\text{ }}$ the probability of bonding and the binodal
+lines are given by
+
+\begin{eqnarray}
+ && p_I \simeq p_{H2}\simeq 1,
+\nonumber\\
+ && f_I \simeq 0,\quad
+\nonumber \\
+ && f_{H2}^{(1)} \simeq
+ \frac 1{1+\kappa N}
+ \left[
+ 1-\exp \left( -\frac 3{16}\frac{Qd^2}{a^2N}\right)
+ \right]
+\lbl{eq28b1}
+\end{eqnarray}
+%
+where $Q$ defined by \reff{eq28a}. Similarly the equilibrium between the
+nematic and the hexagonal H2 phase obeys equations
+%
+\begin{eqnarray}
+&&
+ \frac{\dd F_N}{\dd f_N} = \frac{\dd F_{H2}}{\dd f_{H2}},
+ \quad
+ \frac{\dd F_N}{\dd p_N} = \frac{\dd F_{H2}}{\dd p_{H2}}=0
+\nonumber \\
+&&
+ f_N\frac{\dd F_N}{\dd f_N}-F_N = f_{H2}\frac{\dd F_{H2}}{\dd f_{H2}}-F_{H2}
+\lbl{eq232}
+\end{eqnarray}
+and the corresponding probabilities and binodals are
+%
+\begin{eqnarray}
+&&
+ p_N \simeq 0,\quad p_{H2}\simeq 1,
+\nonumber \\
+&&
+ f_N \simeq 1,
+\nonumber \\
+&&
+ f_{H2}^{(2)} \simeq \frac 1{1+\kappa N}
+ \left[
+ 1-\exp \left( -\frac{\epsilon}{T}
+ +\left( \frac{2bw}{Td}+\frac{2bs}d \right) \left( 1+\frac{2}{Q} \right)
+ +\ln N^{*}+\frac{3d^2\kappa Q}{32a^2} \ln \left( \kappa N\right) \right)
+ \right]
+\lbl{eq28b21}
+\end{eqnarray}
+
+With further decreasing temperature the number of rods in the cross-section $%
+Q$ becomes larger than $\sqrt{N}$ and the cylinders become elongated in one
+direction.
+
+\subsection{Separation of the lamellar phase}
+
+The free energy of the lamellar phase is
+%
+\begin{eqnarray}
+\frac{F_L}T &=&
+ f\frac Ld\left( \frac wT+s\right)
+ +Mfp\left[ \ln N^{*}-\frac \epsilon T\right]
+ +fM\left[ p\ln p+(1-p)\ln (1-p)\right]
+\nonumber \\
+&&
+ +2f\ln \left( \frac Ld\right)
+ +M\frac{\left( 1-f-f\kappa Np\right) }{\kappa N}
+ \ln \left( \frac{2h^{*}}\xi \frac{1-f-f\kappa Np}e\right)
+ +f\frac{ 3\pi ^2d^2\kappa ^2}{32a^2}NMp^3
+\nonumber \\
+&&
+ -0.227f^{*}M \left( \frac{p^2a^2}{\kappa ^2d^2N}\right) ^{1/3}
+ -1.312M \frac{(f-f^{*})}{f^{*}}
+ \left( \frac{p^2d^2}{\kappa a^2N^2}\right) ^{1/3}
+%
+\lbl{eq29}
+\end{eqnarray}
+where
+%
+$$
+h^{*}=\frac{\pi d}2\left( 1+\kappa Np \right) ;
+\quad
+\xi =\frac a{6\pi } \left( \frac{aN}{\kappa pd}\right) ^{1/3}
+$$
+%
+The phase equilibrium between the isotropic and the lamellar phase can be
+found from the equations
+%
+\begin{eqnarray}
+&&
+ \frac{\dd F_I}{\dd f_I} =\frac{\dd F_L}{\dd f_L},
+ \quad
+ \frac{\dd F_I}{\dd p_I}=\frac{\dd F_L}{\dd p_L}
+\nonumber \\
+&&
+ f_I\frac{\dd F_I}{\dd f_I}-F_I = f_L\frac{\dd F_L}{\dd f_L}-F_L
+\lbl{eq2311}
+\end{eqnarray}
+and the probability of bonding and the binodals are given by
+%
+\begin{eqnarray}
+&&
+ p_I \simeq p_L\simeq 1,
+\nonumber\\
+&&
+ f_I \simeq 0,
+\nonumber \\
+&&
+ f_L^{(1)} \simeq \frac{1}{1+\kappa N}
+ \left[
