Changeset 301 in ETALON for papers

Timestamp:

Nov 27, 2015, 11:33:04 AM (9 years ago)

Author:

delerue

Message:

FrUa? paper updated

Location:

papers/2015_FrUa

Files:

• model (deleted)
• models (copied) (copied from papers/2015_FrUa/reconstruction)
• models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.aux (modified) (4 diffs)
• models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.bbl (modified) (1 diff)
• models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.blg (modified) (1 diff)
• models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.log (modified) (15 diffs)
• models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.pdf (modified) (previous)
• models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.tex (modified) (8 diffs)
• models/FrenchUkrainianW2015Nov/bibliography.bib (modified) (1 diff)
• reconstruction (added)

papers/2015_FrUa/models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.aux

@@ -1 +1 @@
 \relax 
 \citation{SPRSmithPurcell}
-\citation{FreeElLaser}
+\citation{NIMA_SP_2014}
 \citation{compsprKarlovetsPotylitsyn}
 \citation{sprpwKarlovetsPotylitsyn}
@@ -7 +7 @@
 \citation{sprpwKarlovetsPotylitsyn}
 \citation{trVerzilov}
+\citation{sprpwKarlovetsPotylitsyn}
+\citation{sprpwKarlovetsPotylitsyn}
 \@writefile{toc}{\contentsline {section}{\numberline {1}Introduction}{1}}
 \newlabel{eq:diff_length}{{1}{1}}
-\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Disposition of the grating, detector, bunch and radiation. Flat grating.\relax }}{1}}
-\providecommand*\caption@xref[2]{\@setref\relax\@undefined{#1}}
-\newlabel{fig:geom1}{{1}{1}}
-\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Disposition of the grating, detector and bunch. Grating with inclined strips\relax }}{1}}
-\newlabel{fig:geom2}{{2}{1}}
 \@writefile{toc}{\contentsline {section}{\numberline {2}Models}{1}}
 \citation{sprpwKarlovetsPotylitsyn}
-\citation{sprpwKarlovetsPotylitsyn}
-\citation{sprpwKarlovetsPotylitsyn}
+\@writefile{lof}{\contentsline {figure}{\numberline {1}{\ignorespaces Disposition of the grating, detector, bunch and radiation. Flat grating.\relax }}{2}}
+\providecommand*\caption@xref[2]{\@setref\relax\@undefined{#1}}
+\newlabel{fig:geom1}{{1}{2}}
+\@writefile{lof}{\contentsline {figure}{\numberline {2}{\ignorespaces Disposition of the grating, detector and bunch. Grating with inclined strips\relax }}{2}}
+\newlabel{fig:geom2}{{2}{2}}
 \newlabel{eq:balzing_modifier}{{2}{2}}
 \@writefile{toc}{\contentsline {subsection}{\numberline {2.1}Simplifications of BDR}{2}}
@@ -24 +24 @@
 \@writefile{toc}{\contentsline {subsubsection}{\numberline {2.1.1}Far zone}{2}}
 \newlabel{eq:far_crit}{{5}{2}}
-\@writefile{toc}{\contentsline {subsubsection}{\numberline {2.1.2}Short grating strips}{2}}
-\newlabel{eq:short_crit}{{6}{2}}
+\@writefile{toc}{\contentsline {subsubsection}{\numberline {2.1.2}Short grating strips}{3}}
+\newlabel{eq:short_crit}{{6}{3}}
 \@writefile{toc}{\contentsline {subsection}{\numberline {2.2}Experimental parameters}{3}}
 \@writefile{toc}{\contentsline {subsection}{\numberline {2.3}Comparison of the SC, RDR and BDR}{3}}
-\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces Phi distribution for SPESO(left) and E 203 d=1,5mm(right)\relax }}{3}}
-\newlabel{fig:Phi1}{{3}{3}}
-\bibstyle{phaip}
-\bibdata{bibliography}
-\bibcite{SPRSmithPurcell}{1}
+\@writefile{lof}{\contentsline {figure}{\numberline {3}{\ignorespaces Phi distribution for SPESO(left) and E 203 d=1,5mm(right)\relax }}{4}}
+\newlabel{fig:Phi1}{{3}{4}}
 \@writefile{lof}{\contentsline {figure}{\numberline {4}{\ignorespaces Phi Distribution for E 203 d=250$\mu $m(left) and E 203 d=50$\mu $m(right)\relax }}{4}}
 \newlabel{fig:Phi2}{{4}{4}}
 \@writefile{lof}{\contentsline {figure}{\numberline {5}{\ignorespaces Phi Distribution for E 203 d=50$\mu $m M=30mm(left) and M=120mm(right)\relax }}{4}}
 \newlabel{fig:Phi3}{{5}{4}}
-\@writefile{toc}{\contentsline {section}{\numberline {3}Interference}{4}}
-\bibcite{FreeElLaser}{2}
-\bibcite{compsprKarlovetsPotylitsyn}{3}
-\bibcite{sprpwKarlovetsPotylitsyn}{4}
-\bibcite{trVerzilov}{5}
+\bibstyle{phaip}
+\bibdata{bibliography}
+\@writefile{toc}{\contentsline {section}{\numberline {3}Interference}{5}}
 \@writefile{lof}{\contentsline {figure}{\numberline {6}{\ignorespaces Dependance of the intensity from R\relax }}{5}}
 \newlabel{fig:IntensR}{{6}{5}}
@@ -49 +44 @@
 \newlabel{fig:Colormap}{{8}{5}}
 \@writefile{toc}{\contentsline {section}{\numberline {4}Summary}{5}}
+\bibcite{SPRSmithPurcell}{1}
+\bibcite{NIMA_SP_2014}{2}
+\bibcite{compsprKarlovetsPotylitsyn}{3}
+\bibcite{sprpwKarlovetsPotylitsyn}{4}
+\bibcite{trVerzilov}{5}

papers/2015_FrUa/models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.bbl

@@ -5 +5 @@
 \newblock Phys. Rev. {\bf 92}, 1069 (1953).
 
