| 1 |
%
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| 2 |
% My Macros
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| 3 |
%
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| 4 |
% Macro declarations
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| 5 |
%
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| 6 |
%---- SLASH
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| 7 |
\def\slasha#1{#1\hskip-0.65em /} %slasha per caratteri piccoli
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| 8 |
\def\slashb#1{#1\hskip-1.3em /} %slashb per quelli grandi
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| 9 |
\def\slashc#1{#1\hskip-.4em /}
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| 10 |
%
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| 11 |
%---- UNITA` DI MISURA
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| 12 |
\def \pb {{\rm \, pb}}
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| 13 |
\def \fb {{\rm \, fb}}
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| 14 |
\def \ipb {{\rm \, pb^{-1}}}
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| 15 |
\def \ifb {{\rm \, fb^{-1}}}
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| 16 |
\def \eV {{\rm \, eV}}
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| 17 |
\def \keV {{\rm \, keV}}
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| 18 |
\def \MeV {{\rm \, MeV}}
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| 19 |
\def \GeV {{\rm \, GeV}}
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| 20 |
\def \TeV {{\rm \, TeV}}
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| 21 |
\def \TeVc {\TeV/c}
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| 22 |
\def \TeVcc {\TeV/c^2}
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| 23 |
\def \GeVc {\GeV/c}
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| 24 |
\def \GeVcc {\GeV/c^2}
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| 25 |
\def \MeVc {\MeV/c}
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| 26 |
\def \MeVcc {\MeV/c^2}
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| 27 |
%
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| 28 |
%---- SIMBOLI
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| 29 |
\def\ga{\mathrel{\raise.3ex\hbox{$>$\kern-.75em\lower1ex\hbox{$\sim$}}}}
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| 30 |
\def\la{\mathrel{\raise.3ex\hbox{$<$\kern-.75em\lower1ex\hbox{$\sim$}}}}
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| 31 |
\newcommand {\lesssim}
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| 32 |
{\,\raisebox{-0.6ex}{$\stackrel{\textstyle<}{\textstyle\sim}$}\,}
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| 33 |
\newcommand {\gtrsim}
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| 34 |
{\,\raisebox{-0.6ex}{$\stackrel{\textstyle>}{\textstyle\sim}$}\,}
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| 35 |
\newcommand{\ckm}{$\checkmark$}
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| 36 |
%
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| 37 |
%---- MISCELLANEA
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| 38 |
\newcommand {\slashed}[1] { \mbox{\rlap{\hbox{/}} #1 }}
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| 39 |
\newcommand {\onehalf} {\raisebox{0.1ex}{${\frac{1}{2}}$}}
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| 40 |
\newcommand {\fivethirds} {\raisebox{0.1ex}{${\frac{5}{3}}$}}
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| 41 |
\newcommand {\OR} {{\tt OR}\,}
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| 42 |
\newcommand {\BR} {{\rm BR}\,}
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| 43 |
\newcommand {\rts} {\sqrt{s}}
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| 44 |
\newcommand {\lumi} {\mathcal{L}}