+ 1-\frac \xi {2h^{*}}
+ \exp \left( -1.312\left( \frac{\kappa ^2d^2N}{a^2}\right) ^{1/3}\right)
+ \right]
+\label{eq28b2}
+\end{eqnarray}
+Similarly the equilibrium between the nematic and the lamellar phase obeys
+equations
+%
+\begin{eqnarray}
+&&
+ \frac{\dd F_N}{\dd f_N} = \frac{\dd F_L}{\dd f_L},
+ \quad
+ \frac{\dd F_N}{\dd p_N} = \frac{\dd F_L}{\dd p_L}
+\nonumber \\
+&&
+ f_N \frac{\dd F_N}{\dd f_N}-F_N = f_L\frac{\dd F_L}{\dd f_L}-F_L
+\lbl{eq2321}
+\end{eqnarray}
+and the corresponding probabilities and binodals are
+%
+\begin{eqnarray}
+&&
+ p_N \simeq 0,
+ \quad
+ p_L\simeq 1,
+\nonumber\\
+&&
+ f_N \simeq 1,
+ \quad
+\nonumber \\
+&&
+ f_L^{(2)} \simeq \frac{1}{1+\kappa N}
+ \left[
+ 1-\exp \left( -\frac \epsilon T
+ +\frac{2bw}{Td}+\frac{2bs}d+\ln N^{*}
+ +\frac{3\pi ^2d^2\kappa ^2N}{32a^2}\right)
+ \right]
+\lbl{eq28b3}
+\end{eqnarray}
+
+\section{Discussion}
+
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+\newpage
+{\bf Literature}
+
+
+Relevant literature
+
+\cite{SemenovKhokhlov,SemenovRubinstein1,Erukhimovich:Gel}
+
+\cite{AndrikopoulosVlassopoulosVoyiatzis,Benmouna}
+
+\cite{KhalaturKhokhlov1,KhalaturKhokhlov2}
+
+\cite{SemenovNyrkovaKhokhlov,3dFlex}
+
+\cite{Angerman:PhaseAssocDiblock,Dormidontova:PhaseHbondBrush}
+
+Theory:
+
+\cite{Ballauff:CompatHairyRodsCoils,Ballauff:PhaseHairyRodsCoils}
+
+Lattice:
+
+\cite{SemenovBlockHomo,Leibler,bookChaikinLubensky,bookKorn}
+
+
+Hairy rods:
+
+Experiment:
+
+\cite{SteuerRehahnBallauff,AdamSpiess,SteuerHorthBallauff}
+
+\cite{GaldaKistnerMartinBallauff,PetekidisVlassopoulosFytas2}
+
+\cite{PetekidisVlassopoulosFytas1}
+
+
+\begin{references}
+
+\end{references}
+
+\end{document}
diff --git a/support/biblio/EXAMPLES/hairy/libtex b/support/biblio/EXAMPLES/hairy/libtex
new file mode 100755
index 0000000000..54db38c841
--- /dev/null
+++ b/support/biblio/EXAMPLES/hairy/libtex
@@ -0,0 +1,51 @@
+PREFIX="../../"
+VLEVEL="1" #verbosity level
+PROJECT="hairy"
+REFS=refers.db
+# FORMATS=$PREFIX"formats/physreve_with_title"
+FORMATS=$PREFIX"formats/macromolecules"
+ABBR=$PREFIX"formats/abbr.tex"
+
+SUFFIX=".1"
+
+BIBLIO=$PREFIX"biblio.pl"
+LATEX="latex"
+DVIPS="dvips"
+PSTOPS="pstops"
+
+RM="rm -f"
+
+OUTTEX="$PROJECT$SUFFIX.tex"
+OUTDVI="$PROJECT$SUFFIX.dvi"
+TEXFILE="$PROJECT.tex"
+DVIFILE="$PROJECT.dvi"
+PSFILE="$PROJECT.ps"
+PS2FILE="$PROJECT.2.ps"
+
+echo $OUTTEX
+
+$RM $PSFILE $PS2FILE $OUTDVI $PROJECT$SUFFIX.aux 2> /dev/null
+
+$BIBLIO -v $VLEVEL -o $OUTTEX -d $REFS -f $FORMATS -a $ABBR --movepoint --nobibitem --uselist $TEXFILE
+# $BIBLIO -v $VLEVEL -o $OUTTEX -d $REFS -f $FORMATS -a $ABBR $TEXFILE
+$LATEX $OUTTEX
+$LATEX $OUTTEX
+
+if [ -e $OUTDVI ]
+then
+ mv $OUTDVI $DVIFILE
+else
+ echo File $OUTDVI not found!!!