-\bibitem{FreeElLaser}
-V.~Kumar and K.-J. Kim,
-\newblock Phys. Rev. E {\bf 73}, 026501 (2006).
+\bibitem{NIMA_SP_2014}
+H.~Andrews et~al.,
+\newblock Nuclear Instruments and Methods in Physics Research Section A:
+  Accelerators, Spectrometers, Detectors and Associated Equipment {\bf 740},
+  212  (2014),
+\newblock Proceedings of the first European Advanced Accelerator Concepts
+  Workshop 2013.
 
 \bibitem{compsprKarlovetsPotylitsyn}

papers/2015_FrUa/models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.blg

@@ -1 @@
-This is BibTeX, Version 0.99dThe top-level auxiliary file: FrUkrWshp_SPR_MalovytsNov2015.aux
+This is BibTeX, Version 0.99d (TeX Live 2013)
+Capacity: max_strings=35307, hash_size=35307, hash_prime=30011
+The top-level auxiliary file: FrUkrWshp_SPR_MalovytsNov2015.aux
 The style file: phaip.bst
 Database file #1: bibliography.bib
+You've used 5 entries,
+            1868 wiz_defined-function locations,
+            607 strings with 6256 characters,
+and the built_in function-call counts, 1015 in all, are:
+= -- 72
+> -- 46
+< -- 0
++ -- 15
+- -- 9
+* -- 86
+:= -- 139
+add.period$ -- 5
+call.type$ -- 5
+change.case$ -- 0
+chr.to.int$ -- 0
+cite$ -- 5
+duplicate$ -- 45
+empty$ -- 97
+format.name$ -- 14
+if$ -- 236
+int.to.chr$ -- 0
+int.to.str$ -- 5
+missing$ -- 5
+newline$ -- 24
+num.names$ -- 5
+pop$ -- 10
+preamble$ -- 1
+purify$ -- 0
+quote$ -- 0
+skip$ -- 53
+stack$ -- 0
+substring$ -- 68
+swap$ -- 15
+text.length$ -- 0
+text.prefix$ -- 0
+top$ -- 0
+type$ -- 0
+warning$ -- 0
+while$ -- 10
+width$ -- 6
+write$ -- 39

papers/2015_FrUa/models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.log

@@ -1 @@
-This is pdfTeX, Version 3.1415926-2.5-1.40.14 (MiKTeX 2.9) (preloaded format=pdflatex 2013.12.8)  23 NOV 2015 06:19
+This is pdfTeX, Version 3.1415926-2.5-1.40.14 (TeX Live 2013) (format=pdflatex 2014.5.30)  27 NOV 2015 11:32
 entering extended mode
-**H:/Univer/France/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.tex
-(H:/Univer/France/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.tex
+ restricted \write18 enabled.
+ file:line:error style messages enabled.
+ %&-line parsing enabled.
+**FrUkrWshp_SPR_MalovytsNov2015.tex
+(./FrUkrWshp_SPR_MalovytsNov2015.tex
 LaTeX2e <2011/06/27>
-Babel <v3.8m> and hyphenation patterns for english, afrikaans, ancientgreek, ar
-abic, armenian, assamese, basque, bengali, bokmal, bulgarian, catalan, coptic, 
-croatian, czech, danish, dutch, esperanto, estonian, farsi, finnish, french, ga
-lician, german, german-x-2013-05-26, greek, gujarati, hindi, hungarian, iceland
-ic, indonesian, interlingua, irish, italian, kannada, kurmanji, latin, latvian,
- lithuanian, malayalam, marathi, mongolian, mongolianlmc, monogreek, ngerman, n
-german-x-2013-05-26, nynorsk, oriya, panjabi, pinyin, polish, portuguese, roman
-ian, russian, sanskrit, serbian, slovak, slovenian, spanish, swedish, swissgerm
-an, tamil, telugu, turkish, turkmen, ukenglish, ukrainian, uppersorbian, usengl
-ishmax, welsh, loaded.
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\base\article.cls
+Babel <3.9f> and hyphenation patterns for 78 languages loaded.
+(/usr/local/texlive/2013/texmf-dist/tex/latex/base/article.cls
 Document Class: article 2007/10/19 v1.4h Standard LaTeX document class
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\base\size11.clo
+(/usr/local/texlive/2013/texmf-dist/tex/latex/base/size11.clo
 File: size11.clo 2007/10/19 v1.4h Standard LaTeX file (size option)
 )
@@ -31 +25 @@
 \bibindent=\dimen102
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\amsmath\amsmath.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/amsmath/amsmath.sty
 Package: amsmath 2013/01/14 v2.14 AMS math features
 \@mathmargin=\skip43
 
 For additional information on amsmath, use the `?' option.
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\amsmath\amstext.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/amsmath/amstext.sty
 Package: amstext 2000/06/29 v2.01
 
