commit 1b123c02005d7c1a1f3f934938f91489530c3101
Author: Thibaut Cuvelier <[email protected]>
Date: Sat Aug 1 22:44:51 2020 +0200
DocBook: improve AAS support.
---
.../docbook/bibliography_precooked_aastex.xml | 236 ++++++++++++++------
lib/layouts/aastex.layout | 2 +
lib/layouts/aastex6.layout | 3 +-
3 files changed, 172 insertions(+), 69 deletions(-)
diff --git a/autotests/export/docbook/bibliography_precooked_aastex.xml
b/autotests/export/docbook/bibliography_precooked_aastex.xml
index d3381b3..baadbc0 100644
--- a/autotests/export/docbook/bibliography_precooked_aastex.xml
+++ b/autotests/export/docbook/bibliography_precooked_aastex.xml
@@ -10,61 +10,81 @@
</section>
<section>
<title>Observations</title>
-<para>All our observations were short direct exposures with CCD's. At Lick
Observatory we used a TI 500<inlineequation><alt role='tex'>\times</alt>
+<para>All our observations were short direct exposures with CCD's. At Lick
Observatory we used a TI 500<inlineequation>
+<alt role='tex'>\times</alt>
<m:math>
<m:mrow><m:mo>×</m:mo>
</m:mrow>
- </m:math></inlineequation>500 chip and a GEC 575<inlineequation><alt
role='tex'>\times</alt>
+ </m:math>
+</inlineequation>500 chip and a GEC 575<inlineequation>
+<alt role='tex'>\times</alt>
<m:math>
<m:mrow><m:mo>×</m:mo>
</m:mrow>
- </m:math></inlineequation>385, on the 1-m Nickel reflector. The only filter
available at Lick was red. At CTIO we used a GEC 575<inlineequation><alt
role='tex'>\times</alt>
+ </m:math>
+</inlineequation>385, on the 1-m Nickel reflector. The only filter available
at Lick was red. At CTIO we used a GEC 575<inlineequation>
+<alt role='tex'>\times</alt>
<m:math>
<m:mrow><m:mo>×</m:mo>
</m:mrow>
- </m:math></inlineequation>385, with <inlineequation><alt role='tex'>B,V,</alt>
+ </m:math>
+</inlineequation>385, with <inlineequation>
+<alt role='tex'>B,V,</alt>
<m:math>
<m:mrow>
<m:mrow><m:mi>B</m:mi><m:mo>,</m:mo><m:mi>V</m:mi><m:mo>,</m:mo>
</m:mrow>
</m:mrow>
- </m:math></inlineequation> and <inlineequation><alt role='tex'>R</alt>
+ </m:math>
+</inlineequation> and <inlineequation>
+<alt role='tex'>R</alt>
<m:math>
<m:mrow><m:mi>R</m:mi>
</m:mrow>
- </m:math></inlineequation> filters, and an RCA 512<inlineequation><alt
role='tex'>\times</alt>
+ </m:math>
+</inlineequation> filters, and an RCA 512<inlineequation>
+<alt role='tex'>\times</alt>
<m:math>
<m:mrow><m:mo>×</m:mo>
</m:mrow>
- </m:math></inlineequation>320, with <inlineequation><alt
role='tex'>U,B,V,R,</alt>
+ </m:math>
+</inlineequation>320, with <inlineequation>
+<alt role='tex'>U,B,V,R,</alt>
<m:math>
<m:mrow>
<m:mrow><m:mi>U</m:mi><m:mo>,</m:mo><m:mi>B</m:mi><m:mo>,</m:mo><m:mi>V</m:mi><m:mo>,</m:mo><m:mi>R</m:mi><m:mo>,</m:mo>
</m:mrow>
</m:mrow>
- </m:math></inlineequation> and <inlineequation><alt role='tex'>I</alt>
+ </m:math>
+</inlineequation> and <inlineequation>
+<alt role='tex'>I</alt>
<m:math>
<m:mrow><m:mi>I</m:mi>
</m:mrow>
- </m:math></inlineequation> 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 <inlineequation><alt role='tex'>U</alt>
+ </m:math>
+</inlineequation> 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 <inlineequation>
+<alt role='tex'>U</alt>
<m:math>
<m:mrow><m:mi>U</m:mi>
</m:mrow>
- </m:math></inlineequation> or even in <inlineequation><alt role='tex'>B</alt>
+ </m:math>
+</inlineequation> or even in <inlineequation>
+<alt role='tex'>B</alt>
<m:math>
<m:mrow><m:mi>B</m:mi>
</m:mrow>