+fi
+
+if [ -e $DVIFILE ]
+then
+ echo MAKING POSTSCRIPT
+ touch $DVIFILE
+ $DVIPS -o $PSFILE $DVIFILE
+ $PSTOPS "2:0L@.7(21cm,0)+1L@.7(21cm,14.85cm)" $PSFILE $PS2FILE
+else
+ echo NO DVI FILE FOUND
+fi
+
+$RM *.log *~ 2> /dev/null
diff --git a/support/biblio/EXAMPLES/hairy/refers.db b/support/biblio/EXAMPLES/hairy/refers.db
new file mode 100644
index 0000000000..509a339644
--- /dev/null
+++ b/support/biblio/EXAMPLES/hairy/refers.db
@@ -0,0 +1,1948 @@
+%LABEL = SuccesvolSolliciteren
+%TYPE = book
+%AUTHORP =
+%AUTHORL = Wams
+%AUTHORF = Bert
+%TITLE = Succesvol Solliciteren! (Het sollicitatiestandaardwerk voor Nederland. Alles over het gehele sollicitatieproces.)
+%PAGES = 240
+%PUBL = SIWU
+%PLACE = Enschede
+%YEAR = 2001
+%----------
+LABEL = bookKorn
+TYPE = book
+AUTHORL = Korn|Korn
+AUTHORF = G. |Th.
+AUTHORM = A. |M.
+TITLE = Mathematical handbook for scientists and engineers : definitions, theorems, and formulas for reference and review
+PAGES = 1130
+PUBL = McGraw-Hill Book Co
+PLACE = New York
+YEAR = 1968
+----------
+LABEL = bookChaikinLubensky
+TYPE = book
+AUTHORP =
+AUTHORL = Chaikin|Lubensky
+AUTHORF = P.|T.
+AUTHORM = M.|C.
+TITLE = Principles of condensed matter physics
+PAGES = 700
+PUBL = Cambridge Univ. Press
+PLACE = Cambridge
+YEAR = 1995
+----------
+LABEL = bookSpinGlassTheory
+TYPE = book
+AUTHORP =
+AUTHORL = Mezard|Parisi|Virasoro
+AUTHORF = M.|G.|M.
+AUTHORM = | |A.
+TITLE = Spin Glass Theory and Beyond
+PAGES =
+PUBL = World Scientific Publishing Co Pte Ltd
+PLACE = Singapore
+YEAR = 1987
+----------
+LABEL = Brinke4
+TYPE = edbook
+AUTHORP = |ten
+AUTHORL = Ikkala|Brinke
+AUTHORF = O.|G.
+BOOKTITLE= Handbook of Advanced Electronic and Photonic Materials and Devices, Part 8 Conducting Polymers
+AUTHORI =
+AUTHORE = Nalwa
+AUTHORG = Hari
+AUTHORH = Singh
+PAGE = 185
+PUBL = Academic Press
+PLACE =
+YEAR = 2000
+----------
+LABEL = AbeBallauff
+TYPE = edbook
+AUTHORL = Abe|Ballauff
+AUTHORF = A.|M.