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\amsmath\amsgen.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/amsmath/amsgen.sty
 File: amsgen.sty 1999/11/30 v2.0
 \@emptytoks=\toks14
 \ex@=\dimen103
 ))
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\amsmath\amsbsy.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/amsmath/amsbsy.sty
 Package: amsbsy 1999/11/29 v1.2d
 \pmbraise@=\dimen104
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\amsmath\amsopn.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/amsmath/amsopn.sty
 Package: amsopn 1999/12/14 v2.01 operator names
 )
@@ -89 +83 @@
 LaTeX Info: Redefining \] on input line 2666.
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\graphics\graphicx.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/graphics/graphicx.sty
 Package: graphicx 1999/02/16 v1.0f Enhanced LaTeX Graphics (DPC,SPQR)
 
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\graphics\keyval.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/graphics/keyval.sty
 Package: keyval 1999/03/16 v1.13 key=value parser (DPC)
 \KV@toks@=\toks19
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\graphics\graphics.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/graphics/graphics.sty
 Package: graphics 2009/02/05 v1.0o Standard LaTeX Graphics (DPC,SPQR)
 
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\graphics\trig.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/graphics/trig.sty
 Package: trig 1999/03/16 v1.09 sin cos tan (DPC)
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\00miktex\graphics.cfg
-File: graphics.cfg 2007/01/18 v1.5 graphics configuration of teTeX/TeXLive
+(/usr/local/texlive/2013/texmf-dist/tex/latex/latexconfig/graphics.cfg
+File: graphics.cfg 2010/04/23 v1.9 graphics configuration of TeX Live
 )
 Package graphics Info: Driver file: pdftex.def on input line 91.
 
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\pdftex-def\pdftex.def
+(/usr/local/texlive/2013/texmf-dist/tex/latex/pdftex-def/pdftex.def
 File: pdftex.def 2011/05/27 v0.06d Graphics/color for pdfTeX
 
-(H:\Programs\Latex\Full_TeX\texmf\tex\generic\oberdiek\infwarerr.sty
+(/usr/local/texlive/2013/texmf-dist/tex/generic/oberdiek/infwarerr.sty
 Package: infwarerr 2010/04/08 v1.3 Providing info/warning/error messages (HO)
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\generic\oberdiek\ltxcmds.sty
+(/usr/local/texlive/2013/texmf-dist/tex/generic/oberdiek/ltxcmds.sty
 Package: ltxcmds 2011/11/09 v1.22 LaTeX kernel commands for general use (HO)
 )
@@ -121 +115 @@
 \Gin@req@width=\dimen113
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\caption\caption.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/caption/caption.sty
 Package: caption 2013/05/02 v3.3-89 Customizing captions (AR)
 
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\caption\caption3.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/caption/caption3.sty
 Package: caption3 2013/05/02 v1.6-88 caption3 kernel (AR)
 Package caption3 Info: TeX engine: e-TeX on input line 57.
@@ -137 +131 @@
 \c@ContinuedFloat=\count100
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\wrapfig\wrapfig.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/wrapfig/wrapfig.sty
 \wrapoverhang=\dimen121
 \WF@size=\dimen122
@@ -145 +139 @@
 Package: wrapfig 2003/01/31  v 3.6
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\float\float.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/float/float.sty
 Package: float 2001/11/08 v1.3d Float enhancements (AL)
 \c@float@type=\count102
@@ -153 +147 @@
 \@floatcapt=\box30
 )
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\graphics\color.sty
+(/usr/local/texlive/2013/texmf-dist/tex/latex/graphics/color.sty
 Package: color 2005/11/14 v1.0j Standard LaTeX Color (DPC)
 
-(H:\Programs\Latex\Full_TeX\texmf\tex\latex\00miktex\color.cfg
+(/usr/local/texlive/2013/texmf-dist/tex/latex/latexconfig/color.cfg
 File: color.cfg 2007/01/18 v1.5 color configuration of teTeX/TeXLive
 )
 Package color Info: Driver file: pdftex.def on input line 130.
 )
-(H:\Univer\France\FrenchUkrainianW2015Nov\FrUkrWshp_SPR_MalovytsNov2015.aux)
+(./FrUkrWshp_SPR_MalovytsNov2015.aux)
+\openout1 = `FrUkrWshp_SPR_MalovytsNov2015.aux'.
+
 LaTeX Font Info:    Checking defaults for OML/cmm/m/it on input line 16.
 LaTeX Font Info:    ... okay on input line 16.
@@ -175 +171 @@
 LaTeX Font Info:    ... okay on input line 16.
 
