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Commit | Line | Data |
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a65a7e70 | 1 | % |
2 | % --------------------------------------------------------------- | |
3 | % define new commands/symbols | |
4 | % --------------------------------------------------------------- | |
5 | % | |
6 | % General stuff | |
7 | % | |
8 | \hyphenation{ALICE} | |
9 | \hyphenation{ATLAS} | |
10 | \hyphenation{ALSIM} | |
11 | \hyphenation{SPSLC} | |
12 | \hyphenation{between} | |
13 | \hyphenation{basis} | |
14 | \hyphenation{robust} | |
15 | \hyphenation{cables} | |
16 | \hyphenation{below} | |
17 | \hyphenation{because} | |
18 | \hyphenation{every rectan-gular} | |
19 | \newcommand{\Lumi}{\ensuremath{\cal{L}}} | |
20 | % | |
21 | \newcommand{\clearemptydoublepage}{\newpage{\pagestyle{empty}\cleardoublepage}} | |
22 | \newcommand{\HRule}{\rule{0.4\linewidth}{0.3mm}} | |
23 | \newcommand{\cinst}[2]{$^{\protect\mathrm{#1)}}$~#2\par} | |
24 | \newcommand{\crefi}[1]{$^{\protect\mathrm{#1)}}$} | |
25 | \newcommand{\crefii}[2]{$^{\protect\mathrm{#1,#2)}}$} | |
26 | \newcommand{\Rule}{\rule[-.7ex]{0ex}{2.9ex}} | |
27 | \newcommand{\rbox}[1]{\raisebox{1.5ex}[-1.5ex]{#1}} | |
28 | % | |
29 | % symbols... | |
30 | % | |
31 | \newcommand{\mrm}{\mathrm} | |
32 | \newcommand{\pt}{\ensuremath{p_{\mathrm{t}}} } | |
33 | \newcommand{\et}{\ensuremath{E_{\mathrm{T}}}} | |
34 | %\newcommand {\pT} {\mbox{$p_{\rm t}$}} | |
35 | \newcommand{\mt}{\ensuremath{m_{\mathrm{t}}}} | |
36 | \newcommand{\minv}{\mbox{$m_{\ee}$}} | |
37 | \newcommand{\ee}{\mbox{e$^+$e$^-$}} | |
38 | \newcommand {\rap} {\mbox{$\left | y \right | $}} | |
39 | %\newcommand{\sigee}{\raisebox{0.2ex}{$\sigma_E$}/\raisebox{-0.4ex}{\kern0.1em$E$}} | |
40 | \newcommand{\sigee}{$\sigma_E$/$E$} | |
41 | \newcommand{\dd}{\mrm{d}} | |
42 | % ... & | |
43 | \newcommand{\eg}{{e.g.~\@\xspace}} | |
44 | \newcommand{\ie}{i.e.\@\xspace} | |
45 | \newcommand{\elm}{e.m.\@\xspace} | |
46 | ||
47 | %\def\mt{\relax \ifmmode m_{\mathrm{t}} \else $m_{\mathrm{t}}$\@\xspace\fi} | |
48 | %\def\pt{\relax \ifmmode p_{\mathrm{t}} \else \mbox{$p_{\mathrm{t}}$}\xspace\fi} | |
49 | % | |
50 | % units of measure | |
51 | % | |
52 | \newcommand {\lum} {\, \mbox{${\rm cm}^{-2} {\rm s}^{-1}$}} | |
53 | \newcommand {\barn} {\, \mbox{${\rm barn}$}} | |
54 | \newcommand {\m} {\, \mbox{${\rm m}$}} | |
55 | \newcommand {\bstar} {\, \mbox{$\beta^{*}$}} | |
56 | \newcommand {\hour} {\, \mbox{${\rm h}$}} | |
57 | \newcommand{\dg}{\mbox{$^\circ$}} | |
58 | %\newcommand {\grad} {\mbox{$^{\circ}$}} | |
59 | \newcommand {\mass} {\mbox{\rm GeV$\kern-0.15em /\kern-0.12em c^2$}} | |
60 | \newcommand {\tev} {\mbox{${\rm TeV}$}} | |
