X-Git-Url: https://git.lyx.org/gitweb/?a=blobdiff_plain;f=lib%2Fexamples%2Faas_sample.lyx;h=042fe8c043b261a5811653a096f120f7222ab330;hb=47b8ab14db71c6932ba5a8f159fc71a745792aca;hp=c77b86e9ad2fb1fc5c857b8f0a48205a0262a982;hpb=41d309b6fb7a397e611f3aa16597ca92c70aa03c;p=lyx.git diff --git a/lib/examples/aas_sample.lyx b/lib/examples/aas_sample.lyx index c77b86e9ad..042fe8c043 100644 --- a/lib/examples/aas_sample.lyx +++ b/lib/examples/aas_sample.lyx @@ -1,5 +1,5 @@ -#LyX 1.5.0svn created this file. For more info see http://www.lyx.org/ -\lyxformat 245 +#LyX 2.0 created this file. For more info see http://www.lyx.org/ +\lyxformat 413 \begin_document \begin_header \textclass aastex @@ -10,62 +10,87 @@ \shorttitle{Djorgovski et al.} \shortauthors{Collapsed Cores in Globular Clusters} \end_preamble +\use_default_options false +\maintain_unincluded_children false \language english +\language_package default \inputencoding default -\fontscheme default +\fontencoding global +\font_roman default +\font_sans default +\font_typewriter default +\font_default_family default +\use_non_tex_fonts false +\font_sc false +\font_osf false +\font_sf_scale 100 +\font_tt_scale 100 + \graphics default +\default_output_format default +\output_sync 0 +\bibtex_command default +\index_command default \paperfontsize default \spacing single +\use_hyperref false \papersize default \use_geometry false \use_amsmath 0 +\use_esint 0 +\use_mhchem 1 +\use_mathdots 1 \cite_engine basic \use_bibtopic false +\use_indices false \paperorientation portrait +\suppress_date false +\use_refstyle 0 +\index Index +\shortcut idx +\color #008000 +\end_index \secnumdepth 3 \tocdepth 3 \paragraph_separation indent -\defskip medskip +\paragraph_indentation default \quotes_language english \papercolumns 1 \papersides 1 \paperpagestyle default \tracking_changes false -\output_changes true +\output_changes false +\html_math_output 0 +\html_css_as_file 0 +\html_be_strict false \end_header \begin_body \begin_layout Title - -Collapsed Cores in Globular Clusters, Gauge-Boson Couplings, and AASTeX -Examples +Collapsed Cores in Globular Clusters, Gauge-Boson Couplings, and AASTeX + Examples \end_layout \begin_layout Author - S. Djorgovski -\begin_inset ERT -status collapsed - -\begin_layout Standard +\begin_inset Flex altaffilmark +status open -\backslash -altaffilmark{1,2,3} +\begin_layout Plain Layout +1,2,3 \end_layout \end_inset and Ivan R. King -\begin_inset ERT +\begin_inset Flex altaffilmark status collapsed -\begin_layout Standard - -\backslash -altaffilmark{1} +\begin_layout Plain Layout +1 \end_layout \end_inset @@ -74,22 +99,18 @@ altaffilmark{1} \end_layout \begin_layout Affiliation - Astronomy Department, University of California, Berkeley, CA 94720 \end_layout \begin_layout Author - C. D. Biemesderfer -\begin_inset ERT +\begin_inset Flex altaffilmark status collapsed -\begin_layout Standard - -\backslash -altaffilmark{4,5} +\begin_layout Plain Layout +4,5 \end_layout \end_inset @@ -98,12 +119,10 @@ altaffilmark{4,5} \end_layout \begin_layout Affiliation - National Optical Astronomy Observatories, Tucson, AZ 85719 \end_layout \begin_layout Email - aastex-help@aas.org \end_layout @@ -112,17 +131,14 @@ aastex-help@aas.org \end_layout \begin_layout Author - R. J. Hanisch -\begin_inset ERT +\begin_inset Flex altaffilmark status collapsed -\begin_layout Standard - -\backslash -altaffilmark{5} +\begin_layout Plain Layout +5 \end_layout \end_inset @@ -131,74 +147,91 @@ altaffilmark{5} \end_layout \begin_layout Affiliation - Space Telescope Science Institute, Baltimore, MD 21218 \end_layout -\begin_layout Standard - - +\begin_layout Altaffilation +1 \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout -\backslash -altaffiltext{1}{Visiting Astronomer, Cerro Tololo Inter-American Observatory. - CTIO is operated by AURA, Inc. -\backslash - under contract to the National Science Foundation.} +}{ \end_layout -\begin_layout Standard +\end_inset +Visiting Astronomer, Cerro Tololo Inter-American Observatory. + CTIO is operated by AURA, Inc. +\begin_inset space \space{} +\end_inset + +under contract to the National Science Foundation. \end_layout -\begin_layout Standard +\begin_layout Altaffilation +2 +\begin_inset ERT +status collapsed -\backslash -altaffiltext{2}{Society of Fellows, Harvard University.