-(H:\Programs\Latex\Full_TeX\texmf\tex\context\base\supp-pdf.mkii
+(/usr/local/texlive/2013/texmf-dist/tex/context/base/supp-pdf.mkii
 [Loading MPS to PDF converter (version 2006.09.02).]
 \scratchcounter=\count103
@@ -188 +184 @@
 \makeMPintoPDFobject=\count108
 \everyMPtoPDFconversion=\toks24
-)
+) (/usr/local/texlive/2013/texmf-dist/tex/generic/oberdiek/pdftexcmds.sty
+Package: pdftexcmds 2011/11/29 v0.20 Utility functions of pdfTeX for LuaTeX (HO
+)
+
+(/usr/local/texlive/2013/texmf-dist/tex/generic/oberdiek/ifluatex.sty
+Package: ifluatex 2010/03/01 v1.3 Provides the ifluatex switch (HO)
+Package ifluatex Info: LuaTeX not detected.
+)
+(/usr/local/texlive/2013/texmf-dist/tex/generic/oberdiek/ifpdf.sty
+Package: ifpdf 2011/01/30 v2.3 Provides the ifpdf switch (HO)
+Package ifpdf Info: pdfTeX in PDF mode is detected.
+)
+Package pdftexcmds Info: LuaTeX not detected.
+Package pdftexcmds Info: \pdf@primitive is available.
+Package pdftexcmds Info: \pdf@ifprimitive is available.
+Package pdftexcmds Info: \pdfdraftmode found.
+)
+(/usr/local/texlive/2013/texmf-dist/tex/latex/oberdiek/epstopdf-base.sty
+Package: epstopdf-base 2010/02/09 v2.5 Base part for package epstopdf
+
+(/usr/local/texlive/2013/texmf-dist/tex/latex/oberdiek/grfext.sty
+Package: grfext 2010/08/19 v1.1 Manage graphics extensions (HO)
+
+(/usr/local/texlive/2013/texmf-dist/tex/generic/oberdiek/kvdefinekeys.sty
+Package: kvdefinekeys 2011/04/07 v1.3 Define keys (HO)
+))
+(/usr/local/texlive/2013/texmf-dist/tex/latex/oberdiek/kvoptions.sty
+Package: kvoptions 2011/06/30 v3.11 Key value format for package options (HO)
+
+(/usr/local/texlive/2013/texmf-dist/tex/generic/oberdiek/kvsetkeys.sty
+Package: kvsetkeys 2012/04/25 v1.16 Key value parser (HO)
+
+(/usr/local/texlive/2013/texmf-dist/tex/generic/oberdiek/etexcmds.sty
+Package: etexcmds 2011/02/16 v1.5 Avoid name clashes with e-TeX commands (HO)
+Package etexcmds Info: Could not find \expanded.
+(etexcmds)             That can mean that you are not using pdfTeX 1.50 or
+(etexcmds)             that some package has redefined \expanded.
+(etexcmds)             In the latter case, load this package earlier.
+)))
+Package grfext Info: Graphics extension search list:
+(grfext)             [.png,.pdf,.jpg,.mps,.jpeg,.jbig2,.jb2,.PNG,.PDF,.JPG,.JPE
+G,.JBIG2,.JB2,.eps]
+(grfext)             \AppendGraphicsExtensions on input line 452.
+
+(/usr/local/texlive/2013/texmf-dist/tex/latex/latexconfig/epstopdf-sys.cfg
+File: epstopdf-sys.cfg 2010/07/13 v1.3 Configuration of (r)epstopdf for TeX Liv
+e
+))
 Package caption Info: Begin \AtBeginDocument code.
 Package caption Info: float package is loaded.
 Package caption Info: wrapfig package is loaded.
 Package caption Info: End \AtBeginDocument code.
- <geometry1.png, id=1, 738.50906pt x 414.79968pt>
+Missing character: There is no é in font cmr12!
+
+<geometry1.png, id=1, 738.50906pt x 414.79968pt>
 File: geometry1.png Graphic file (type png)
  <use geometry1.png>
-Package pdftex.def Info: geometry1.png used on input line 34.
+Package pdftex.def Info: geometry1.png used on input line 40.
 (pdftex.def)             Requested size: 245.00275pt x 137.61218pt.
 
@@ -202 +247 @@
 File: geometry3.png Graphic file (type png)
  <use geometry3.png>
-Package pdftex.def Info: geometry3.png used on input line 38.
+Package pdftex.def Info: geometry3.png used on input line 44.
 (pdftex.def)             Requested size: 245.00275pt x 115.70741pt.
  [1
 
-{H:/Programs/Latex/Full_TeX/texmf/pdftex/config/pdftex.map} <H:/Univer/France/F
-renchUkrainianW2015Nov/geometry1.png> <H:/Univer/France/FrenchUkrainianW2015Nov
-/geometry3.png>] [2] <SPESO/RDR_SC_full90.png, id=23, 578.16pt x 433.62pt>
+{/usr/local/texlive/2013/texmf-var/fonts/map/pdftex/updmap/pdftex.map}] [2 <./g
+eometry1.png> <./geometry3.png>] <SPESO/RDR_SC_full90.png, id=23, 578.16pt x 43
+3.62pt>
 File: SPESO/RDR_SC_full90.png Graphic file (type png)
 
 <use SPESO/RDR_SC_full90.png>
-Package pdftex.def Info: SPESO/RDR_SC_full90.png used on input line 140.
+Package pdftex.def Info: SPESO/RDR_SC_full90.png used on input line 147.
 (pdftex.def)             Requested size: 237.49924pt x 178.12279pt.
 
@@ -219 +264 @@
 
 <use E_203_d1500/RDR_SC_full90.png>
-Package pdftex.def Info: E_203_d1500/RDR_SC_full90.png used on input line 143.
+Package pdftex.def Info: E_203_d1500/RDR_SC_full90.png used on input line 150.
 (pdftex.def)             Requested size: 237.49924pt x 178.12279pt.
 
@@ -226 +271 @@
 
 <use E_203_d0250/RDR_SC_full90.png>
-Package pdftex.def Info: E_203_d0250/RDR_SC_full90.png used on input line 152.
+Package pdftex.def Info: E_203_d0250/RDR_SC_full90.png used on input line 159.
 (pdftex.def)             Requested size: 237.49924pt x 178.12279pt.
 
@@ -233 +278 @@
 
 <use E_203_d0050/RDR_SC_full90.png>
-Package pdftex.def Info: E_203_d0050/RDR_SC_full90.png used on input line 155.
+Package pdftex.def Info: E_203_d0050/RDR_SC_full90.png used on input line 162.
 (pdftex.def)             Requested size: 237.49924pt x 178.12279pt.
 