+BOOKTITLE= Liquid Crystallinity in Polymers, Chapter 4 The Flory Lattice Model
+%%%: Principles and Fundamental Properties
+AUTHORI =
+AUTHORE = Ciferri
+AUTHORG = A.
+AUTHORH =
+PAGE = 131
+EPAGE = 167
+PUBL = VCH Publishers
+PLACE = New York
+YEAR = 1991
+----------
+LABEL = KhokhlovTBOA
+TYPE = edbook
+AUTHORL = Khokhlov
+AUTHORF = A.
+AUTHORM = R.
+BOOKTITLE= Liquid Crystallinity in Polymers, Chapter 3 Theories Based on the Onsager Approach
+%%%: Principles and Fundamental Properties
+AUTHORI =
+AUTHORE = Ciferri
+AUTHORG = A.
+AUTHORH =
+PAGE = 97
+EPAGE = 129
+PUBL = VCH Publishers
+PLACE = New York
+YEAR = 1991
+----------
+LABEL = bookMcArdle
+TYPE = edbook
+AUTHORL = Warner
+AUTHORF = M
+AUTHORM =
+TITLE =
+BOOKTITLE= Side Chain Liquid Crystal Polymers
+AUTHORI =
+AUTHORE = McArdle
+AUTHORG = C.
+AUTHORH = B.
+PUBL = Blackie
+PLACE = Glasgow and London
+YEAR = 1989
+----------
+LABEL = bookdeGennesLiqCryst
+TYPE = book
+AUTHORP = de
+AUTHORL = Gennes
+AUTHORF = P.-G.
+AUTHORM =
+TITLE = The Physics of Liquid Crystals
+PUBL = Clarendon Press
+PLACE = Oxford
+YEAR = 1974
+----------
+LABEL = bookdeGennesScalingConcepts
+TYPE = book
+AUTHORP = de
+AUTHORL = Gennes
+AUTHORF = P.-G.
+AUTHORM =
+TITLE = Scaling Concepts in Polymer Physics
+PUBL = Cornell University Press
+PLACE = Ithaca
+YEAR = 1985
+----------
+LABEL = bookPlate
+TYPE = book
+AUTHORL = Plate|Shibaev
+AUTHORF = N. |V.
+AUTHORM = A. |P.
+TITLE = Comb-Shaped Polymers and Liquid Crystals
+PUBL = Plenum Press
+PLACE = New York and London
+YEAR = 1987
+----------
+LABEL = GrosKhokh
+TYPE = book
+AUTHORL = Grosberg|Khokhlov
+AUTHORF = A. |A.
+AUTHORM = Yu. |R.
+TITLE = Statistical Physics of \mml
+PUBL = American Institute of Physics
+PLACE = New York
+YEAR = 1994
+----------
+LABEL = Landau
+TYPE = book
+AUTHORL = Landau|Lifshits
+AUTHORF = L |E.
+AUTHORM = D. |M.
+TITLE = Statistical Physics
+PUBL = Pergamon
+PLACE = Oxford
+YEAR = 1980
+----------
+LABEL = bookLipatovNesterov
+TYPE = book
+AUTHORL = Lipatov|Nesterov
+AUTHORF = Y. |A.
+AUTHORM = S. |E.
+TITLE = Thermodynamics of Polymer Blends
+PUBL = Technomic
+PLACE = Lancaster, Basel
+YEAR = 1997
+----------
+LABEL = bookCloizeaux
+TYPE = book
+AUTHORP = des
+AUTHORL = Cloizeaux|Jannink
+AUTHORF = J. |G.
+TITLE = Polymers in Solutions: Their modelling and Structure
+PUBL = Clarendon Press
+PLACE = Oxford
+YEAR = 1990
+----------
+LABEL = LifshitzGrosbergKhokhlov1
+TYPE = article
+AUTHORL = Lifshitz|Grosberg|Khokhlov
+AUTHORF = I. |A. |A.
+AUTHORM = M. |Yu. |R.