- </m:math></inlineequation>. All four cameras had scales of the order of 0.4
arcsec/pixel, and our field sizes were around 3 arcmin.</para>
+ </m:math>
+</inlineequation>. All four cameras had scales of the order of 0.4
arcsec/pixel, and our field sizes were around 3 arcmin.</para>
<para>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 CCD profiles by collecting from the
literature a number of star-count profiles <biblioref endterm="kin68" />,
<biblioref endterm="pet76" />, <biblioref endterm="har84" />, <biblioref
endterm="ort85" />, as well as photoelectric profiles <biblioref
endterm="kin66" />, <biblioref endterm="kin75" /> and electronographic profiles
<biblioref endterm="kro84" />. In a few cases we judged normality by eye
estimates on one of the Sky Surveys.</para>
</section>
<section>
@@ -74,7 +94,8 @@
<section>
<title>Formalism</title>
<para><anchor xml:id="bozomath" /></para>
-<para>A tree-level amplitude in <inlineequation><alt
role='tex'>e^{+}e^{-}</alt>
+<para>A tree-level amplitude in <inlineequation>
+<alt role='tex'>e^{+}e^{-}</alt>
<m:math>
<m:mrow>
@@ -93,7 +114,9 @@
</m:msup>
</m:mrow>
</m:mrow>
- </m:math></inlineequation> collisions can be expressed in terms of fermion
strings of the form <informalequation><alt
role='tex'>\bar{v}(p_{2},\sigma_{2})P_{-\tau}\hat{a}_{1}\hat{a}_{2}\cdots\hat{a}_{n}u(p_{1},\sigma_{1}),</alt>
+ </m:math>
+</inlineequation> collisions can be expressed in terms of fermion strings of
the form <informalequation>
+<alt
role='tex'>\bar{v}(p_{2},\sigma_{2})P_{-\tau}\hat{a}_{1}\hat{a}_{2}\cdots\hat{a}_{n}u(p_{1},\sigma_{1}),</alt>
<m:math>
<m:mrow>
@@ -178,17 +201,23 @@
<m:mo>,</m:mo>
</m:mrow>
</m:mrow>
- </m:math></informalequation> where <inlineequation><alt role='tex'>p</alt>
+ </m:math>
+</informalequation> where <inlineequation>
+<alt role='tex'>p</alt>
<m:math>
<m:mrow><m:mi>p</m:mi>
</m:mrow>
- </m:math></inlineequation> and <inlineequation><alt role='tex'>\sigma</alt>
+ </m:math>
+</inlineequation> and <inlineequation>
+<alt role='tex'>\sigma</alt>
<m:math>
<m:mrow><m:mi>σ</m:mi>
</m:mrow>
- </m:math></inlineequation> label the initial <inlineequation><alt
role='tex'>e^{\pm}</alt>
+ </m:math>
+</inlineequation> label the initial <inlineequation>
+<alt role='tex'>e^{\pm}</alt>
<m:math>
<m:mrow>
@@ -199,7 +228,9 @@
</m:mrow>
</m:msup>
</m:mrow>
- </m:math></inlineequation> four-momenta and helicities <inlineequation><alt
role='tex'>(\sigma=\pm1)</alt>
+ </m:math>
+</inlineequation> four-momenta and helicities <inlineequation>
+<alt role='tex'>(\sigma=\pm1)</alt>
<m:math>
<m:mrow><m:mo form='prefix' fence='true' stretchy='true'
symmetric='true'><m:mrow>(</m:mrow></m:mo>
@@ -209,7 +240,9 @@
<m:mo form='postfix' fence='true' stretchy='true'
symmetric='true'><m:mrow>)</m:mrow></m:mo>
</m:mrow>
- </m:math></inlineequation>, <inlineequation><alt
role='tex'>\hat{a}_{i}=a_{i}^{\mu}\gamma_{\nu}</alt>
+ </m:math>
+</inlineequation>, <inlineequation>
+<alt role='tex'>\hat{a}_{i}=a_{i}^{\mu}\gamma_{\nu}</alt>
<m:math>
<m:mrow>
@@ -240,7 +273,9 @@
</m:msub>
</m:mrow>
</m:mrow>
- </m:math></inlineequation> and <inlineequation><alt
role='tex'>P_{\tau}=\frac{1}{2}(1+\tau\gamma_{5})</alt>
+ </m:math>
+</inlineequation> and <inlineequation>
+<alt role='tex'>P_{\tau}=\frac{1}{2}(1+\tau\gamma_{5})</alt>
<m:math>
<m:mrow>
@@ -270,7 +305,9 @@
</m:mrow>
</m:mrow>
- </m:math></inlineequation> is a chirality projection operator