@@ -241 +286 @@
 <use E_203_d0050M30/RDR_SC_full90.png>
 Package pdftex.def Info: E_203_d0050M30/RDR_SC_full90.png used on input line 16
-1.
+8.
 (pdftex.def)             Requested size: 237.49924pt x 178.12279pt.
 
@@ -249 +294 @@
 <use E_203_d0050M120/RDR_SC_full90.png>
 Package pdftex.def Info: E_203_d0050M120/RDR_SC_full90.png used on input line 1
-64.
-(pdftex.def)             Requested size: 237.49924pt x 178.12279pt.
- [3 <H:/Univer/France/FrenchUkrainianW2015Nov/SPESO/RDR_SC_full90.png (PNG copy
-)> <H:/Univer/France/FrenchUkrainianW2015Nov/E_203_d1500/RDR_SC_full90.png (PNG
- copy)>]
-<E_203_d0250/far_pre_theta190phi0.png, id=32, 578.16pt x 433.62pt>
+71.
+(pdftex.def)             Requested size: 237.49924pt x 178.12279pt.
+ [3]
+
+LaTeX Warning: Text page 4 contains only floats.
+
+
+Overfull \vbox (1.73834pt too high) has occurred while \output is active []
+
+
+[4 <./SPESO/RDR_SC_full90.png (PNG copy)> <./E_203_d1500/RDR_SC_full90.png (PNG
+ copy)> <./E_203_d0250/RDR_SC_full90.png (PNG copy)> <./E_203_d0050/RDR_SC_full
+90.png (PNG copy)> <./E_203_d0050M30/RDR_SC_full90.png (PNG copy)> <./E_203_d00
+50M120/RDR_SC_full90.png (PNG copy)>]
+<E_203_d0250/far_pre_theta190phi0.png, id=35, 578.16pt x 433.62pt>
 File: E_203_d0250/far_pre_theta190phi0.png Graphic file (type png)
 
 <use E_203_d0250/far_pre_theta190phi0.png>
 Package pdftex.def Info: E_203_d0250/far_pre_theta190phi0.png used on input lin
-e 174.
+e 183.
 (pdftex.def)             Requested size: 165.00092pt x 123.7484pt.
 
-<E_203_d0250/far_pre_theta290phi0.png, id=33, 578.16pt x 433.62pt>
+<E_203_d0250/far_pre_theta290phi0.png, id=36, 578.16pt x 433.62pt>
 File: E_203_d0250/far_pre_theta290phi0.png Graphic file (type png)
 
 <use E_203_d0250/far_pre_theta290phi0.png>
 Package pdftex.def Info: E_203_d0250/far_pre_theta290phi0.png used on input lin
-e 177.
+e 186.
 (pdftex.def)             Requested size: 165.00092pt x 123.7484pt.
 
-<E_203_d0250/far_pre_theta390phi0.png, id=34, 578.16pt x 433.62pt>
+<E_203_d0250/far_pre_theta390phi0.png, id=37, 578.16pt x 433.62pt>
 File: E_203_d0250/far_pre_theta390phi0.png Graphic file (type png)
 
 <use E_203_d0250/far_pre_theta390phi0.png>
 Package pdftex.def Info: E_203_d0250/far_pre_theta390phi0.png used on input lin
-e 180.
+e 189.
 (pdftex.def)             Requested size: 165.00092pt x 123.7484pt.
 
-<Plot4_ZY.png, id=35, 578.16pt x 433.62pt>
+<Plot4_ZY.png, id=38, 578.16pt x 433.62pt>
 File: Plot4_ZY.png Graphic file (type png)
  <use Plot4_ZY.png>
-Package pdftex.def Info: Plot4_ZY.png used on input line 188.
+Package pdftex.def Info: Plot4_ZY.png used on input line 197.
 (pdftex.def)             Requested size: 245.00275pt x 183.74681pt.
 
-<colormapNE_203_d50um3.png, id=37, 7227.0pt x 5058.9pt>
+<colormapNE_203_d50um3.png, id=40, 7227.0pt x 5058.9pt>
 File: colormapNE_203_d50um3.png Graphic file (type png)
 