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| 45 |
\newcommand {\Lumi} {\int\lumi\mathrm{d}t}
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| 46 |
\newcommand {\gradi} {^\circ}
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| 47 |
\newcommand {\de} {\partial}
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| 48 |
\newcommand {\um} {\, \mu \rm m}
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| 49 |
\newcommand {\nm} {\rm \, nm}
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| 50 |
\newcommand {\mrad} {\rm \, mrad}
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| 51 |
\newcommand {\us} {\, \mu \rm s}
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| 52 |
\newcommand {\cm} {\rm \, cm}
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| 53 |
\newcommand {\mm} {\rm \, mm}
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| 54 |
\newcommand {\mA} {\rm \, mA}
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| 55 |
\newcommand {\muF} {\rm \, \mu F}
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| 56 |
\newcommand {\uV} {\rm \, \mu V}
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| 57 |
\newcommand {\mV} {\rm \, mV}
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| 58 |
\newcommand {\m} {\rm \, m}
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| 59 |
\newcommand {\km} {\rm \, km}
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| 60 |
\newcommand {\V} {\rm \, V}
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| 61 |
\newcommand {\T} {\rm \, T}
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| 62 |
\newcommand {\kV} {\rm \, kV}
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| 63 |
\newcommand {\kVm} {\rm \, kV\! / \! m}
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| 64 |
\newcommand {\MVm} {\rm \, MV\! / \! m}
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| 65 |
\newcommand {\MHz} {\rm \, MHz}
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| 66 |
\newcommand {\kHz} {\rm \, kHz}
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| 67 |
\newcommand {\ohm} {\, \Omega}
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| 68 |
\newcommand {\ns} {\rm \, ns}
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| 69 |
\newcommand {\ps} {\rm \, ps}
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| 70 |
%
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| 71 |
%---- THEORY groups & AOB
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| 72 |
\newcommand {\gws} {\mathrm{SU(2)_L \otimes U(1)_Y}}
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| 73 |
\newcommand {\sul} {\mathrm{SU(2)_L}}
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| 74 |
\newcommand {\suc} {\mathrm{SU(3)_C}}
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| 75 |
\newcommand {\ul} {\mathrm{U(1)_Y}}
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| 76 |
\newcommand {\uem} {\mathrm{U(1)_{em}}}
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| 77 |
\newcommand {\sigmabar} {\overline{\sigma}}
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| 78 |
\newcommand {\gmunu} {g^{\mu \nu}}
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| 79 |
\newcommand {\munu} {{\mu \nu}}
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| 80 |
\newcommand {\obra} {\langle 0 |}
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| 81 |
\newcommand {\oket} {| 0 \rangle}
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| 82 |
%
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| 83 |
%---- THEORY lepton fields
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| 84 |
\newcommand {\LL} {L^{\alpha}_{\mathrm L}}
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| 85 |
\newcommand {\LLd} {L^{\dagger \alpha}_{\mathrm L}}
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| 86 |
\newcommand {\lL} {\ell^{\alpha}_{\mathrm L}}