+JOURNAL = \rmp
+VOL = 50
+PAGE = 683
+EPAGE = 713
+YEAR = 1978
+TITLE = Some problems of the statistical physics of polymer chains with volume interaction
+URL = RevModPhys_LifshitsGrosbergKhokhlov1978.pdf
+----------
+LABEL = Vasilevskaya
+TYPE = article
+AUTHORP = | | | |ten
+AUTHORL = Vasilevskaya|Klochkov|Khalatur|Khokhlov|Brinke
+AUTHORF = V. |A. |P. |A. |G.
+AUTHORM = V. |A. |G. |R. |
+TITLE = Microphase separation within comb-like copolymer with attractive side-chains: computer simulations
+JOURNAL = \mts
+VOL = 10
+PAGE = 389
+EPAGE = 394
+YEAR = 2001
+URL = vasilevskaya_attractive.pdf
+----------
+LABEL = Helfand1
+TYPE = article
+AUTHORL = Helfand|Wasserman
+AUTHORF = E. |Z.
+AUTHORM = |R.
+TITLE =
+JOURNAL = \mml
+VOL = 9
+PAGE = 879
+YEAR = 1976
+----------
+LABEL = Tsukahara0
+TYPE = edbook
+AUTHORL = Tsukahara
+AUTHORF = Y.
+BOOKTITLE=Macromolecular Design: Concept and Practice
+AUTHORI =
+AUTHORE = Mishra
+AUTHORG = M.
+AUTHORH =
+PAGE = 161
+EPAGE = 227
+PUBL = Polymer Frontiers International Inc.
+PLACE = New York
+YEAR = 1993
+----------
+LABEL = Schmidt
+TYPE = article
+AUTHORL = Tsukahara|Tsutsumi|Yamashita|Shimada
+AUTHORF = Y. |K. |S. |S.
+TITLE =
+JOURNAL = \mml
+VOL = 23
+PAGE = 5201
+YEAR = 1990
+----------
+LABEL = Tsukahara2
+TYPE = article
+AUTHORL = Tsukahara|Mizuno|Segawa|Yamashita
+AUTHORF = Y. |K. |A. |Y.
+TITLE =
+JOURNAL = \mml
+VOL = 22
+PAGE = 1546
+EPAGE = 1552
+YEAR = 1989
+----------
+LABEL = Tsukahara3
+TYPE = article
+AUTHORL = Tsukahara|Tsutsumi|Yamashita
+AUTHORF = Y. |K. |Y.
+TITLE =
+JOURNAL = \mml
+VOL = 22
+PAGE = 2869
+EPAGE = 2871
+YEAR = 1989
+----------
+LABEL = Ballauff
+TYPE = article
+AUTHORL = Ballauff
+AUTHORF = M.
+AUTHORM =
+TITLE =
+JOURNAL = \ang
+VOL = 28
+PAGE = 253
+YEAR = 1989
+----------
+LABEL = Antonietti
+TYPE = article
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+AUTHORM = | |F.
+TITLE = Highly Ordered Materials with Ultra-Low Surface Energies. Polyelectrolyte-Surfactant Complexes with Fluorinated Surfactants
+JOURNAL = \advm
+VOL = 8
+PAGE = 45
+YEAR = 1996
+----------
+LABEL = Thunemann
+TYPE = article
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+AUTHORM = F. |H.
+TITLE = PHYSISORPTION, INTERFACIAL FILMS, MEMBRANES - Self-Assembly of Perfluorodecanoic Acid with Cationic Copolymers: Ultra-Low Energy Surfaces and Mesomorphous Structures
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+VOL = 14
+PAGE = 4898
+EPAGE = 4903
+YEAR = 1998
+----------
+LABEL = Semenov
+TYPE = article
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+PAGE = 733
+YEAR = 1985
+VOL = 61
+----------
+LABEL = LikhtmanSemenov
+TYPE = article
+AUTHORL = Likhtman|Semenov
+AUTHORF = A.|A.
+AUTHORM = E.|N.
+JOURNAL = \mml
+PAGE = 7273
+EPAGE = 7278
+YEAR = 1997
+VOL = 30
+TITLE = Theory of Microphase Separation in Block Copolymer/Homopolymer Mixtures
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+----------
+LABEL = RubinsteinSemenov
+TYPE = article
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+AUTHORF = M.|A.