 <use colormapNE_203_d50um3.png>
-Package pdftex.def Info: colormapNE_203_d50um3.png used on input line 192.
+Package pdftex.def Info: colormapNE_203_d50um3.png used on input line 201.
 (pdftex.def)             Requested size: 245.00275pt x 171.44453pt.
-
-(H:\Univer\France\FrenchUkrainianW2015Nov\FrUkrWshp_SPR_MalovytsNov2015.bbl
-[4 <H:/Univer/France/FrenchUkrainianW2015Nov/E_203_d0250/RDR_SC_full90.png (PNG
- copy)> <H:/Univer/France/FrenchUkrainianW2015Nov/E_203_d0050/RDR_SC_full90.png
- (PNG copy)> <H:/Univer/France/FrenchUkrainianW2015Nov/E_203_d0050M30/RDR_SC_fu
-ll90.png (PNG copy)> <H:/Univer/France/FrenchUkrainianW2015Nov/E_203_d0050M120/
-RDR_SC_full90.png (PNG copy)>]) [5 <H:/Univer/France/FrenchUkrainianW2015Nov/E_
-203_d0250/far_pre_theta190phi0.png (PNG copy)> <H:/Univer/France/FrenchUkrainia
-nW2015Nov/E_203_d0250/far_pre_theta290phi0.png (PNG copy)> <H:/Univer/France/Fr
-enchUkrainianW2015Nov/E_203_d0250/far_pre_theta390phi0.png (PNG copy)> <H:/Univ
-er/France/FrenchUkrainianW2015Nov/Plot4_ZY.png> <H:/Univer/France/FrenchUkraini
-anW2015Nov/colormapNE_203_d50um3.png (PNG copy)>]
-(H:\Univer\France\FrenchUkrainianW2015Nov\FrUkrWshp_SPR_MalovytsNov2015.aux) ) 
+ (./FrUkrWshp_SPR_MalovytsNov2015.bbl [5 <./E_203_d0250/far_pre_theta190phi0.pn
+g (PNG copy)> <./E_203_d0250/far_pre_theta290phi0.png (PNG copy)> <./E_203_d025
+0/far_pre_theta390phi0.png (PNG copy)> <./Plot4_ZY.png> <./colormapNE_203_d50um
+3.png (PNG copy)>]) [6]
+(./FrUkrWshp_SPR_MalovytsNov2015.aux)
+
+LaTeX Warning: Label(s) may have changed. Rerun to get cross-references right.
+
+ ) 
 Here is how much of TeX's memory you used:
- 3014 strings out of 493921
- 45469 string characters out of 3150556
- 106614 words of memory out of 3000000
- 6293 multiletter control sequences out of 15000+200000
- 10055 words of font info for 36 fonts, out of 3000000 for 9000
- 841 hyphenation exceptions out of 8191
- 36i,21n,38p,656b,320s stack positions out of 5000i,500n,10000p,200000b,50000s
-<
-H:/Programs/Latex/Full_TeX/texmf/fonts/type1/public/amsfonts/cm/cmbx10.pfb><H:/
-Programs/Latex/Full_TeX/texmf/fonts/type1/public/amsfonts/cm/cmbx12.pfb><H:/Pro
-grams/Latex/Full_TeX/texmf/fonts/type1/public/amsfonts/cm/cmex10.pfb><H:/Progra
-ms/Latex/Full_TeX/texmf/fonts/type1/public/amsfonts/cm/cmmi10.pfb><H:/Programs/
-Latex/Full_TeX/texmf/fonts/type1/public/amsfonts/cm/cmmi8.pfb><H:/Programs/Late
-x/Full_TeX/texmf/fonts/type1/public/amsfonts/cm/cmr10.pfb><H:/Programs/Latex/Fu
-ll_TeX/texmf/fonts/type1/public/amsfonts/cm/cmr12.pfb><H:/Programs/Latex/Full_T
-eX/texmf/fonts/type1/public/amsfonts/cm/cmr17.pfb><H:/Programs/Latex/Full_TeX/t
-exmf/fonts/type1/public/amsfonts/cm/cmr6.pfb><H:/Programs/Latex/Full_TeX/texmf/
-fonts/type1/public/amsfonts/cm/cmr8.pfb><H:/Programs/Latex/Full_TeX/texmf/fonts
-/type1/public/amsfonts/cm/cmsy10.pfb><H:/Programs/Latex/Full_TeX/texmf/fonts/ty
-pe1/public/amsfonts/cm/cmsy8.pfb><H:/Programs/Latex/Full_TeX/texmf/fonts/type1/
-public/amsfonts/cm/cmti10.pfb>
-Output written on FrUkrWshp_SPR_MalovytsNov2015.pdf (5 pages, 821195 bytes).
+ 3368 strings out of 493315
+ 51761 string characters out of 6137904
+ 118618 words of memory out of 5000000
+ 6777 multiletter control sequences out of 15000+600000
+ 10017 words of font info for 36 fonts, out of 8000000 for 9000
+ 957 hyphenation exceptions out of 8191
+ 38i,21n,38p,625b,320s stack positions out of 5000i,500n,10000p,200000b,80000s
+</usr/local/texlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmbx10.pfb
+></usr/local/texlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmbx12.pfb>
+</usr/local/texlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmex10.pfb><
+/usr/local/texlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmmi10.pfb></
+usr/local/texlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmmi8.pfb></us
+r/local/texlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmr10.pfb></usr/
+local/texlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmr12.pfb></usr/lo
+cal/texlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmr17.pfb></usr/loca
+l/texlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmr6.pfb></usr/local/t
+exlive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmr8.pfb></usr/local/texl
+ive/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmsy10.pfb></usr/local/texli
+ve/2013/texmf-dist/fonts/type1/public/amsfonts/cm/cmsy8.pfb>
+Output written on FrUkrWshp_SPR_MalovytsNov2015.pdf (6 pages, 805361 bytes).
 PDF statistics:
- 85 PDF objects out of 1000 (max. 8388607)
+ 86 PDF objects out of 1000 (max. 8388607)
+ 51 compressed objects within 1 object stream
  0 named destinations out of 1000 (max. 500000)
  66 words of extra memory for PDF output out of 10000 (max. 10000000)

papers/2015_FrUa/models/FrenchUkrainianW2015Nov/FrUkrWshp_SPR_MalovytsNov2015.tex