} +\begin_layout Plain Layout + +}{ \end_layout -\begin_layout Standard +\end_inset +Society of Fellows, Harvard University. \end_layout -\begin_layout Standard +\begin_layout Altaffilation +3 +\begin_inset ERT +status collapsed -\backslash -altaffiltext{3}{present address: Center for Astrophysics, 60 Garden Street, - Cambridge, MA 02138} +\begin_layout Plain Layout + +}{ \end_layout -\begin_layout Standard +\end_inset +present address: Center for Astrophysics, 60 Garden Street, Cambridge, MA + 02138 \end_layout -\begin_layout Standard +\begin_layout Altaffilation +4 +\begin_inset ERT +status collapsed -\backslash -altaffiltext{4}{Visiting Programmer, Space Telescope Science Institute} - +\begin_layout Plain Layout + +}{ \end_layout -\begin_layout Standard +\end_inset +Visiting Programmer, Space Telescope Science Institute \end_layout -\begin_layout Standard +\begin_layout Altaffilation +5 +\begin_inset ERT +status collapsed -\backslash -altaffiltext{5}{Patron, Alonso's Bar and Grill} +\begin_layout Plain Layout + +}{ \end_layout \end_inset - +Patron, Alonso's Bar and Grill \end_layout \begin_layout Abstract - This is a preliminary report on surface photometry of the major fraction of known globular clusters, to see which of them show the signs of a collapsed core. @@ -207,23 +240,21 @@ This is a preliminary report on surface photometry of the major fraction \end_layout \begin_layout Keywords - clusters: globular, peanut---bosons: bozos \end_layout \begin_layout Section - Introduction \end_layout \begin_layout Standard - A focal problem today in the dynamics of globular clusters is core collapse. It has been predicted by theory for decades \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash citep{hen61,lyn68,spi85} @@ -236,7 +267,8 @@ citep{hen61,lyn68,spi85} \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash citep{kin75,new78} @@ -249,7 +281,8 @@ citep{kin75,new78} \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash citet{aur82} @@ -262,7 +295,8 @@ citet{aur82} \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash citep[Paper I]{djo84} @@ -275,7 +309,8 @@ citep[Paper I]{djo84} \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash citep{can78} @@ -288,56 +323,54 @@ citep{can78} \end_layout \begin_layout Section - Observations \end_layout \begin_layout Standard - All our observations were short direct exposures with CCD's. At Lick Observatory we used a TI 500 -\begin_inset Formula \( \times \) +\begin_inset Formula $\times$ \end_inset 500 chip and a GEC 575 -\begin_inset Formula \( \times \) +\begin_inset Formula $\times$ \end_inset 385, on the 1-m Nickel reflector. The only filter available at Lick was red. At CTIO we used a GEC 575 -\begin_inset Formula \( \times \) +\begin_inset Formula $\times$ \end_inset 385, with -\begin_inset Formula \( B,V, \) +\begin_inset Formula $B,V,$ \end_inset and -\begin_inset Formula \( R \) +\begin_inset Formula $R$ \end_inset filters, and an RCA 512 -\begin_inset Formula \( \times \) +\begin_inset Formula $\times$ \end_inset 320, with -\begin_inset Formula \( U,B,V,R, \) +\begin_inset Formula $U,B,V,R,$ \end_inset and -\begin_inset Formula \( I \) +\begin_inset Formula $I$ \end_inset filters, on the 1.5-m reflector. In the CTIO observations we tried to concentrate on the shortest practicable wavelengths; but faintness, reddening, and poor short-wavelength sensitivity often kept us from observing in -\begin_inset Formula \( U \) +\begin_inset Formula $U$ \end_inset or even in -\begin_inset Formula \( B \) +\begin_inset Formula $B$ \end_inset . @@ -346,7 +379,6 @@ All our observations were short direct exposures with CCD's. \end_layout \begin_layout Standard - The CCD images are unfortunately not always suitable, for very poor clusters or for clusters with large cores. Since the latter are easily studied by other means, we augmented our own @@ -355,7 +387,8 @@ The CCD images are unfortunately not always suitable, for very poor clusters \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash citep{kin68,pet76,har84,ort85} @@ -367,7 +400,8 @@ citep{kin68,pet76,har84,ort85} \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash citep{kin66,kin75} @@ -379,7 +413,8 @@ citep{kin66,kin75} \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash citep{kro84} @@ -392,19 +427,16 @@ citep{kro84} \end_layout \begin_layout Section - Helicity Amplitudes \end_layout \begin_layout Standard - It has been realized that helicity amplitudes provide a convenient means for Feynman diagram \begin_inset Foot status collapsed -\begin_layout Standard - +\begin_layout Plain Layout Footnotes can be inserted like this. \end_layout @@ -416,7 +448,9 @@ Footnotes can be inserted like this. amplitude squared becomes unwieldy. Our calculations use the helicity techniques developed by other authors -\begin_inset LatexCommand \cite{hag86} +\begin_inset CommandInset citation +LatexCommand cite +key "hag86" \end_inset @@ -424,14 +458,13 @@ Footnotes can be inserted like this. \end_layout \begin_layout Subsection - Formalism \end_layout \begin_layout Standard - - -\begin_inset LatexCommand \label{bozomath} +\begin_inset CommandInset label +LatexCommand label +name "bozomath" \end_inset @@ -439,49 +472,49 @@ Formalism \end_layout \begin_layout Standard - A tree-level amplitude in -\begin_inset Formula \( e^{+}e^{-} \) +\begin_inset Formula $e^{+}e^{-}$ \end_inset collisions can be expressed in terms of fermion strings of the form -\begin_inset Formula \begin{equation} -\bar{v}(p_{2},\sigma _{2})P_{-\tau }\hat{a}_{1}\hat{a}_{2}\cdots \hat{a}_{n}u(p_{1},\sigma _{1}), +\begin_inset Formula +\begin{equation} +\bar{v}(p_{2},\sigma_{2})P_{-\tau}\hat{a}_{1}\hat{a}_{2}\cdots\hat{a}_{n}u(p_{1},\sigma_{1}), \end{equation} \end_inset where -\begin_inset Formula \( p \) +\begin_inset Formula $p$ \end_inset and -\begin_inset Formula \( \sigma \) +\begin_inset Formula $\sigma$ \end_inset label the initial -\begin_inset Formula \( e^{\pm } \) +\begin_inset Formula $e^{\pm}$ \end_inset four-momenta and helicities -\begin_inset Formula \( (\sigma =\pm 1) \) +\begin_inset Formula $(\sigma=\pm1)$ \end_inset , -\begin_inset Formula \( \hat{a}_{i}=a^{\mu }_{i}\gamma _{\nu } \) +\begin_inset Formula $\hat{a}_{i}=a_{i}^{\mu}\gamma_{\nu}$ \end_inset and -\begin_inset Formula \( P_{\tau }=\frac{1}{2}(1+\tau \gamma _{5}) \) +\begin_inset Formula $P_{\tau}=\frac{1}{2}(1+\tau\gamma_{5})$ \end_inset is a chirality projection operator -\begin_inset Formula \( (\tau =\pm1 ) \) +\begin_inset Formula $(\tau=\pm1)$ \end_inset . The -\begin_inset Formula \( a^{\mu }_{i} \) +\begin_inset Formula $a_{i}^{\mu}$ \end_inset may be formed from particle four-momenta, gauge-boson polarization vectors @@ -490,54 +523,55 @@ te fermions. \end_layout \begin_layout NoteToEditor - Figures 1 and 2 should appear side-by-side in print \end_layout \begin_layout Standard - In the chiral representation the -\begin_inset Formula \( \gamma \) +\begin_inset Formula $\gamma$ \end_inset matrices are expressed in terms of -\begin_inset Formula \( 2\times 2 \) +\begin_inset Formula $2\times2$ \end_inset Pauli matrices -\begin_inset Formula \( \sigma \) +\begin_inset Formula $\sigma$ \end_inset and the unit matrix 1 as -\begin_inset Formula \begin{eqnarray} -\gamma ^{\mu } & = & \left( \begin{array}{cc} -0 & \sigma ^{\mu }_{+}\\ -\sigma ^{\mu }_{-} & 0 -\end{array}\right) ,\gamma ^{5}=\left( \begin{array}{cc} +\begin_inset Formula +\begin{eqnarray*} +\gamma^{\mu} & = & \left(\begin{array}{cc} +0 & \sigma_{+}^{\mu}\\ +\sigma_{-}^{\mu} & 0 +\end{array}\right),\gamma^{5}=\left(\begin{array}{cc} -1 & 0\\ 0 & 1 -\end{array}\right) ,\nonumber \\ -\sigma ^{\mu }_{\pm } & = & ({\textbf {1}},\pm \sigma ),\nonumber -\end{eqnarray} +\end{array}\right),\\ +\sigma_{\pm}^{\mu} & = & ({\textbf{1}},\pm\sigma), +\end{eqnarray*} \end_inset giving -\begin_inset Formula \begin{equation} -\hat{a}=\left( \begin{array}{cc} +\begin_inset Formula +\begin{equation} +\hat{a}=\left(\begin{array}{cc} 0 & (\hat{a})_{+}\\ (\hat{a})_{-} & 0 -\end{array}\right) ,(\hat{a})_{\pm }=a_{\mu }\sigma ^{\mu }_{\pm }, +\end{array}\right),(\hat{a})_{\pm}=a_{\mu}\sigma_{\pm}^{\mu}, \end{equation} \end_inset The spinors are expressed in terms of two-component Weyl spinors as -\begin_inset Formula \begin{equation} -u=\left( \begin{array}{c} +\begin_inset Formula +\begin{equation} +u=\left(\begin{array}{c} (u)_{-}\\ (u)_{+} -\end{array}\right) ,v={\textbf {(}}\vdag _{+}{\textbf {,}}\vdag _{-}{\textbf {)}}. +\end{array}\right),v={\textbf{(}}\vdag_{+}{\textbf{,}}\vdag_{-}{\textbf{)}}. \end{equation} \end_inset @@ -546,24 +580,22 @@ u=\left( \begin{array}{c} \end_layout \begin_layout Standard - The Weyl spinors are given in terms of helicity eigenstates -\begin_inset Formula \( \chi _{\lambda }(p) \) +\begin_inset Formula $\chi_{\lambda}(p)$ \end_inset with -\begin_inset Formula \( \lambda =\pm1 \) +\begin_inset Formula $\lambda=\pm1$ \end_inset by \end_layout \begin_layout MathLetters - - -\begin_inset Formula \begin{eqnarray} -u(p,\lambda )_{\pm } & = & (E\pm \lambda |{\textbf {p}}|)^{1/2}\chi _{\lambda }(p),\\ -v(p,\lambda )_{\pm } & = & \pm \lambda (E\mp \lambda |{\textbf {p}}|)^{1/2}\chi _{-\lambda }(p) +\begin_inset Formula +\begin{eqnarray} +u(p,\lambda)_{\pm} & = & (E\pm\lambda|{\textbf{p}}|)^{1/2}\chi_{\lambda}(p),\\ +v(p,\lambda)_{\pm} & = & \pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi_{-\lambda}(p) \end{eqnarray} \end_inset @@ -572,49 +604,52 @@ v(p,\lambda )_{\pm } & = & \pm \lambda (E\mp \lambda |{\textbf {p}}|)^{1/2}\chi \end_layout \begin_layout Section - Floating material and so forth \end_layout \begin_layout Standard - Consider a task that computes profile parameters for a modified Lorentzian of the form -\begin_inset Formula \begin{equation} +\begin_inset Formula +\begin{equation} I=\frac{1}{1+d_{1}^{P(1+d_{2})}} \end{equation} \end_inset where -\begin_inset Formula \[ -d_{1}=\sqrt{\left( \begin{array}{c} -\frac{x_{1}}{R_{maj}} -\end{array}\right) ^{2}+\left( \begin{array}{c} -\frac{y_{1}}{R_{min}} -\end{array}\right) ^{2}}\] +\begin_inset