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| 87 |
\newcommand {\lLd} {\ell^{\dagger \alpha}_{\mathrm L}}
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| 88 |
\newcommand {\ld} {\ell^{\dagger \alpha}}
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| 89 |
\newcommand {\lb} {\overline{\ell}^{\alpha}}
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| 90 |
\newcommand {\lR} {\ell^{\alpha}_{\mathrm R}}
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| 91 |
\newcommand {\lRd} {\ell^{\dagger \alpha}_{\mathrm R}}
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| 92 |
\newcommand {\nuL} {\nu^{\alpha}_{\mathrm L}}
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| 93 |
\newcommand {\nuLb} {\overline{\nu}^{\alpha}_{\mathrm L}}
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| 94 |
\newcommand {\nub} {\overline{\nu}^{\alpha}}
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| 95 |
\newcommand {\lept} {\ell^\alpha}
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| 96 |
\newcommand {\neut} {\nu^{\alpha}}
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| 97 |
\newcommand {\nuLd} {\nu^{\dagger \alpha}_{\mathrm L}}
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| 98 |
\newcommand {\Phid} {\Phi^\dagger}
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| 99 |
%
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| 100 |
%---- THEORY quark fields
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| 101 |
\newcommand {\up} {u^{\alpha}}
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| 102 |
\newcommand {\ub} {\overline{u}^{\alpha}}
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| 103 |
\newcommand {\down} {d^{\alpha}}
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| 104 |
\newcommand {\db} {\overline{d}^{\alpha}}
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| 105 |
\newcommand {\QL} {Q^{\alpha}_{\mathrm L}}
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| 106 |
\newcommand {\QLd} {Q^{\dagger \alpha}_{\mathrm L}}
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| 107 |
\newcommand {\UL} {U^{\alpha}_{\mathrm L}}
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| 108 |
\newcommand {\ULd} {U^{\dagger \alpha}_{\mathrm L}}
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| 109 |
\newcommand {\UR} {U^{\alpha}_{\mathrm R}}
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| 110 |
\newcommand {\URd} {U^{\dagger \alpha}_{\mathrm R}}
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| 111 |
\newcommand {\DL} {D^{\alpha}_{\mathrm L}}
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| 112 |
\newcommand {\DLd} {D^{\dagger \alpha}_{\mathrm L}}
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| 113 |
\newcommand {\DR} {D^{\alpha}_{\mathrm R}}
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| 114 |
\newcommand {\DRd} {D^{\dagger \alpha}_{\mathrm R}}
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| 115 |
\newcommand {\bfell} {\ell\kern-0.4em
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| 116 |
\ell\kern-0.4em
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| 117 |
\ell\kern-0.4em
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| 118 |
\ell }
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| 119 |
\newcommand {\obfell} {\overline{\ell}\kern-0.4em
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| 120 |
\overline{\ell}\kern-0.4em
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| 121 |
\overline{\ell}\kern-0.4em
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| 122 |
\overline{\ell}}
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| 123 |
\newcommand {\bfH} {\, {\cal H}\kern-0.5em \kern-0.4em
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| 124 |
{\cal H}\kern-0.5em \kern-0.4em
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| 125 |
{\cal H}\kern0.1em }