@@ -16 +16 @@
 \begin{document}
         \title{Comparison of Smith-Purcell radiation models}
-        \author{Maksym Malovytsia}
+        \author{Maksym Malovytsia$^{1,2}$, Nicolas Delerue$^{2}$\\$^{1}$ Kharkiv University\\ $^{2}$ LAL, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, Orsay, France. }
         \renewcommand{\today}{2015}
         \maketitle
+\begin{abstract}
+Smith-Purcell radiation is used in several applications including the measurement of the longitudinal profile of electron bunches. A correct reconstruction of such profile requires a good understanding of the underlaying model. We have compared the two leading models  of Smith-Purcell radiation and shown that they are in good agreement. We have also studied the interference effects that modulate the signal in the near-field zone.
+\end{abstract}
+        
         \section{Introduction}
-        \par Smith-Purcell (SP) radiation \cite{SPRSmithPurcell} has been discovered sixty years ago. This phenomena occurs, when charged particles pass near periodical conductive grating. Wavelength of produced radiation could be determined by a simple equation:
+        \par Smith-Purcell (SP) radiation \cite{SPRSmithPurcell} has been discovered sixty years ago. This phenomena occurs, when charged particles pass near periodical conductive grating. The wavelength of the radiation produced  is given by a simple equation:
         \begin{equation}\label{eq:diff_length}
             \lambda=\frac{d}{n}\left(\frac{1}{\beta}-cos{\theta}\right)
         \end{equation}
-        \textit{Where $ \lambda $ - length of the radiation, $ d $ - period of the grating, $ n $ - order of radiation and $ \theta $ -polar observation angle (see Fig. \ref{fig:geom1})}
-
-        There are several ideas based on SP radiation, such as compact free electron laser \cite{FreeElLaser} and non-invasive bunch profile measurement methods [insert citation].
-
-        Several models \cite{compsprKarlovetsPotylitsyn} of SP radiation intensity distribution were proposed. Though there are experiment [insert citation] for each of these models, that agrees with theory, it has been pointed out in \cite{sprpwKarlovetsPotylitsyn} that there should be interference effects that affects predicted intensities.
+        Where $ \lambda $ is the wavelength of the radiation, $ d $ is the period of the grating, $ n $ is the order of the radiation and $ \theta $ is the polar observation angle (see Fig. \ref{fig:geom1}).
+
+        There are several ideas of applications based on SP radiation, including non-invasive bunch profile measurement methods \cite{NIMA_SP_2014}.
+
+        Several models \cite{compsprKarlovetsPotylitsyn} of SP radiation intensity distribution were proposed. Though there are experiment  for each of these models, that agrees with these theory a comparison of these models is important to discriminate them experimentally.
+        
+        It has also been shown in \cite{sprpwKarlovetsPotylitsyn} that the predicted intensities should be affected by interference effects.
 
     \begin{figure}[!htb]
@@ -52 +58 @@
     \section{Models}
 
-        Surface Current (SC) and Resonant Diffraction Radiation (RDR) models presented in \cite{compsprKarlovetsPotylitsyn} as a semi-analytical equations, which could be easily calculated, so they are likely to be used in the SP radiation simulations. But those expressions are achieved with assumptions that detector is infinitely far from the source of radiation and grating strips have infinite length.
-
-        Karlovets and Poptylitsyn in their work \cite{sprpwKarlovetsPotylitsyn} proposed more basic model of SP radiation. The idea was to use Backward~Diffraction~Radiation~(BDR), described in \cite{trVerzilov}, and calculate intensity on the detector point as interference of the waves from each point of the grating. Using this approach automatically includes grating sizes and source-detector distance. The problem of using this method is long computation time, as the equations for intensity of SP radiation are expressed through double integrals.
+        The Surface Current (SC) and Resonant Diffraction Radiation (RDR) models are presented in \cite{compsprKarlovetsPotylitsyn} as a semi-analytical equations, which could be easily calculated, so they are easy to use in the SP radiation simulations. However those expressions are achieved with the assumption that the detector is infinitely far from the source of radiation and grating strips have infinite length.
+
+        Karlovets and Poptylitsyn in their work \cite{sprpwKarlovetsPotylitsyn} proposed a basic model of SP radiation. The idea was to use Backward~Diffraction~Radiation~(BDR), described in \cite{trVerzilov}, and calculate the intensity on the detector point as interference of the waves from each point of the grating. Using this approach automatically includes grating sizes and source-detector distance. The problem of using this method is long computation time, as the equations for intensity of SP radiation are expressed through double integrals.
 
         It is also must be mentioned that, unlike SC and RDR models, BDR model proposed in \cite{sprpwKarlovetsPotylitsyn} does not include blaze angle $\theta_0$ (see Fig. \ref{fig:geom2}). It could be easily done, by changing every term of the Eq.~8 in \cite{sprpwKarlovetsPotylitsyn}, that represents beam-grating separation, by variable that depends on the position over the grating. For example:
@@ -102 +108 @@
                                  \end{split}    
                         \end{equation}
+                        
         \subsubsection{Far zone}
-            Far zone is reference to the range of distances between the source and the detector at which interference effects are not visible, alternatively it could be said, that it is distances at which we see our grating as single point of radiation. Criterion of far zone is obtained by Karlovets and Potylitsyn in \cite{sprpwKarlovetsPotylitsyn}:
+            The far zone is the range of distances between the source and the detector at which interference effects are not visible, alternatively it could be said, that it is distances at which we see our grating as single point of radiation. Criterion for the far zone has been obtained by Karlovets and Potylitsyn in \cite{sprpwKarlovetsPotylitsyn}:
             \begin{equation}\label{eq:far_crit}
                 R_0 \gg N^2 d (1+\cos{\theta})
@@ -110 +117 @@
             Using this approximations it is easy to transform Eq.~(\ref{eq:full_model}) into two separated single integrals, which will significantly decrease computation time.
         \subsubsection{Short grating strips}
-            It could happen, that our's detector is closer than given far zone criterion Eq.~(\ref{eq:far_crit}). In that case smaller parameter could be used such as strip width "a". It is simple to calculate criterion for this case, it will be:
+        When the detector is closer that the far zone limit different assumption are possible if the following condition is met:
             \begin{equation}\label{eq:short_crit}
                 R_0 \gg \frac{d}{4(1-\cos{\theta})}
@@ -117 +124 @@
 