Formula +\[ +d_{1}=\sqrt{\left(\begin{array}{c} +\frac{x_{1}}{R_{maj}}\end{array}\right)^{2}+\left(\begin{array}{c} +\frac{y_{1}}{R_{min}}\end{array}\right)^{2}} +\] \end_inset -\begin_inset Formula \[ -d_{2}=\sqrt{\left( \begin{array}{c} -\frac{x_{1}}{PR_{maj}} -\end{array}\right) ^{2}+\left( \begin{array}{c} -\case {y_{1}}{PR_{min}} -\end{array}\right) ^{2}}\] +\begin_inset Formula +\[ +d_{2}=\sqrt{\left(\begin{array}{c} +\frac{x_{1}}{PR_{maj}}\end{array}\right)^{2}+\left(\begin{array}{c} +\case{y_{1}}{PR_{min}}\end{array}\right)^{2}} +\] \end_inset -\begin_inset Formula \[ -x_{1}=(x-x_{0})\cos \Theta +(y-y_{0})\sin \Theta \] +\begin_inset Formula +\[ +x_{1}=(x-x_{0})\cos\Theta+(y-y_{0})\sin\Theta +\] \end_inset -\begin_inset Formula \[ -y_{1}=-(x-x_{0})\sin \Theta +(y-y_{0})\cos \Theta \] +\begin_inset Formula +\[ +y_{1}=-(x-x_{0})\sin\Theta+(y-y_{0})\cos\Theta +\] \end_inset @@ -622,56 +657,48 @@ y_{1}=-(x-x_{0})\sin \Theta +(y-y_{0})\cos \Theta \] \end_layout \begin_layout Standard - In these expressions -\begin_inset Formula \( x_{0} \) +\begin_inset Formula $x_{0}$ \end_inset , -\begin_inset Formula \( y_{0} \) +\begin_inset Formula $y_{0}$ \end_inset is the star center, and -\begin_inset Formula \( \Theta \) +\begin_inset Formula $\Theta$ \end_inset is the angle with the -\begin_inset Formula \( x \) +\begin_inset Formula $x$ \end_inset axis. - Results of this task are shown in table\InsetSpace ~ + Results of this task are shown in table +\begin_inset space ~ +\end_inset -\begin_inset LatexCommand \ref{tbl-2} + +\begin_inset CommandInset ref +LatexCommand ref +reference "tbl-2" \end_inset . It is not clear how these sorts of analyses may affect determination of -\begin_inset Formula \( M_{\sun } \) -\end_inset - -, but the assumption is that the alternate results should be less than 90 -\begin_inset ERT -status collapsed - -\begin_layout Standard - -\backslash -degr -\backslash - -\end_layout - +\begin_inset Formula $M_{\sun}$ \end_inset -out of phase with previous values. +, but the assumption is that the alternate results should be less than 90° + out of phase with previous values. We have no observations of \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash ion{Ca}{2} @@ -684,7 +711,8 @@ ion{Ca}{2} \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash slantfrac{4}{5} @@ -700,31 +728,40 @@ slantfrac{4}{5} \end_layout \begin_layout Standard - We are grateful to V. Barger, T. Han, and R. J. N. - Phillips for doing the math in section\InsetSpace ~ + Phillips for doing the math in section +\begin_inset space ~ +\end_inset + -\begin_inset LatexCommand \ref{bozomath} +\begin_inset CommandInset ref +LatexCommand ref +reference "bozomath" \end_inset . More information on the AASTeX macros package are available at +\begin_inset Flex URL +status collapsed -\begin_inset LatexCommand \url{http://www.aas.org/publications/aastex} +\begin_layout Plain Layout -\end_inset +http://www.aas.org/publications/aastex +\end_layout +\end_inset or the \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash anchor{ftp://www.aas.org/pubs/}{AAS ftp site} @@ -740,15 +777,14 @@ anchor{ftp://www.aas.org/pubs/}{AAS ftp site} \end_layout \begin_layout Section - Appendicial material \end_layout \begin_layout Standard - Consider once again a task that computes profile parameters for a modified Lorentzian of the form -\begin_inset Formula \begin{equation} +\begin_inset Formula +\begin{equation} I=\frac{1}{1+d_{1}^{P(1+d_{2})}} \end{equation} @@ -758,32 +794,30 @@ I=\frac{1}{1+d_{1}^{P(1+d_{2})}} \end_layout \begin_layout MathLetters - - -\begin_inset Formula \[ -d_{1}=\frac{3}{4}\sqrt{\left( \begin{array}{c} -\frac{x_{1}}{R_{maj}} -\end{array}\right) ^{2}+\left( \begin{array}{c} -\frac{y_{1}}{R_{min}} -\end{array}\right) ^{2}}\] +\begin_inset Formula +\[ +d_{1}=\frac{3}{4}\sqrt{\left(\begin{array}{c} +\frac{x_{1}}{R_{maj}}\end{array}\right)^{2}+\left(\begin{array}{c} +\frac{y_{1}}{R_{min}}\end{array}\right)^{2}} +\] \end_inset -\begin_inset Formula \begin{equation} -d_{2}=\case {3}{4}\sqrt{\left( \begin{array}{c} -\frac{x_{1}}{PR_{maj}} -\end{array}\right) ^{2}+\left( \begin{array}{c} -\case {y_{1}}{PR_{min}} -\end{array}\right) ^{2}} +\begin_inset Formula +\begin{equation} +d_{2}=\case{3}{4}\sqrt{\left(\begin{array}{c} +\frac{x_{1}}{PR_{maj}}\end{array}\right)^{2}+\left(\begin{array}{c} +\case{y_{1}}{PR_{min}}\end{array}\right)^{2}} \end{equation} \end_inset -\begin_inset Formula \begin{eqnarray} -x_{1} & = & (x-x_{0})\cos \Theta +(y-y_{0})\sin \Theta \\ -y_{1} & = & -(x-x_{0})\sin \Theta +(y-y_{0})\cos \Theta +\begin_inset Formula +\begin{eqnarray} +x_{1} & = & (x-x_{0})\cos\Theta+(y-y_{0})\sin\Theta\\ +y_{1} & = & -(x-x_{0})\sin\Theta+(y-y_{0})\cos\Theta \end{eqnarray} \end_inset @@ -792,10 +826,10 @@ y_{1} & = & -(x-x_{0})\sin \Theta +(y-y_{0})\cos \Theta \end_layout \begin_layout Standard - For completeness, here is one last equation. -\begin_inset Formula \begin{equation} +\begin_inset Formula +\begin{equation} e=mc^{2} \end{equation} @@ -805,15 +839,20 @@ e=mc^{2} \end_layout \begin_layout References -\bibitem [Auri\`ere(1982)]{aur82} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Auri\\`ere(1982)" +key "aur82" + +\end_inset -Auri\i \`{e} -re, M. +Aurière, M. 1982, \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash aap @@ -825,7 +864,12 @@ aap \end_layout \begin_layout References -\bibitem [Canizares et al.(1978)]{can78} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Canizares et al.(1978)" +key "can78" + +\end_inset Canizares, C. R., Grindlay, J. @@ -836,7 +880,8 @@ Canizares, C. \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash apj @@ -848,7 +893,12 @@ apj \end_layout \begin_layout References -\bibitem [Djorgovski and King(1984)]{djo84} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Djorgovski and King(1984)" +key "djo84" + +\end_inset Djorgovski, S., and King, I. R. @@ -856,7 +906,8 @@ Djorgovski, S., and King, I. \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash apjl @@ -868,14 +919,24 @@ apjl \end_layout \begin_layout References -\bibitem [Hagiwara and Zeppenfeld(1986)]{hag86} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Hagiwara and Zeppenfeld(1986)" +key "hag86" + +\end_inset Hagiwara, K., and Zeppenfeld, D. 1986, Nucl.Phys., 274, 1 \end_layout \begin_layout References -\bibitem [Harris and van den Bergh(1984)]{har84} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Harris and van den Bergh(1984)" +key "har84" + +\end_inset Harris, W. E., and van den Bergh, S. @@ -883,7 +944,8 @@ Harris, W. \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash aj @@ -895,15 +957,24 @@ aj \end_layout \begin_layout References -\bibitem [H\`enon(1961)]{hen61} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "H\\`enon(1961)" +key "hen61" + +\end_inset -H\i \'{e} -non, M. +Hénon, M. 1961, Ann.d'Ap., 24, 369 \end_layout \begin_layout References -\bibitem [King(1966)]{kin66} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "King(1966)" +key "kin66" + +\end_inset King, I. R. @@ -911,7 +982,8 @@ King, I. \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash aj @@ -923,7 +995,12 @@ aj \end_layout \begin_layout References -\bibitem [King(1975)]{kin75} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "King(1975)" +key "kin75" + +\end_inset King, I. R. @@ -932,7 +1009,12 @@ King, I. \end_layout \begin_layout References -\bibitem [King et al.(1968)]{kin68} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "King et al.(1968)" +key "kin68" + +\end_inset King, I. R., Hedemann, E., Hodge, S. @@ -942,7 +1024,8 @@ King, I. \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash aj @@ -954,7 +1037,12 @@ aj \end_layout \begin_layout References -\bibitem [Kron et al.(1984)]{kro84} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Kron et al.(1984)" +key "kro84" + +\end_inset Kron, G. E., Hewitt, A. @@ -964,7 +1052,8 @@ Kron, G. \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash pasp @@ -976,14 +1065,20 @@ pasp \end_layout \begin_layout References -\bibitem [Lynden-Bell and Wood(1968)]{lyn68} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Lynden-Bell and Wood(1968)" +key "lyn68" + +\end_inset Lynden-Bell, D., and Wood, R. 1968, \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash mnras @@ -995,7 +1090,12 @@ mnras \end_layout \begin_layout References -\bibitem [Newell and O'Neil(1978)]{new78} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Newell and O'Neil(1978)" +key "new78" + +\end_inset Newell, E. B., and O'Neil, E. @@ -1004,7 +1104,8 @@ Newell, E. \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash apjs @@ -1016,14 +1117,20 @@ apjs \end_layout \begin_layout References -\bibitem [Ortolani et al.(1985)]{ort85} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Ortolani et al.