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| 126 |
\newcommand {\obfH} {\, \overline{\cal H}\kern-0.5em \kern-0.4em
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| 127 |
\overline{\cal H}\kern-0.5em \kern-0.4em
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| 128 |
\overline{\cal H}\kern0.1em }
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| 129 |
%
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| 130 |
%---- PARTICELLE
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| 131 |
\def \b {{\mathrm b}}
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| 132 |
\def \t {{\mathrm t}}
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| 133 |
\def \charm {{\mathrm c}}
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| 134 |
\def \d {{\mathrm d}}
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| 135 |
\def \u {{\mathrm u}}
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| 136 |
\def \e {{\mathrm e}}
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| 137 |
\def \q {{\mathrm q}}
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| 138 |
\def \g {{\mathrm g}}
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| 139 |
\def \p {{\mathrm p}}
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| 140 |
\def \s {{\mathrm s}}
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| 141 |
\def \n {{\mathrm n}}
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| 142 |
\def \h {{\mathrm h}}
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| 143 |
\def \l {\ell}
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| 144 |
\def \f {{\mathrm f}}
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| 145 |
%\def \f {{f}}
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| 146 |
\def \A {{\mathrm A}}
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| 147 |
\def \B {{\mathrm B}}
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| 148 |
\def \D {{\mathrm D}}
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| 149 |
\def \K {{\mathrm K}}
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| 150 |
\def \X {{\mathrm X}}
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| 151 |
\def \Y {{\mathrm Y}}
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| 152 |
\def \W {{\mathrm W}}
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| 153 |
\def \H {{\mathrm H}}
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| 154 |
\def \Z {{\mathrm Z}}
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| 155 |
\def \S {{\mathrm S}}
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| 156 |
\def \N {{\mathrm N}}
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| 157 |
\def \L {{\mathrm L}}
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| 158 |
\def \R {{\mathrm R}}
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| 159 |
\def \P {{\mathrm P}}
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| 160 |
\def \G {{\mathrm G}}
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| 161 |
%
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| 162 |
%---- Higgs
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| 163 |
\newcommand {\ho} {{\h^0}}
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| 164 |
\newcommand {\Ho} {{\H^0}}
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| 165 |
\newcommand {\Ao} {{\A^0}}
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| 166 |
\newcommand {\Hpm} {{\H^\pm}}
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| 167 |
\newcommand {\clsb} {{\mathrm CL_{\rm s+b}}}
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| 168 |
\newcommand {\clb} {{\mathrm CL_{\rm b}}}
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| 169 |
%
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| 170 |
%---- SUSY
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| 171 |
\newcommand {\dm} {\Delta m}