+AUTHORM = |N.
+JOURNAL = \mml
+PAGE = 1058
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+YEAR = 2001
+VOL = 34
+TITLE = Dynamics of Entangled Solutions of Associating Polymers
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+----------
+LABEL = Floudas
+TYPE = article
+AUTHORL = Floudas|Hadjichristidis|Stamm|Likhtman|Semenov
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+YEAR = 1997
+VOL = 106
+TITLE = Microphase separation in block copolymer-homopolymer blends: Theory and experiment
+URL = JCP03318.pdf
+----------
+LABEL = Leibler
+TYPE = article
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+AUTHORF = L.
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+PAGE = 1602
+YEAR = 1980
+VOL = 13
+----------
+LABEL = FredricksonHelfand
+TYPE = article
+AUTHORL = Fredrickson|Helfand
+AUTHORF = G. |E.
+AUTHORM = H. |
+TITLE =
+JOURNAL = \mml
+PAGE = 697
+YEAR = 1987
+VOL = 87
+----------
+LABEL = Dobrynin1
+TYPE = article
+AUTHORL = Dobrynin|Erukhimovich
+AUTHORF = A.|I.
+AUTHORM = V.|Y.
+TITLE = Computer-aided comparative investigation of architecture influence of block copolymer phase diagrams
+JOURNAL = \mml
+PAGE = 276
+EPAGE = 281
+YEAR = 1993
+VOL = 26
+----------
+LABEL = Cruz1
+TYPE = article
+AUTHORL = Olvera de la Cruz|Sanchez
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+TITLE =
+JOURNAL = \mml
+PAGE = 2501
+YEAR = 1986
+VOL = 19
+----------
+LABEL = Foster1
+TYPE = article
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+JOURNAL = \mml
+PAGE = 3450
+EPAGE = 3462
+YEAR = 1995
+VOL = 28
+TITLE = Macrophase and Microphase Separation in Random Comb Copolymers
+----------
+LABEL = WernerFredrickson
+TYPE = article
+AUTHORL = Werner|Fredrickson
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+AUTHORM = |H.
+TITLE = Architectural Effects on the Stability Limits of $ABS$ Block Copolymers
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+PAGE = 849
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+YEAR = 1997
+VOL = 35
+URL = JPolimSciB_v35p849y1997.pdf
+----------
+LABEL = Nap1
+TYPE = article
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+YEAR = 2001
+VOL = 4
+----------
+LABEL = Brinke1
+TYPE = article
+AUTHORL = Ruokolainen|M\"akinen|Torkkeli|M\"akel\"a|Serimaa|Brinke|Ikkala
+AUTHORP = | | | | |ten |
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+EPAGE = 560
+YEAR = 1998
+VOL = 280
+URL = mika/Brinke1.pdf
+----------
+LABEL = Brinke2
+TYPE = article
+AUTHORP = |de |de | | |ten |
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+PAGE = 117
+EPAGE = 121
+YEAR = 2001
+VOL = 13
+URL = mika/Brinke2.pdf
+----------
+LABEL = Brinke3
+TYPE = article
+AUTHORL = Kosonen|Ruokolainen|Knaapila|Torkkeli|Jokela|Serimaa|Brinke|Bras|Monkman|Ikkala
+AUTHORP = | | | | | |ten
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+PAGE = 8671
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+YEAR = 2000
+VOL = 33
+URL = mika/Brinke3.pdf
+----------
+LABEL = 3dFlex
+TYPE = article
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+PAGE = 3447
+EPAGE = 3452
+YEAR = 2000
+VOL = 33
+URL = mika/3dFlex.pdf
+----------
+LABEL = Birshtein
+TYPE = article
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+VOL = 29
+----------
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+PAGE = 2825
+YEAR = 1993
+VOL = 26
+----------
+LABEL = Rouault1
+TYPE = article
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+PAGE = 2605
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+YEAR = 1996
+VOL = 29
+URL = Rouault1.pdf
+----------
+LABEL = Rouault2
+TYPE = article
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+VOL = 7
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+----------
+LABEL = Mika1
+TYPE = article
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+AUTHORF = M.|O.|G.