<inlineequation><alt role='tex'>(\tau=\pm1)</alt>
+ </m:math>
+</inlineequation> is a chirality projection operator <inlineequation>
+<alt role='tex'>(\tau=\pm1)</alt>
<m:math>
<m:mrow><m:mo form='prefix' fence='true' stretchy='true'
symmetric='true'><m:mrow>(</m:mrow></m:mo>
@@ -280,7 +317,9 @@
<m:mo form='postfix' fence='true' stretchy='true'
symmetric='true'><m:mrow>)</m:mrow></m:mo>
</m:mrow>
- </m:math></inlineequation>. The <inlineequation><alt
role='tex'>a_{i}^{\mu}</alt>
+ </m:math>
+</inlineequation>. The <inlineequation>
+<alt role='tex'>a_{i}^{\mu}</alt>
<m:math>
<m:mrow>
@@ -293,26 +332,34 @@
</m:mrow>
</m:msubsup>
</m:mrow>
- </m:math></inlineequation> may be formed from particle four-momenta,
gauge-boson polarization vectors or fermion strings with an uncontracted
Lorentz index associated with final-state fermions.</para>
+ </m:math>
+</inlineequation> may be formed from particle four-momenta, gauge-boson
polarization vectors or fermion strings with an uncontracted Lorentz index
associated with final-state fermions.</para>
<NoteToEditor>Figures 1 and 2 should appear side-by-side in
print</NoteToEditor>
-<para>In the chiral representation the <inlineequation><alt
role='tex'>\gamma</alt>
+<para>In the chiral representation the <inlineequation>
+<alt role='tex'>\gamma</alt>
<m:math>
<m:mrow><m:mi>γ</m:mi>
</m:mrow>
- </m:math></inlineequation> matrices are expressed in terms of
<inlineequation><alt role='tex'>2\times2</alt>
+ </m:math>
+</inlineequation> matrices are expressed in terms of <inlineequation>
+<alt role='tex'>2\times2</alt>
<m:math>
<m:mrow>
<m:mrow><m:mn>2</m:mn><m:mo>×</m:mo><m:mn>2</m:mn>
</m:mrow>
</m:mrow>
- </m:math></inlineequation> Pauli matrices <inlineequation><alt
role='tex'>\sigma</alt>
+ </m:math>
+</inlineequation> Pauli matrices <inlineequation>
+<alt role='tex'>\sigma</alt>
<m:math>
<m:mrow><m:mi>σ</m:mi>
</m:mrow>
- </m:math></inlineequation> and the unit matrix 1 as <informalequation><alt
role='tex'>\gamma^{\mu} & = & \left(\begin{array}{cc}
+ </m:math>
+</inlineequation> and the unit matrix 1 as <informalequation>
+<alt role='tex'>\gamma^{\mu} & = & \left(\begin{array}{cc}
0 & \sigma_{+}^{\mu}\\
\sigma_{-}^{\mu} & 0
\end{array}\right),\gamma^{5}=\left(\begin{array}{cc}
@@ -420,7 +467,9 @@
</m:mtd>
</m:mtr>
</m:mtable>
- </m:math></informalequation> giving <informalequation><alt
role='tex'>\hat{a}=\left(\begin{array}{cc}
+ </m:math>
+</informalequation> giving <informalequation>
+<alt role='tex'>\hat{a}=\left(\begin{array}{cc}
0 & (\hat{a})_{+}\\
(\hat{a})_{-} & 0
\end{array}\right),(\hat{a})_{\pm}=a_{\mu}\sigma_{\pm}^{\mu},</alt>
@@ -496,11 +545,15 @@
</m:msubsup><m:mo>,</m:mo>
</m:mrow>
</m:mrow>
- </m:math></informalequation> The spinors are expressed in terms of
two-component Weyl spinors as <informalequation><alt
role='tex'>u=\left(\begin{array}{c}
+ </m:math>
+</informalequation> The spinors are expressed in terms of two-component Weyl
spinors as <informalequation>
+<alt role='tex'>u=\left(\begin{array}{c}
(u)_{-}\\
(u)_{+}
-\end{array}\right),v={\textbf{(}}\vdag_{+}{\textbf{,}}\vdag_{-}{\textbf{)}}.</alt>MathML
export failed. Please report this as a bug.</informalequation></para>
-<para>The Weyl spinors are given in terms of helicity eigenstates
<inlineequation><alt role='tex'>\chi_{\lambda}(p)</alt>
+\end{array}\right),v={\textbf{(}}\vdag_{+}{\textbf{,}}\vdag_{-}{\textbf{)}}.</alt>MathML
export failed. Please report this as a bug.