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| 172 |
\newcommand {\dM} {\Delta M}
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| 173 |
\newcommand {\ldm} {\mbox{``low $\dm$''}}
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| 174 |
\newcommand {\hdm} {\mbox{``high $\dm$''}}
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| 175 |
\newcommand {\nnc} {{\overline{\mathrm N}_{95}}}
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| 176 |
\newcommand {\snc} {{\overline{\sigma}_{95}}}
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| 177 |
\newcommand {\susy} {{supersymmetry}}
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| 178 |
\newcommand {\susyc} {{supersymmetric}}
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| 179 |
\newcommand {\aj} {\mbox{\sf AJ}}
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| 180 |
\newcommand {\ajl} {\mbox{\sf AJL}}
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| 181 |
\newcommand {\llh} {\mbox{\sf LLH}}
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| 182 |
%
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| 183 |
%---- SPARTICELLE
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| 184 |
\newcommand {\rpc} {{\rm RPC}}
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| 185 |
\newcommand {\rpv} {{\rm RPV}}
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| 186 |
\newcommand {\sfe} {{\tilde{\f}}}
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| 187 |
\newcommand {\sfL} {{\tilde{\f}_{\mathrm L}}}
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| 188 |
\newcommand {\sfR} {{\tilde{\f}_{\mathrm R}}}
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| 189 |
\newcommand {\sfone} {{\tilde{\f}_{1}}}
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| 190 |
\newcommand {\sftwo} {{\tilde{\f}_{2}}}
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| 191 |
\newcommand {\sneu} {{\tilde{\nu}}}
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| 192 |
\newcommand {\wino} {{\mathrm{\widetilde{W}}}}
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| 193 |
\newcommand {\bino} {{\mathrm{\widetilde{B}}}}
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| 194 |
\newcommand {\se} {{\mathrm{\tilde{e}}}}
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| 195 |
\newcommand {\seR} {{\mathrm{\tilde{e}_{R}}}}
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| 196 |
\newcommand {\seL} {{\mathrm{\tilde{e}_{L}}}}
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| 197 |
\newcommand {\st} {{\mathrm{\tilde{\tau}}}}
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| 198 |
\newcommand {\stR} {{\mathrm{\tilde{\tau}_{R}}}}
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| 199 |
\newcommand {\stL} {{\mathrm{\tilde{\tau}_{L}}}}
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| 200 |
\newcommand {\stone} {{\mathrm{\tilde{\tau}_{1}}}}
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| 201 |
\newcommand {\sttwo} {{\mathrm{\tilde{\tau}_{2}}}}
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| 202 |
\newcommand {\sm} {{\mathrm{\tilde{\mu}}}}
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| 203 |
\newcommand {\smR} {{\mathrm{\tilde{\mu}_{R}}}}
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| 204 |
\newcommand {\smL} {{\mathrm{\tilde{\mu}_{L}}}}
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| 205 |
\newcommand {\Sup} {{\mathrm{\tilde{u}}}}
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| 206 |
\newcommand {\suR} {{\mathrm{\tilde{u}_{R}}}}
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| 207 |
\newcommand {\suL} {{\mathrm{\tilde{u}_{L}}}}
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| 208 |
\newcommand {\sdo} {{\mathrm{\tilde{d}}}}
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| 209 |
\newcommand {\sdR} {{\mathrm{\tilde{d}_{R}}}}
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| 210 |