     \subsection{Experimental parameters}
-        As initial data for simulation it was decided to use real experiments, as it would be possible to compare theory with experiment later. The experiments are SPESO at Soleil synchrotron and E 203 at SLAC. For convenience the initial parameters are presented in the table below.
+        As parameters for our simulations it was decided to use real experiments, as it would be possible to compare theory with experiment later. The experiments are SPESO at Soleil Synchrotron and E-203 at SLAC. For convenience the initial parameters are presented in the table below.
     \begin{center}
         \begin{tabular}{|l|c|c|c|c|}
         \hline
         % after \\: \hline or \cline{col1-col2} \cline{col3-col4} ...
-        Parameter/Experiment & SPESO & E 203 & E 203 & E 203 \\ \hline
+        Parameter/Experiment & SPESO & E-203 & E-203 & E-203 \\ \hline
         $\gamma$           & 200 & 40000 & 40000 & 40000 \\
         $d, \mu m$         & 10000 & 1500 & 250 & 50 \\
@@ -167 +174 @@
     \end{figure}
 
+As one can see on Fig.~\ref{fig:Phi2} and Fig.~\ref{fig:Phi3} the RDR and SC models produce the same angular distribute and the signal intensity are comparable (within experimental uncertainties). It would there fore be difficult to discriminate experimentally between  these models.
+
     \section{Interference}
-    In far zone models intensity is inverse proportional to the square of distance between source and observer. Picture changes when observer go closer to the source and use full model for BDR. As can be seen at the Fig. \ref{fig:IntensR} Intensity per solid angle is constant at big distances and begins to oscillate at small distances. This means that interference at near source distances depends not only on the angles, but on distance also. And as shown on the \ref{fig:IntensR} interference effect is considerable.
+    In far zone models the signal intensity is inversely proportional to the square of  the distance between the source and the detector. This changes when is closer closer to the source and one must then use the full model for BDR. As can be seen on Fig. \ref{fig:IntensR} the intensity per solid angle is constant at big distances and begins to oscillate at small distances. This means that the interference at near source distances depends not only on the angles, but on the distance also. And as shown on the \ref{fig:IntensR} the interference effect can be considerable.
     
     \begin{figure}[!htb]
@@ -183 +192 @@
     \end{figure}
     
-     It is important to know if we should consider interference effects in our calculations or no, for this we have criterion for determining if we are in the far zone or not is \ref{eq:far_crit}. For easier understanding it could be visualized as curve in the two dimensional plot Fig. \ref{fig:FarPlot}, where ZY plane is $X_T$$Z_T$ on Fig. \ref{fig:geom1}.
+     It is important to know if we should consider interference effects in our calculations or not, for this we have criterion for determining if we are in the far zone or not is Eq. \ref{eq:far_crit}. For easier understanding it could be visualized as curve in the two dimensional plot shown on  Fig. \ref{fig:FarPlot}, where ZY plane is $X_T$$Z_T$ on Fig. \ref{fig:geom1}.
         \begin{figure}[!htb]
         \minipage{0.49\textwidth}
@@ -196 +205 @@
     \end{figure}
     \section{Summary}
+    We have studied two important effect that can change the intensity of the Smith-Purcell Radiation and could thus affect its usability as a longitudinal profile monitor.
+    We have compared the two leading models under experimental conditions and shown that it would not be possible to discriminate them experimentally. We have also shown that interferences in the near field zone have a significant effect and must be taken into account to estimate the correct intensity of SPR.
     
         \bibliographystyle{phaip}

papers/2015_FrUa/models/FrenchUkrainianW2015Nov/bibliography.bib

@@ -263 +263 @@
   doi = {10.1103/PhysRevE.73.026501},
   url = {http://link.aps.org/doi/10.1103/PhysRevE.73.026501}
-}
+ }
+  
+  @article{NIMA_SP_2014,
+        Author = {H.L. Andrews and F. Bakkali Taheri and J. Barros and R. Bartolini and L. Cassinari and C. Clarke and S. Le Corre and N. Delerue and G. Doucas and N. Fuster-Martinez and I. Konoplev and M. Labat and C. Perry and A. Reichold and S. Stevenson and M. Vieille Grosjean},
+        Date-Added = {2014-10-10 01:03:36 +0000},
+        Date-Modified = {2014-10-10 01:03:52 +0000},
+        Doi = {http://dx.doi.org/10.1016/j.nima.2013.11.090},
+        Issn = {0168-9002},
+        Journal = {Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment},
+        Keywords = {Synchrotron \{SOLEIL\}},
+        Note = {Proceedings of the first European Advanced Accelerator Concepts Workshop 2013},
+        Number = {0},
+        Pages = {212 - 215},
+        Title = {Longitudinal profile monitors using Coherent Smith--Purcell radiation},
+        Url = {http://www.sciencedirect.com/science/article/pii/S0168900213016550},
+        Volume = {740},
+        Year = {2014},
+        Bdsk-Url-1 = {http://www.sciencedirect.com/science/article/pii/S0168900213016550},
+        Bdsk-Url-2 = {http://dx.doi.org/10.1016/j.nima.2013.11.090}}
+
+