(1985)" +key "ort85" + +\end_inset Ortolani, S., Rosino, L., and Sandage, A. 1985, \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash aj @@ -1035,7 +1142,12 @@ aj \end_layout \begin_layout References -\bibitem [Peterson(1976)]{pet76} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Peterson(1976)" +key "pet76" + +\end_inset Peterson, C. J. @@ -1043,7 +1155,8 @@ Peterson, C. \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash aj @@ -1055,7 +1168,12 @@ aj \end_layout \begin_layout References -\bibitem [Spitzer(1985)]{spi85} +\begin_inset CommandInset bibitem +LatexCommand bibitem +label "Spitzer(1985)" +key "spi85" + +\end_inset Spitzer, L. 1985, Dynamics of Star Clusters, J. @@ -1064,26 +1182,16 @@ Spitzer, L. \end_layout \begin_layout Standard - - -\begin_inset ERT -status collapsed - -\begin_layout Standard - -\backslash -clearpage -\end_layout - +\begin_inset Newpage clearpage \end_inset \end_layout \begin_layout FigCaption - - -\begin_inset LatexCommand \label{fig1} +\begin_inset CommandInset label +LatexCommand label +name "fig1" \end_inset @@ -1091,9 +1199,9 @@ This is the first figure and it uses sgi9259.eps as its EPS figure file. \end_layout \begin_layout FigCaption - - -\begin_inset LatexCommand \label{fig2} +\begin_inset CommandInset label +LatexCommand label +name "fig2" \end_inset @@ -1104,9 +1212,9 @@ This is an example of a long figure caption that must be set as a paragraph. \end_layout \begin_layout FigCaption - - -\begin_inset LatexCommand \label{fig3} +\begin_inset CommandInset label +LatexCommand label +name "fig3" \end_inset @@ -1115,55 +1223,49 @@ This figure has no associated EPS file, so the optional parameter is omitted. \end_layout \begin_layout Standard - - -\begin_inset ERT -status collapsed - -\begin_layout Standard - -\backslash -clearpage -\end_layout - +\begin_inset Newpage clearpage \end_inset \end_layout \begin_layout Standard - \begin_inset Float table wide false sideways false status open -\begin_layout Caption +\begin_layout Plain Layout +\begin_inset Caption +\begin_layout Plain Layout Terribly relevant tabular information. -\begin_inset LatexCommand \label{tbl-2} +\begin_inset CommandInset label +LatexCommand label +name "tbl-2" \end_inset \end_layout -\begin_layout Standard - - -\begin_inset VSpace medskip \end_inset \end_layout +\begin_layout Plain Layout +\begin_inset VSpace medskip +\end_inset -\begin_layout Standard +\end_layout -\begin_inset Tabular +\begin_layout Plain Layout +\align center +\begin_inset Tabular - + @@ -1178,33 +1280,30 @@ Terribly relevant tabular information. - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout Star \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout Height \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -\begin_inset Formula \( d_{x} \) +\begin_inset Formula $d_{x}$ \end_inset @@ -1212,13 +1311,12 @@ Star \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -\begin_inset Formula \( d_{y} \) +\begin_inset Formula $d_{y}$ \end_inset @@ -1226,13 +1324,12 @@ Star \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -\begin_inset Formula \( n \) +\begin_inset Formula $n$ \end_inset @@ -1240,13 +1337,12 @@ Star \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -\begin_inset Formula \( \chi ^{2} \) +\begin_inset Formula $\chi^{2}$ \end_inset @@ -1254,13 +1350,12 @@ Star \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -\begin_inset Formula \( R_{maj} \) +\begin_inset Formula $R_{maj}$ \end_inset @@ -1268,13 +1363,12 @@ Star \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -\begin_inset Formula \( R_{min} \) +\begin_inset Formula $R_{min}$ \end_inset @@ -1285,20 +1379,16 @@ Star \begin_inset Text -\begin_layout Standard - - -\begin_inset Formula \( P \) +\begin_layout Plain Layout +\begin_inset Formula $P$ \end_inset -\begin_inset ERT +\begin_inset Flex tablenotemark status collapsed -\begin_layout Standard - -\backslash -tablenotemark{a} +\begin_layout Plain Layout +a \end_layout \end_inset @@ -1308,13 +1398,12 @@ tablenotemark{a} \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -\begin_inset Formula \( PR_{maj} \) +\begin_inset Formula $PR_{maj}$ \end_inset @@ -1322,13 +1411,12 @@ tablenotemark{a} \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -\begin_inset Formula \( PR_{min} \) +\begin_inset Formula $PR_{min}$ \end_inset @@ -1339,20 +1427,16 @@ tablenotemark{a} \begin_inset Text -\begin_layout Standard - - -\begin_inset Formula \( \Theta \) +\begin_layout Plain Layout +\begin_inset Formula $\Theta$ \end_inset -\begin_inset ERT +\begin_inset Flex tablenotemark status collapsed -\begin_layout Standard - -\backslash -tablenotemark{b} +\begin_layout Plain Layout +b \end_layout \end_inset @@ -1365,8 +1449,7 @@ tablenotemark{b} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout Ref. \end_layout @@ -1377,13 +1460,12 @@ Ref. \begin_inset Text -\begin_layout Standard - - +\begin_layout Plain Layout \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + \backslash tableline @@ -1401,8 +1483,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 33472.5 \end_layout @@ -1411,8 +1492,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -0.1 \end_layout @@ -1421,8 +1501,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 0.4 \end_layout @@ -1431,8 +1510,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 53 \end_layout @@ -1441,8 +1519,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 27.4 \end_layout @@ -1451,8 +1528,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 2.065 \end_layout @@ -1461,8 +1537,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1.940 \end_layout @@ -1471,8 +1546,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 3.900 \end_layout @@ -1481,8 +1555,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 68.3 \end_layout @@ -1491,8 +1564,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 116.2 \end_layout @@ -1501,8 +1573,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -27.639 \end_layout @@ -1511,8 +1582,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1,2 \end_layout @@ -1523,8 +1593,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 2 \end_layout @@ -1533,8 +1602,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 27802.4 \end_layout @@ -1543,8 +1611,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -0.3 \end_layout @@ -1553,8 +1620,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -0.2 \end_layout @@ -1563,8 +1629,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 60 \end_layout @@ -1573,8 +1638,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 3.7 \end_layout @@ -1583,8 +1647,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1.628 \end_layout @@ -1593,8 +1656,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1.510 \end_layout @@ -1603,8 +1665,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 2.156 \end_layout @@ -1613,8 +1674,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 6.8 \end_layout @@ -1623,8 +1683,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 7.5 \end_layout @@ -1633,8 +1692,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -26.764 \end_layout @@ -1643,8 +1701,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 3 \end_layout @@ -1655,8 +1712,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 3 \end_layout @@ -1665,8 +1721,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 29210.6 \end_layout @@ -1675,8 +1730,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 0.9 \end_layout @@ -1685,8 +1739,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 0.3 \end_layout @@ -1695,8 +1748,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 60 \end_layout @@ -1705,8 +1757,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 3.4 \end_layout @@ -1715,8 +1766,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1.622 \end_layout @@ -1725,8 +1775,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1.551 \end_layout @@ -1735,8 +1784,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 2.159 \end_layout @@ -1745,8 +1793,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 6.7 \end_layout @@ -1755,8 +1802,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 7.3 \end_layout @@ -1765,8 +1811,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -40.272 \end_layout @@ -1775,8 +1820,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 4 \end_layout @@ -1787,8 +1831,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 4 \end_layout @@ -1797,8 +1840,7 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 32733.8 \end_layout @@ -1807,16 +1849,13 @@ tableline \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -1.2 -\begin_inset ERT -status collapsed - -\begin_layout Standard +\begin_inset Flex tablenotemark +status open -\backslash -tablenotemark{c} +\begin_layout Plain Layout +c \end_layout \end_inset @@ -1829,8 +1868,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -0.5 \end_layout @@ -1839,8 +1877,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 41 \end_layout @@ -1849,8 +1886,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 54.8 \end_layout @@ -1859,8 +1895,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 2.282 \end_layout @@ -1869,8 +1904,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 2.156 \end_layout @@ -1879,8 +1913,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 4.313 \end_layout @@ -1889,8 +1922,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 117.4 \end_layout @@ -1899,8 +1931,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 78.2 \end_layout @@ -1909,8 +1940,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -35.847 \end_layout @@ -1919,8 +1949,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 5,6 \end_layout @@ -1931,8 +1960,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 5 \end_layout @@ -1941,8 +1969,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 9607.4 \end_layout @@ -1951,8 +1978,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -0.4 \end_layout @@ -1961,8 +1987,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -0.4 \end_layout @@ -1971,8 +1996,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 60 \end_layout @@ -1981,8 +2005,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1.4 \end_layout @@ -1991,16 +2014,13 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1.669 -\begin_inset ERT +\begin_inset Flex tablenotemark status collapsed -\begin_layout Standard - -\backslash -tablenotemark{c} +\begin_layout Plain Layout +c \end_layout \end_inset @@ -2013,8 +2033,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1.574 \end_layout @@ -2023,8 +2042,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 2.343 \end_layout @@ -2033,8 +2051,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 8.0 \end_layout @@ -2043,8 +2060,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 8.9 \end_layout @@ -2053,8 +2069,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -33.417 \end_layout @@ -2063,8 +2078,7 @@ tablenotemark{c} \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 7 \end_layout @@ -2072,131 +2086,118 @@ tablenotemark{c} - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 6 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 31638.6 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 1.6 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 0.1 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 39 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 315.2 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 3.433 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 3.075 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 7.488 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 92.1 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 25.3 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout -12.052 \end_layout \end_inset - + \begin_inset Text -\begin_layout Standard - +\begin_layout Plain Layout 8 \end_layout @@ -2210,55 +2211,85 @@ tablenotemark{c} \end_layout -\begin_layout Standard - - +\begin_layout Table note +a \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout -\backslash -tablenotetext{a}{Sample footnote for table~ -\backslash -ref{tbl-2} that was generated with the -\backslash -LaTeX -\backslash - table environment} +}{ \end_layout -\begin_layout Standard +\end_inset +Sample footnote for table +\begin_inset space ~ +\end_inset + + +\begin_inset CommandInset ref +LatexCommand ref +reference "tbl-2" + +\end_inset + + that was generated with the LaTeX table environment \end_layout -\begin_layout Standard +\begin_layout Table note +b +\begin_inset ERT +status collapsed -\backslash -tablenotetext{b}{Yet another sample footnote for table~ -\backslash -ref{tbl-2}} +\begin_layout Plain Layout + +}{ \end_layout -\begin_layout Standard +\end_inset + +Yet another sample footnote for table +\begin_inset space ~ +\end_inset + + +\begin_inset CommandInset ref +LatexCommand ref +reference "tbl-2" + +\end_inset + \end_layout -\begin_layout Standard +\begin_layout Table note +c +\begin_inset ERT +status collapsed -\backslash -tablenotetext{c}{Another sample footnote for table~ -\backslash -ref{tbl-2}} +\begin_layout Plain Layout + +}{ \end_layout \end_inset +Another sample footnote for table +\begin_inset space ~ +\end_inset + + +\begin_inset CommandInset ref +LatexCommand ref +reference "tbl-2" + +\end_inset + \end_layout \begin_layout TableComments - We can also attach a long-ish paragraph of explanatory material to a table. Use \backslash @@ -2269,7 +2300,6 @@ tablerefs to append a list of references. \end_layout \begin_layout TableRefs - (1) Barbuy, Spite, & Spite 1985; (2) Bond 1980; (3) Carbon et al. 1987; (4) Hobbs & Duncan 1987; (5) Gilroy et al. 1988: (6) Gratton & Ortolani 1986; (7) Gratton & Sneden 1987; (8) Gratton @@ -2285,15 +2315,15 @@ tablerefs to append a list of references. \end_inset + \end_layout \begin_layout Standard - - \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + % LyX can load deluxetable files verbatim. To see this in action, uncomment the following \end_layout @@ -2304,12 +2334,11 @@ status collapsed \end_layout \begin_layout Standard - - \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + % line (delete the \end_layout @@ -2323,7 +2352,8 @@ status collapsed \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + % \end_layout @@ -2337,7 +2367,8 @@ status collapsed \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + ) and copy the file table.tex from the AASTeX 5.0 distribution into \end_layout @@ -2347,12 +2378,11 @@ status collapsed \end_layout \begin_layout Standard - - \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + % the same directory as this file. \end_layout @@ -2362,24 +2392,24 @@ status collapsed \end_layout \begin_layout Standard - - \begin_inset ERT status collapsed -\begin_layout Standard +\begin_layout Plain Layout + % \end_layout \end_inset -\begin_inset Include \input{table} +\begin_inset CommandInset include +LatexCommand input +filename "table" \end_inset - \end_layout \end_body