61 | \newcommand {\gev} {\mbox{${\rm GeV}$}} | |
62 | \newcommand {\mev} {\mbox{${\rm MeV}$}} | |
63 | \newcommand {\kev} {\mbox{${\rm keV}$}} | |
64 | \newcommand {\mom} {\mbox{\rm GeV$\kern-0.15em /\kern-0.12em c$}} | |
65 | \newcommand {\mum} {\mbox{$\mu {\rm m}$}} | |
66 | \newcommand {\gmom} {\mbox{\rm GeV$\kern-0.15em /\kern-0.12em c$}} | |
67 | \newcommand {\mmass} {\mbox{\rm MeV$\kern-0.15em /\kern-0.12em c^2$}} | |
68 | \newcommand {\mmom} {\mbox{\rm MeV$\kern-0.15em /\kern-0.12em c$}} | |
69 | \newcommand {\nb} {\mbox{\rm nb}} | |
70 | \newcommand {\musec} {\mbox{$\mu {\rm s}$}} | |
71 | \newcommand {\cm} {\mbox{${\rm cm}$}} | |
72 | \newcommand {\mm} {\mbox{${\rm mm}$}} | |
73 | \newcommand {\cmq} {\mbox{${\rm cm}^{2}$}} | |
74 | \newcommand {\dens} {\mbox{${\rm g}/{\rm cm}^{3}$}} | |
75 | % | |
76 | % Particles | |
77 | % | |
78 | \newcommand{\pizero}{\mbox{$\mathrm {\pi^0}$}} | |
79 | \newcommand{\K}{\mbox{$\mathrm {K}$}} | |
80 | \newcommand{\Kzs}{\mbox{$\mathrm {K^0_S}$}} | |
81 | \newcommand{\KzS}{\mbox{$\mathrm {K^0_S}$}} | |
82 | \newcommand{\KzL}{\mbox{$\mathrm {K^0_L}$}} | |
83 | \newcommand{\Jpsi} {\mbox{J\kern-0.05em /\kern-0.05em$\psi$}\xspace} | |
84 | \newcommand{\psip} {\mbox{$\psi^\prime$}\xspace} | |
85 | \newcommand{\Ups} {\mbox{$\Upsilon$}\xspace} | |
86 | \newcommand{\Upsp} {\mbox{$\Upsilon^\prime$}\xspace} | |
87 | \newcommand{\Upspp} {\mbox{$\Upsilon^{\prime\prime}$}\xspace} | |
88 | \newcommand{\qqbar} {\mbox{$q\bar{q}$}\xspace} | |
89 | ||
90 | %\newcommand{\qqbar}{\mbox{$\mathrm {q\overline{q}}$}} | |
91 | \newcommand{\ppbar}{\mbox{$\mathrm {p\overline{p}}$}} | |
92 | \newcommand{\ccbar}{\mbox{$\mathrm {c\overline{c}}$}} | |
93 | \newcommand{\bbbar}{\mbox{$\mathrm {b\overline{b}}$}} | |
94 | \newcommand{\sbbbar}{\mbox{$\scriptstyle\mathrm {b\overline{b}}$}} | |
95 | \newcommand{\ttbar}{\mbox{$\mathrm {t\overline{t}}$}} | |
96 | \newcommand{\sttbar}{\mbox{$\scriptstyle\mathrm {t\overline{t}}$}} | |
97 | \newcommand{\BBbar}{\mbox{$\mathrm {B\overline{B}}$}} | |
98 | \newcommand{\Bzd}{\mbox{$\mathrm {B^0_d}$}} | |
99 | \newcommand{\Bbzd}{\mbox{$\mathrm {\overline{B}^0_d}$}} | |
100 | \newcommand{\Bzs}{\mbox{$\mathrm {B^0_s}$}} | |
101 | \newcommand{\Bbzs}{\mbox{$\mathrm {\overline{B}^0_s}$}} | |
102 | \newcommand{\gaga}{\mbox{$\mathrm {\gamma\gamma}$}} | |
103 | % | |
104 | % Bibliography stuff | |
105 | % | |
106 | \def\NIM#1#2#3{Nucl. Instr. Meth. {\bf #1}\ (#2)\ #3} | |
107 | \def\IEEE#1#2#3{IEEE Trans. Nucl. Sci. {\bf #1}\ (#2)\ #3} | |
108 | \def\NP#1#2#3{Nucl. Phys. {\bf #1}\ (#2)\ #3} | |
109 | \def\PL#1#2#3{Phys. Lett. {\bf #1}\ (#2)\ #3} | |
110 | \def\PR#1#2#3{Phys. Rev. {\bf #1}\ (#2)\ #3} | |