\newcommand {\sdL} {{\mathrm{\tilde{d}_{L}}}}
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| 211 |
\newcommand {\sch} {{\mathrm{\tilde{c}}}}
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| 212 |
\newcommand {\scR} {{\mathrm{\tilde{c}_{R}}}}
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| 213 |
\newcommand {\scL} {{\mathrm{\tilde{c}_{L}}}}
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| 214 |
\newcommand {\sst} {{\mathrm{\tilde{s}}}}
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| 215 |
\newcommand {\ssR} {{\mathrm{\tilde{s}_{R}}}}
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| 216 |
\newcommand {\ssL} {{\mathrm{\tilde{s}_{L}}}}
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| 217 |
\newcommand {\stopR} {{\tilde{\mathrm{t}}_{R}}}
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| 218 |
\newcommand {\stopL} {{\tilde{\mathrm{t}}_{L}}}
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| 219 |
\newcommand {\stopone} {{\tilde{\mathrm{t}}_{1}}}
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| 220 |
\newcommand {\stoptwo} {{\mathrm{\tilde{t}_{2}}}}
|
| 221 |
\newcommand {\sto} {{\tilde{\mathrm{t}}}}
|
| 222 |
\newcommand {\SQ} {{\mathrm{\widetilde{Q}}}}
|
| 223 |
\newcommand {\STO} {{\mathrm{\widetilde{T}}}}
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| 224 |
\newcommand {\glu} {{\mathrm{\tilde{g}}}}
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| 225 |
\newcommand {\sbotR} {{\mathrm{\tilde{b}_{R}}}}
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| 226 |
\newcommand {\sbotL} {{\mathrm{\tilde{b}_{L}}}}
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| 227 |
\newcommand {\sbotone} {{\mathrm{\tilde{b}_{1}}}}
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| 228 |
\newcommand {\sbottwo} {{\mathrm{\tilde{b}_{2}}}}
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| 229 |
\newcommand {\sbot} {{\tilde{\mathrm{b}}}}
|
| 230 |
\newcommand {\squa} {{\tilde{\mathrm{q}}}}
|
| 231 |
\newcommand {\squal} {{\tilde{\mathrm{q}}_{\rm L}}}
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| 232 |
\newcommand {\squar} {{\tilde{\mathrm{q}}_{\rm R}}}
|
| 233 |
\newcommand {\sqL} {{\tilde{\mathrm{q}}_{\rm L}}}
|
| 234 |
\newcommand {\sqR} {{\tilde{\mathrm{q}}_{\rm R}}}
|
| 235 |
\newcommand {\snu} {{\tilde{\nu}}}
|
| 236 |
\newcommand {\snue} {{\tilde{\nu}_{\mathrm e}}}
|
| 237 |
\newcommand {\snum} {{\tilde{\nu}_{\mu}}}
|
| 238 |
\newcommand {\snut} {{\tilde{\nu}_{\tau}}}
|
| 239 |
\newcommand {\neu} {{\chi}}
|
| 240 |
\newcommand {\chap} {{\chi^+}}
|
| 241 |
\newcommand {\cham} {{\chi^-}}
|
| 242 |
\newcommand {\chapm} {{\chi^\pm}}
|
| 243 |
|
| 244 |
%
|
| 245 |
%---- SUSY PARAMETRI
|
| 246 |
\newcommand {\thstop} {\mathrm{\theta_{\tilde{t}}}}
|
| 247 |
\newcommand {\thsbot} {\mathrm{\theta_{\tilde{b}}}}
|
| 248 |
\newcommand {\thsqua} {\mathrm{\theta_{\tilde{q}}}}
|
| 249 |
\newcommand {\Mcha}{M_{\chi^\pm}}
|
| 250 |
\newcommand {\Mchi}{M_\chi}
|
| 251 |
\newcommand {\Msnu}{M_{\tilde{\nu}}}
|
| 252 |
\newcommand {\tanb}{\tan\beta}
|
| 253 |
%
|
| 254 |
%---- ABBREVIAZIONI
|
| 255 |
|
| 256 |
%
|
| 257 |
%---- PROCESSI FISICI
|
| 258 |
\newcommand {\rb} {{\rm R_{\b}}}
|
| 259 |
\newcommand {\qq} {{\q \overline{\q}}}
|
| 260 |
\newcommand {\bb} {{\b \overline{\b}}}
|
| 261 |
\newcommand {\cc} {{\charm \overline{\charm}}}
|
| 262 |
\newcommand {\ff} {{\f \overline{\f}}}
|
| 263 |
\newcommand {\el} {{\e ^+}}
|
| 264 |
\newcommand {\po} {{\e ^-}}
|
| 265 |
\newcommand {\ee} {{\e ^+ \e ^-}}
|
| 266 |
\newcommand {\fbody} {{\sto \to \b \chi {\rm f \bar{f}'}}}
|
| 267 |
\newcommand {\gaga} {\gamma\gamma}
|
| 268 |
\newcommand {\ggqq} {\gamma\gamma \rightarrow \q\overline{\q}}
|
| 269 |
\newcommand {\ggtt} {\gamma\gamma \rightarrow \tau^{+}\tau^{-}}
|
| 270 |
\newcommand {\qqg} {\q\overline{\q}\gamma}
|
| 271 |