+</informalequation></para>
+<para>The Weyl spinors are given in terms of helicity eigenstates
<inlineequation>
+<alt role='tex'>\chi_{\lambda}(p)</alt>
<m:math>
<m:mrow>
@@ -516,16 +569,20 @@
</m:mrow>
</m:mrow>
- </m:math></inlineequation> with <inlineequation><alt
role='tex'>\lambda=\pm1</alt>
+ </m:math>
+</inlineequation> with <inlineequation>
+<alt role='tex'>\lambda=\pm1</alt>
<m:math>
<m:mrow>
<m:mrow><m:mi>λ</m:mi><m:mo>=</m:mo><m:mo>±</m:mo><m:mn>1</m:mn>
</m:mrow>
</m:mrow>
- </m:math></inlineequation> by </para>
+ </m:math>
+</inlineequation> by </para>
<MathLetters>
-<informalequation><alt role='tex'>u(p,\lambda)_{\pm} & = &
(E\pm\lambda|{\textbf{p}}|)^{1/2}\chi_{\lambda}(p),\\
+<informalequation>
+<alt role='tex'>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)
</alt>
<m:math>
@@ -612,13 +669,15 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mtd>
</m:mtr>
</m:mtable>
- </m:math></informalequation>
+ </m:math>
+</informalequation>
</MathLetters>
</section>
</section>
<section>
<title>Floating material and so forth</title>
-<para>Consider a task that computes profile parameters for a modified
Lorentzian of the form <informalequation><alt
role='tex'>I=\frac{1}{1+d_{1}^{P(1+d_{2})}}</alt>
+<para>Consider a task that computes profile parameters for a modified
Lorentzian of the form <informalequation>
+<alt role='tex'>I=\frac{1}{1+d_{1}^{P(1+d_{2})}}</alt>
<m:math>
<m:mrow>
@@ -654,7 +713,9 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mfrac>
</m:mrow>
</m:mrow>
- </m:math></informalequation> where <informalequation><alt
role='tex'>d_{1}=\sqrt{\left(\begin{array}{c}
+ </m:math>
+</informalequation> where <informalequation>
+<alt role='tex'>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}}</alt>
<m:math>
@@ -737,9 +798,13 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:msqrt>
</m:mrow>
</m:mrow>
- </m:math></informalequation><informalequation><alt
role='tex'>d_{2}=\sqrt{\left(\begin{array}{c}
+ </m:math>
+</informalequation><informalequation>
+<alt role='tex'>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}}</alt>MathML export failed.
Please report this as a bug.</informalequation><informalequation><alt
role='tex'>x_{1}=(x-x_{0})\cos\Theta+(y-y_{0})\sin\Theta</alt>
+\case{y_{1}}{PR_{min}}\end{array}\right)^{2}}</alt>MathML export failed.
Please report this as a bug.