111 | \def\PRL#1#2#3{Phys. Rev. Lett. {\bf #1}\ (#2)\ #3} | |
112 | \def\ZP#1#2#3{Z. Phys. {\bf #1}\ (#2)\ #3} | |
113 | \def\EJP#1#2#3{Eur. J. Phys. {\bf #1}\ (#2)\ #3} | |
114 | \def\JPG#1#2#3{J. Phys. G: Nucl. Part. Phys. {\bf #1}\ (#2)\ #3} | |
115 | \def\RMP#1#2#3{Rev. Mod. Phys. {\bf #1}\ (#2)\ #3} | |
116 | \def\ARNPS#1#2#3{Ann. Rev. Nucl. Part. Sc. {\bf #1}\ (#2)\ #3} | |
117 | \def\PRP#1#2#3{Phys. Rep. {\bf #1}\ (#2)\ #3} | |
118 | \def\RPP#1#2#3{Rep. on Progr. in Phys. {\bf #1}\ (#2)\ #3} | |
119 | %\def\#1#2#3{ {\bf #1}\ (#2)\ #3} | |
120 | ||
121 | \def\ALI#1#2{ALICE Internal Note {\sc #1--#2}} | |
122 | \def\ALIC#1#2#3{ALICE Internal Note {\sc #1--#2 (#3)}} | |
123 | \def\subNIM{submitted to Nucl. Instr. Meth.} | |
124 | \def\subIEEE{submitted to IEEE Trans. Nucl. Sci.} | |
125 | \def\subNP{submitted to Nucl. Phys.} | |
126 | \def\subPL{submitted to Phys. Lett.} | |
127 | \def\subPR{submitted to Phys. Rev.} | |
128 | \def\subPRL{submitted to Phys. Rev. Lett.} | |
129 | \def\subEJP{submitted to Eur. J. Phys.} | |
130 | %\def\tosubNIM{to be submitted to Nucl. Instrum. Methods} | |
131 | %\def\tosubNP{to be submitted to Nucl. Phys.} | |
132 | %\def\tosubPL{to be submitted to Phys. Lett.} | |
133 | %\def\tosubPR{to be submitted to Phys. Rev.} | |
134 | %\def\tosubPRL{to be submitted to Phys. Rev. Lett.} | |
135 | %\def\tosubZP{to be submitted to Z. Phys.} | |
136 | % | |
137 | % Gases | |
138 | % | |
139 | \def\xea{\mbox{Xe,CH$_4$ (10\%)}} | |
140 | \def\xeb{\mbox{Xe,CO$_2$ (10\%)}} | |
141 | \def\xec{\mbox{Xe,CO$_2$ (15\%)}} | |
142 | \def\xed{\mbox{Xe,CO$_2$ (20\%)}} | |
143 | % | |
144 | % other things... | |
145 | % | |
146 | \def\tvi{\vrule height 12pt depth 5pt width 0pt} | |
147 | \def\vphant{\vphantom{{{1\over{2}}\over{{1\over{2}}}}}} | |
148 | \def\dis{\displaystyle} | |
149 | ||
150 | \newlength{\digitwidth} \settowidth{\digitwidth}{\rm 0} | |
151 | \newlength{\ql} \newlength{\qll} \newlength{\qlll} \newlength{\qllll} | |
152 | \newlength{\qlp} \newlength{\qllp} \newlength{\qlllp} \newlength{\qllllp} | |
153 | \settowidth{\ql}{0} \settowidth{\qll}{00} \settowidth{\qlll}{000} \settowidth{\qllll}{0000} | |
154 | \settowidth{\qlp}{.0} \settowidth{\qllp}{.00} \settowidth{\qlllp}{.000} \settowidth{\qllllp}{.0000} | |
155 | \newlength{\qlup} \newlength{\qlupp} | |
156 | \settowidth{\qlup}{$^{\prime}$} \settowidth{\qlupp}{$^{\prime\prime}$} | |
157 | % | |
158 | % --------------------------------------------------------- | |
159 | % - End of Definitions | |
160 | % --------------------------------------------------------- | |
161 | ||
162 | ||
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166 | ||
167 | ||
168 |