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Commit | Line | Data |
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883031eb | 1 | %\r |
2 | % ---------------------------------------------------------------\r | |
3 | % define new commands/symbols\r | |
4 | % ---------------------------------------------------------------\r | |
5 | %\r | |
6 | % General stuff\r | |
7 | %\r | |
8 | \hyphenation{ALICE}\r | |
9 | \hyphenation{ATLAS}\r | |
10 | \hyphenation{ALSIM}\r | |
11 | \hyphenation{SPSLC}\r | |
12 | \hyphenation{between}\r | |
13 | \hyphenation{basis}\r | |
14 | \hyphenation{robust}\r | |
15 | \hyphenation{cables}\r | |
16 | \hyphenation{below}\r | |
17 | \hyphenation{because}\r | |
18 | \hyphenation{every rectan-gular}\r | |
19 | \newcommand{\Lumi}{\ensuremath{\cal{L}}}\r | |
20 | %\r | |
21 | \newcommand{\clearemptydoublepage}{\newpage{\pagestyle{empty}\cleardoublepage}}\r | |
22 | \newcommand{\HRule}{\rule{0.4\linewidth}{0.3mm}}\r | |
23 | \newcommand{\cinst}[2]{$^{\protect\mathrm{#1)}}$~#2\par}\r | |
24 | \newcommand{\crefi}[1]{$^{\protect\mathrm{#1)}}$}\r | |
25 | \newcommand{\crefii}[2]{$^{\protect\mathrm{#1,#2)}}$}\r | |
26 | \newcommand{\Rule}{\rule[-.7ex]{0ex}{2.9ex}}\r | |
27 | \newcommand{\rbox}[1]{\raisebox{1.5ex}[-1.5ex]{#1}}\r | |
28 | %\r | |
29 | % symbols...\r | |
30 | %\r | |
31 | \newcommand{\mrm}{\mathrm}\r | |
32 | \newcommand{\pt}{\ensuremath{p_{\mathrm{t}}} }\r | |
33 | \newcommand{\et}{\ensuremath{E_{\mathrm{T}}}}\r | |
34 | %\newcommand {\pT} {\mbox{$p_{\rm t}$}}\r | |
35 | \newcommand{\mt}{\ensuremath{m_{\mathrm{t}}}}\r | |
36 | \newcommand{\minv}{\mbox{$m_{\ee}$}}\r | |
37 | \newcommand{\ee}{\mbox{e$^+$e$^-$}}\r | |
38 | \newcommand {\rap} {\mbox{$\left | y \right | $}}\r | |
39 | %\newcommand{\sigee}{\raisebox{0.2ex}{$\sigma_E$}/\raisebox{-0.4ex}{\kern0.1em$E$}}\r | |
40 | \newcommand{\sigee}{$\sigma_E$/$E$}\r | |
41 | \newcommand{\dd}{\mrm{d}}\r | |
42 | % ... &\r | |
43 | \newcommand{\eg}{{e.g.~\@\xspace}}\r | |
44 | \newcommand{\ie}{i.e.\@\xspace}\r | |
45 | \newcommand{\elm}{e.m.\@\xspace}\r | |
46 | \r | |
47 | %\def\mt{\relax \ifmmode m_{\mathrm{t}} \else $m_{\mathrm{t}}$\@\xspace\fi}\r | |
48 | %\def\pt{\relax \ifmmode p_{\mathrm{t}} \else \mbox{$p_{\mathrm{t}}$}\xspace\fi}\r | |
49 | %\r | |
50 | % units of measure\r | |
51 | %\r | |
52 | \newcommand {\lum} {\, \mbox{${\rm cm}^{-2} {\rm s}^{-1}$}}\r | |
53 | \newcommand {\barn} {\, \mbox{${\rm barn}$}}\r | |
54 | \newcommand {\m} {\, \mbox{${\rm m}$}}\r | |
55 | \newcommand {\bstar} {\, \mbox{$\beta^{*}$}}\r | |
56 | \newcommand {\hour} {\, \mbox{${\rm h}$}}\r | |
57 | \newcommand{\dg}{\mbox{$^\circ$}}\r | |
58 | %\newcommand {\grad} {\mbox{$^{\circ}$}}\r | |
59 | \newcommand {\mass} {\mbox{\rm GeV$\kern-0.15em /\kern-0.12em c^2$}}\r | |