+</informalequation><informalequation>
+<alt role='tex'>x_{1}=(x-x_{0})\cos\Theta+(y-y_{0})\sin\Theta</alt>
<m:math>
<m:mrow>
@@ -774,7 +839,9 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
<m:mo>sin</m:mo><m:mo>Θ</m:mo>
</m:mrow>
</m:mrow>
- </m:math></informalequation><informalequation><alt
role='tex'>y_{1}=-(x-x_{0})\sin\Theta+(y-y_{0})\cos\Theta</alt>
+ </m:math>
+</informalequation><informalequation>
+<alt role='tex'>y_{1}=-(x-x_{0})\sin\Theta+(y-y_{0})\cos\Theta</alt>
<m:math>
<m:mrow>
@@ -809,8 +876,10 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
<m:mo>cos</m:mo><m:mo>Θ</m:mo>
</m:mrow>
</m:mrow>
- </m:math></informalequation></para>
-<para>In these expressions <inlineequation><alt role='tex'>x_{0}</alt>
+ </m:math>
+</informalequation></para>
+<para>In these expressions <inlineequation>
+<alt role='tex'>x_{0}</alt>
<m:math>
<m:mrow>
@@ -821,7 +890,9 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mrow>
</m:msub>
</m:mrow>
- </m:math></inlineequation>,<inlineequation><alt role='tex'>y_{0}</alt>
+ </m:math>
+</inlineequation>,<inlineequation>
+<alt role='tex'>y_{0}</alt>
<m:math>
<m:mrow>
@@ -832,17 +903,23 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mrow>
</m:msub>
</m:mrow>
- </m:math></inlineequation> is the star center, and <inlineequation><alt
role='tex'>\Theta</alt>
+ </m:math>
+</inlineequation> is the star center, and <inlineequation>
+<alt role='tex'>\Theta</alt>
<m:math>
<m:mrow><m:mo>Θ</m:mo>
</m:mrow>
- </m:math></inlineequation> is the angle with the <inlineequation><alt
role='tex'>x</alt>
+ </m:math>
+</inlineequation> is the angle with the <inlineequation>
+<alt role='tex'>x</alt>
<m:math>
<m:mrow><m:mi>x</m:mi>
</m:mrow>
- </m:math></inlineequation> axis. Results of this task are shown in
table <xref linkend="tbl-2" />. It is not clear how these sorts of
analyses may affect determination of <inlineequation><alt
role='tex'>M_{\text{\sun}}</alt>
+ </m:math>
+</inlineequation> axis. Results of this task are shown in table <xref
linkend="tbl-2" />. It is not clear how these sorts of analyses may affect
determination of <inlineequation>
+<alt role='tex'>M_{\text{\sun}}</alt>
<m:math>
<m:mrow>
@@ -855,7 +932,9 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mrow>
</m:msub>
</m:mrow>
- </m:math></inlineequation>, but the assumption is that the alternate results
should be less than 90° out of phase with previous values. We have no
observations of <!-- \ion{Ca}{2} -->. Roughly <inlineequation><alt
role='tex'>\nicefrac{4}{5}</alt>
+ </m:math>
+</inlineequation>, but the assumption is that the alternate results should be
less than 90° out of phase with previous values. We have no observations of
<!-- \ion{Ca}{2} -->. Roughly <inlineequation>
+<alt role='tex'>\nicefrac{4}{5}</alt>
<m:math>
<m:mrow>
@@ -866,8 +945,9 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mrow>
</m:mfrac>
</m:mrow>
- </m:math></inlineequation> of the electronically submitted abstracts for AAS
meetings are error-free. </para>
-<Acknowledgements>We are grateful to V. Barger, T. Han, and R. J. N. Phillips
for doing the math in section <xref linkend="bozomath" />. More
information on the AASTeX macros package are available at <link
xlink:href="http://www.aas.org/publications/aastex";>http://www.aas.org/publications/aastex</link>
or the <link xlink:href="ftp://www.aas.org/pubs/AAS ftp site">AAS ftp
site</link>.</Acknowledgements>
+ </m:math>
+</inlineequation> of the electronically submitted abstracts for AAS meetings
are error-free. </para>
+<acknowledgement><para>We are grateful to V. Barger, T. Han, and R. J. N.