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+VOL = 110
+URL = mika/Mika1.pdf
+----------
+LABEL = Mika2
+TYPE = article
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+AUTHORF = M.|A.|O.|G.
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+VOL = 21
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+----------
+LABEL = Mika3
+TYPE = article
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+AUTHORF = M.|A.|I.|O.|G.
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+YEAR = 1999
+VOL = 32
+URL = mika/Mika3.pdf
+----------
+LABEL = Mika4
+TYPE = article
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+----------
+LABEL = 2dComb
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+LABEL = 3dRigid
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+LABEL = FredricksonLiu
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+YEAR = 1994
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+----------
+LABEL = LiuFredrickson
+TYPE = article
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+YEAR = 1993
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+LABEL = RaphaelFredricksonPincus
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+LABEL = RaphaelPincusFredrickson
+TYPE = article
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+LABEL = FredricksonLeibler
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+LABEL = HongChouHuang
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+----------
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+TYPE = article
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+----------
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+TYPE = article
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+----------
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+----------
+LABEL = Wintermantel1
+TYPE = article
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+----------
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+TYPE = article
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+----------
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+----------
+LABEL = GerleRoos
+TYPE = article
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+YEAR = 1999
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+----------
+LABEL = FischerGerleSchmidt
+TYPE = article
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+AUTHORM =
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+----------
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+----------
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+JOURNAL = \mml
+YEAR = 1999
+VOL = 32
+PAGE = 6813
+EPAGE = 6820
+TITLE = Weak Segregation Theory of Microphase Separation in Associating Binary Homopolymer Blends
+URL = ma981518e.pdf
+----------
+LABEL = Dormidontova:PhaseHbondBrush
+TYPE = article
+AUTHORL = Dormidontova|Brinke
+AUTHORF = E. |G.
+AUTHORP = |ten
+JOURNAL = \mml
+YEAR = 1998
+VOL = 31
+PAGE = 2649
+EPAGE = 2660
+TITLE = Phase Behavior of Hydrogen-Bonding Polymer-Oligomer Mixtures
+URL = ma9710904.pdf
+----------
+LABEL = Erukhimovich:Gel
+TYPE = article
+AUTHORL = Erukhimovich
+AUTHORF = I.
+AUTHORM = Ya.
+JOURNAL = \jetp
+YEAR = 1995
+VOL = 81
+PAGE = 553
+EPAGE = 566
+TITLE = Statistical Theory of Sol-Gel Transition in Weak Gels
+URL =
+----------
+LABEL = MB1091
+TYPE = article
+AUTHORL = Matsen|Bates
+AUTHORF = M.|F.
+AUTHORM = W.|S.
+JOURNAL = \mml
+YEAR = 1996
+VOL = 29
+PAGE = 1091
+EPAGE = 1098
+TITLE = Unifying Weak- and Strong-Segregation Block Copolymer Theories
+URL = MB1091.ps
+----------
+LABEL = BF525
+TYPE = article
+AUTHORL = Bates|Fredrickson
+AUTHORF = F.|G.
+AUTHORM = S.|H.
+JOURNAL = \arpc
+YEAR = 1990
+VOL = 41
+PAGE = 525
+EPAGE = 557
+TITLE = Block Copolymer Thermodynamics: Theory And Experiment
+URL = http://physchem.annualreviews.org/1990/
+----------
+LABEL = Flory:MML:11:1138
+TYPE = article
+AUTHORL = Flory
+AUTHORF = P.
+AUTHORM = J.
+JOURNAL = \mml
+YEAR = 1978
+VOL = 11
+PAGE = 1138
+EPAGE =
+TITLE =
+URL =
+----------
+LABEL = 2sorts
+TYPE = article0
+AUTHORL = Stepanyan|Subbotin|Brinke
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+AUTHORP = | |ten
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+%TITLE=Microphase separation within comb-like copolymer with attractive side-chains: computer simulations1
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+EOF \ No newline at end of file