60 | \newcommand {\tev} {\mbox{${\rm TeV}$}}\r | |
61 | \newcommand {\gev} {\mbox{${\rm GeV}$}}\r | |
62 | \newcommand {\mev} {\mbox{${\rm MeV}$}}\r | |
63 | \newcommand {\kev} {\mbox{${\rm keV}$}}\r | |
64 | \newcommand {\mom} {\mbox{\rm GeV$\kern-0.15em /\kern-0.12em c$}}\r | |
65 | \newcommand {\mum} {\mbox{$\mu {\rm m}$}}\r | |
66 | \newcommand {\gmom} {\mbox{\rm GeV$\kern-0.15em /\kern-0.12em c$}}\r | |
67 | \newcommand {\mmass} {\mbox{\rm MeV$\kern-0.15em /\kern-0.12em c^2$}}\r | |
68 | \newcommand {\mmom} {\mbox{\rm MeV$\kern-0.15em /\kern-0.12em c$}}\r | |
69 | \newcommand {\nb} {\mbox{\rm nb}}\r | |
70 | \newcommand {\musec} {\mbox{$\mu {\rm s}$}}\r | |
71 | \newcommand {\cm} {\mbox{${\rm cm}$}}\r | |
72 | \newcommand {\mm} {\mbox{${\rm mm}$}}\r | |
73 | \newcommand {\cmq} {\mbox{${\rm cm}^{2}$}}\r | |
74 | \newcommand {\dens} {\mbox{${\rm g}/{\rm cm}^{3}$}}\r | |
75 | %\r | |
76 | % Particles\r | |
77 | %\r | |
78 | \newcommand{\pizero}{\mbox{$\mathrm {\pi^0}$}}\r | |
79 | \newcommand{\K}{\mbox{$\mathrm {K}$}}\r | |
80 | \newcommand{\Kzs}{\mbox{$\mathrm {K^0_S}$}}\r | |
81 | \newcommand{\KzS}{\mbox{$\mathrm {K^0_S}$}}\r | |
82 | \newcommand{\KzL}{\mbox{$\mathrm {K^0_L}$}}\r | |
83 | \newcommand{\Jpsi} {\mbox{J\kern-0.05em /\kern-0.05em$\psi$}\xspace}\r | |
84 | \newcommand{\psip} {\mbox{$\psi^\prime$}\xspace}\r | |
85 | \newcommand{\Ups} {\mbox{$\Upsilon$}\xspace}\r | |
86 | \newcommand{\Upsp} {\mbox{$\Upsilon^\prime$}\xspace}\r | |
87 | \newcommand{\Upspp} {\mbox{$\Upsilon^{\prime\prime}$}\xspace}\r | |
88 | \newcommand{\qqbar} {\mbox{$q\bar{q}$}\xspace}\r | |
89 | \r | |
90 | %\newcommand{\qqbar}{\mbox{$\mathrm {q\overline{q}}$}}\r | |
91 | \newcommand{\ppbar}{\mbox{$\mathrm {p\overline{p}}$}}\r | |
92 | \newcommand{\ccbar}{\mbox{$\mathrm {c\overline{c}}$}}\r | |
93 | \newcommand{\bbbar}{\mbox{$\mathrm {b\overline{b}}$}}\r | |
94 | \newcommand{\sbbbar}{\mbox{$\scriptstyle\mathrm {b\overline{b}}$}}\r | |
95 | \newcommand{\ttbar}{\mbox{$\mathrm {t\overline{t}}$}}\r | |
96 | \newcommand{\sttbar}{\mbox{$\scriptstyle\mathrm {t\overline{t}}$}}\r | |
97 | \newcommand{\BBbar}{\mbox{$\mathrm {B\overline{B}}$}}\r | |
98 | \newcommand{\Bzd}{\mbox{$\mathrm {B^0_d}$}}\r | |
99 | \newcommand{\Bbzd}{\mbox{$\mathrm {\overline{B}^0_d}$}}\r | |
100 | \newcommand{\Bzs}{\mbox{$\mathrm {B^0_s}$}}\r | |
101 | \newcommand{\Bbzs}{\mbox{$\mathrm {\overline{B}^0_s}$}}\r | |
102 | \newcommand{\gaga}{\mbox{$\mathrm {\gamma\gamma}$}}\r | |
103 | %\r | |
104 | % Bibliography stuff\r | |
105 | %\r | |
106 | \def\NIM#1#2#3{Nucl. Instr. Meth. {\bf #1}\ (#2)\ #3}\r | |
107 | \def\IEEE#1#2#3{IEEE Trans. Nucl. Sci. {\bf #1}\ (#2)\ #3}\r | |
108 | \def\NP#1#2#3{Nucl. Phys. {\bf #1}\ (#2)\ #3}\r | |
109 | \def\PL#1#2#3{Phys. Lett. {\bf #1}\ (#2)\ #3}\r | |
110 | \def\PR#1#2#3{Phys. Rev. {\bf #1}\ (#2)\ #3}\r | |