Phillips for doing the math in section <xref linkend="bozomath" />. More
information on the AASTeX macros package are available at <link
xlink:href="http://www.aas.org/publications/aastex";>http://www.aas.org/publications/aastex</link>
or the <link xlink:href="ftp://www.aas.org/pubs/AAS ftp site">AAS ftp
site</link>.</para></acknowledgement>
<Software>IRAF, AIPS, Astropy, ...</Software>
<Appendix></Appendix>
<bibliography>
@@ -895,7 +975,8 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
<tr>
<td align='center' valign='top'>Star </td>
<td align='right' valign='top'> Height </td>
-<td align='right' valign='top'> <inlineequation><alt role='tex'>d_{x}</alt>
+<td align='right' valign='top'> <inlineequation>
+<alt role='tex'>d_{x}</alt>
<m:math>
<m:mrow>
@@ -906,8 +987,10 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mrow>
</m:msub>
</m:mrow>
- </m:math></inlineequation></td>
-<td align='right' valign='top'> <inlineequation><alt role='tex'>d_{y}</alt>
+ </m:math>
+</inlineequation></td>
+<td align='right' valign='top'> <inlineequation>
+<alt role='tex'>d_{y}</alt>
<m:math>
<m:mrow>
@@ -918,14 +1001,18 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mrow>
</m:msub>
</m:mrow>
- </m:math></inlineequation></td>
-<td align='right' valign='top'> <inlineequation><alt role='tex'>n</alt>
+ </m:math>
+</inlineequation></td>
+<td align='right' valign='top'> <inlineequation>
+<alt role='tex'>n</alt>
<m:math>
<m:mrow><m:mi>n</m:mi>
</m:mrow>
- </m:math></inlineequation></td>
-<td align='right' valign='top'> <inlineequation><alt role='tex'>\chi^{2}</alt>
+ </m:math>
+</inlineequation></td>
+<td align='right' valign='top'> <inlineequation>
+<alt role='tex'>\chi^{2}</alt>
<m:math>
<m:mrow>
@@ -936,8 +1023,10 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mrow>
</m:msup>
</m:mrow>
- </m:math></inlineequation></td>
-<td align='right' valign='top'> <inlineequation><alt role='tex'>R_{maj}</alt>
+ </m:math>
+</inlineequation></td>
+<td align='right' valign='top'> <inlineequation>
+<alt role='tex'>R_{maj}</alt>
<m:math>
<m:mrow>
@@ -950,8 +1039,10 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mrow>
</m:msub>
</m:mrow>
- </m:math></inlineequation></td>
-<td align='right' valign='top'> <inlineequation><alt role='tex'>R_{min}</alt>
+ </m:math>
+</inlineequation></td>
+<td align='right' valign='top'> <inlineequation>
+<alt role='tex'>R_{min}</alt>
<m:math>
<m:mrow>
@@ -964,14 +1055,18 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:mrow>
</m:msub>
</m:mrow>
- </m:math></inlineequation></td>
-<td align='center' valign='top' colspan='1'><inlineequation><alt
role='tex'>P</alt>
+ </m:math>
+</inlineequation></td>
+<td align='center' valign='top' colspan='1'><inlineequation>
+<alt role='tex'>P</alt>
<m:math>
<m:mrow><m:mi>P</m:mi>
</m:mrow>
- </m:math></inlineequation>a</td>
-<td align='right' valign='top'> <inlineequation><alt role='tex'>PR_{maj}</alt>
+ </m:math>
+</inlineequation>a</td>
+<td align='right' valign='top'> <inlineequation>
+<alt role='tex'>PR_{maj}</alt>
<m:math>
<m:mrow>
@@ -986,8 +1081,10 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:msub>
</m:mrow>
</m:mrow>
- </m:math></inlineequation></td>
-<td align='right' valign='top'> <inlineequation><alt role='tex'>PR_{min}</alt>
+ </m:math>
+</inlineequation></td>
+<td align='right' valign='top'> <inlineequation>
+<alt role='tex'>PR_{min}</alt>
<m:math>
<m:mrow>
@@ -1002,13 +1099,16 @@ v(p,\lambda)_{\pm} & = &
\pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi
</m:msub>
</m:mrow>
</m:mrow>
- </m:math></inlineequation></td>
-<td align='center' valign='top' colspan='1'><inlineequation><alt
role='tex'>\Theta</alt>
+ </m:math>
+</inlineequation></td>
+<td align='center' valign='top' colspan='1'><inlineequation>
+<alt role='tex'>\Theta</alt>
<m:math>
<m:mrow><m:mo>Θ</m:mo>
</m:mrow>
- </m:math></inlineequation>b</td>
+ </m:math>
+</inlineequation>b</td>
<td align='center' valign='top'>Ref.</td>
</tr>
<tr>
diff --git a/lib/layouts/aastex.layout b/lib/layouts/aastex.layout
index 866c88f..275018a 100644
--- a/lib/layouts/aastex.layout
+++ b/lib/layouts/aastex.layout
@@ -334,6 +334,8 @@ Style Acknowledgements
Size Normal
Shape Italic
EndFont
+ DocBookTag para
+ DocBookWrapperTag acknowledgement
End
diff --git a/lib/layouts/aastex6.layout b/lib/layouts/aastex6.layout
index 1c6054a..52c38be 100644
--- a/lib/layouts/aastex6.layout
+++ b/lib/layouts/aastex6.layout
@@ -67,7 +67,8 @@ Style Software
LabelFont
Shape Italic
EndFont
- DocBookTag application
+ DocBookWrapperTag para
+ DocBookTag application
End
# other new commands are mainly for the user preamble
--
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