111 | \def\PRL#1#2#3{Phys. Rev. Lett. {\bf #1}\ (#2)\ #3}\r | |
112 | \def\ZP#1#2#3{Z. Phys. {\bf #1}\ (#2)\ #3}\r | |
113 | \def\EJP#1#2#3{Eur. J. Phys. {\bf #1}\ (#2)\ #3}\r | |
114 | \def\JPG#1#2#3{J. Phys. G: Nucl. Part. Phys. {\bf #1}\ (#2)\ #3}\r | |
115 | \def\RMP#1#2#3{Rev. Mod. Phys. {\bf #1}\ (#2)\ #3}\r | |
116 | \def\ARNPS#1#2#3{Ann. Rev. Nucl. Part. Sc. {\bf #1}\ (#2)\ #3}\r | |
117 | \def\PRP#1#2#3{Phys. Rep. {\bf #1}\ (#2)\ #3}\r | |
118 | \def\RPP#1#2#3{Rep. on Progr. in Phys. {\bf #1}\ (#2)\ #3}\r | |
119 | %\def\#1#2#3{ {\bf #1}\ (#2)\ #3}\r | |
120 | \r | |
121 | \def\ALI#1#2{ALICE Internal Note {\sc #1--#2}}\r | |
122 | \def\ALIC#1#2#3{ALICE Internal Note {\sc #1--#2 (#3)}}\r | |
123 | \def\subNIM{submitted to Nucl. Instr. Meth.}\r | |
124 | \def\subIEEE{submitted to IEEE Trans. Nucl. Sci.}\r | |
125 | \def\subNP{submitted to Nucl. Phys.}\r | |
126 | \def\subPL{submitted to Phys. Lett.}\r | |
127 | \def\subPR{submitted to Phys. Rev.}\r | |
128 | \def\subPRL{submitted to Phys. Rev. Lett.}\r | |
129 | \def\subEJP{submitted to Eur. J. Phys.}\r | |
130 | %\def\tosubNIM{to be submitted to Nucl. Instrum. Methods}\r | |
131 | %\def\tosubNP{to be submitted to Nucl. Phys.}\r | |
132 | %\def\tosubPL{to be submitted to Phys. Lett.}\r | |
133 | %\def\tosubPR{to be submitted to Phys. Rev.}\r | |
134 | %\def\tosubPRL{to be submitted to Phys. Rev. Lett.}\r | |
135 | %\def\tosubZP{to be submitted to Z. Phys.}\r | |
136 | %\r | |
137 | % Gases\r | |
138 | %\r | |
139 | \def\xea{\mbox{Xe,CH$_4$ (10\%)}}\r | |
140 | \def\xeb{\mbox{Xe,CO$_2$ (10\%)}}\r | |
141 | \def\xec{\mbox{Xe,CO$_2$ (15\%)}}\r | |
142 | \def\xed{\mbox{Xe,CO$_2$ (20\%)}}\r | |
143 | %\r | |
144 | % other things...\r | |
145 | %\r | |
146 | \def\tvi{\vrule height 12pt depth 5pt width 0pt}\r | |
147 | \def\vphant{\vphantom{{{1\over{2}}\over{{1\over{2}}}}}}\r | |
148 | \def\dis{\displaystyle}\r | |
149 | \r | |
150 | \newlength{\digitwidth} \settowidth{\digitwidth}{\rm 0}\r | |
151 | \newlength{\ql} \newlength{\qll} \newlength{\qlll} \newlength{\qllll}\r | |
152 | \newlength{\qlp} \newlength{\qllp} \newlength{\qlllp} \newlength{\qllllp}\r | |
153 | \settowidth{\ql}{0} \settowidth{\qll}{00} \settowidth{\qlll}{000} \settowidth{\qllll}{0000}\r | |
154 | \settowidth{\qlp}{.0} \settowidth{\qllp}{.00} \settowidth{\qlllp}{.000} \settowidth{\qllllp}{.0000}\r | |
155 | \newlength{\qlup} \newlength{\qlupp}\r | |
156 | \settowidth{\qlup}{$^{\prime}$} \settowidth{\qlupp}{$^{\prime\prime}$}\r | |
157 | %\r | |
158 | % ---------------------------------------------------------\r | |
159 | % - End of Definitions\r | |
160 | % ---------------------------------------------------------\r | |
161 | \r | |
162 | \r | |
163 | \r | |
164 | \r | |
165 | \r | |
166 | \r | |
167 | \r | |
168 | \r |