\newcommand {\ttg} {\tau^{+}\tau^{-}\gamma}
|
| 272 |
\newcommand {\wenu} {{\rm We\nu_\e}}
|
| 273 |
\newcommand {\gsZ} {\gamma^\star\mathrm{Z}}
|
| 274 |
\newcommand {\ggh} {\gamma\gamma\rightarrow{\mathrm{hadrons}}}
|
| 275 |
\newcommand {\ZZg} {\mathrm ZZ^{*}/\gamma^{*}}
|
| 276 |
\newcommand {\ZZ} {{\mathrm ZZ}}
|
| 277 |
%
|
| 278 |
%---- VARIABILI
|
| 279 |
\newcommand {\zo} {{z_0}}
|
| 280 |
\newcommand {\ip} {{d_0}}
|
| 281 |
%\newcommand {\thr} {{T_{\rm thrust}}}
|
| 282 |
\newcommand {\thr} {{{\rm thrust}}}
|
| 283 |
\newcommand {\athr} {{\hat{\rm a}_{\rm thrust}}}
|
| 284 |
\newcommand {\ththr} {{\theta_{\rm thrust}}}
|
| 285 |
\newcommand {\acol} {{\Phi_{\rm acol}}}
|
| 286 |
\newcommand {\acop} {{\Phi_{\rm acop}}}
|
| 287 |
\newcommand {\acopt} {{\Phi_{\rm acop_T}}}
|
| 288 |
\newcommand {\thpoint} {\theta_{\rm point}}
|
| 289 |
\newcommand {\thscat} {\theta_{\rm scat}}
|
| 290 |
\newcommand {\etwelve} {E_{12\gradi}}
|
| 291 |
\newcommand {\ethirty} {E_{30\gradi}}
|
| 292 |
\newcommand {\eiso}[1] {E^{\, \triangleleft 30\gradi}_{#1}}
|
| 293 |
\newcommand {\phimiss} {{\phi_{\vec{p}_{\rm miss}}}}
|
| 294 |
\newcommand {\ewedge} {E(\phi_{\vec{p}_{\rm miss}}\pm 15\gradi)}
|
| 295 |
%\newcommand {\ewedge} {{E_{\rm w}}}
|
| 296 |
\newcommand {\evis} {E_{\rm vis}}
|
| 297 |
\newcommand {\etot} {E_{\rm vis}}
|
| 298 |
\newcommand {\emis} {E_{\rm miss}}
|
| 299 |
\newcommand {\mvis} {M_{\rm vis}}
|
| 300 |
\newcommand {\mtot} {M_{\rm vis}}
|
| 301 |
\newcommand {\mmis} {M_{\rm miss}}
|
| 302 |
\newcommand {\mhad} {M^{\rm ex \, \ell_1}_{\rm vis}}
|
| 303 |
\newcommand {\mhadtwo} {M^{\rm ex \, \ell_1\ell_2}_{\rm vis}}
|
| 304 |
\newcommand {\ehad} {E^{\rm NH}_{\rm vis}}
|
| 305 |
\newcommand {\epho} {E^{\gamma}_{\rm vis}}
|
| 306 |
\newcommand {\echa} {E^{\rm ch}_{\rm vis}}
|
| 307 |
\newcommand {\nch} {{N_{\rm ch}}}
|
| 308 |
\newcommand {\elept} {E_{\rm lept}}
|
| 309 |
\newcommand {\elepone} {E_{\ell _1}}
|
| 310 |
\newcommand {\eleptwo} {E_{\ell _2}}
|
| 311 |
\newcommand {\pvis} {{\vec{p}_{\rm vis}}}
|
| 312 |
\newcommand {\pmis} {{\vec{p}_{\rm miss}}}
|
| 313 |
\newcommand {\thmiss} {{\theta_{\pmis}}}
|
| 314 |
\newcommand {\pt} {{p_{\rm t}}}
|
| 315 |
\newcommand {\ptch} {{p_{\rm t}^{\rm ch}}}
|
| 316 |
\newcommand {\pch} {{p^{\rm ch}}}
|
| 317 |
\newcommand {\pz} {{p_z}}
|
| 318 |
\newcommand {\ptnoNH} {{p_{\rm t}^{\rm ex \, NH}}}
|
| 319 |
\newcommand {\puds} {{P_{\rm uds}}}
|
| 320 |
%
|
| 321 |
\newcommand {\pmiss} {{P\!\!\!\,\!/ }}
|
| 322 |
\newcommand {\emiss} {{E\!\!\!\,\!/ }}
|
| 323 |
%
|
| 324 |
%
|
| 325 |
% no more of Christian's random capitalization!
|
| 326 |
% more of mine
|
| 327 |
\newcommand{\brchal}{\cal{B}($\PCha \rightarrow \ell\nu\PChi\ $)}
|
| 328 |
\newcommand{\M}{M_{2}}
|
| 329 |
\newcommand{\Mp}{M_{2}}
|
| 330 |
\newcommand{\sigbg}{\sigma_{\mathrm{bg}}}
|
| 331 |
\newcommand{\ww} {\mathrm {WW}}
|
| 332 |
\newcommand{\zz} {\mathrm Z\gamma^{*}}
|
| 333 |
\newcommand{\ewnu} {\mathrm{eW}\nu}
|
| 334 |
\newcommand{\eez} {\mathrm {eeZ}}
|
| 335 |
\newcommand{\gagall}{{\gamma\gamma\rightarrow \ell\ell }}
|
| 336 |
\newcommand{\Pstaup}{{\widetilde{\tau}_{1}}}
|
| 337 |
\newcommand{\Pstaul}{{\widetilde{\tau}_{L}}}
|
| 338 |
\newcommand{\Pstaur}{{\widetilde{\tau}_{R}}}
|
| 339 |
\newcommand{\mzero}{m_{0}}
|
| 340 |
\newcommand{\msnu}{M_{\tilde{\nu}}}
|
| 341 |
\newcommand{\mcha}{M_{\chi^{\pm}}}
|
| 342 |
\newcommand{\mchi}{M_{\chi}}
|
| 343 |
\newcommand{\mstau}{M_{{\widetilde{\tau}_{1}}}}
|
| 344 |
\newcommand{\atau}{A_{\tau}}
|
| 345 |
\newcommand{\chsnu}{\PCha \rightarrow \ell \tilde{\nu}}
|
| 346 |
\newcommand{\chstau}{\PCha \rightarrow \tilde{\tau}_{1}\nu}
|
| 347 |
\newcommand{\chlep}{\PCha \rightarrow \ell\nu\chi}
|
| 348 |
\newcommand{\Tcsq}{\mathrm{TeV}/c^2}
|
| 349 |
% new for thesis
|
| 350 |
\newcommand{\nobs}{N_{\mathrm{obs}}}
|
| 351 |
\newcommand{\nlim}{N_{\mathrm{lim}}}
|
| 352 |
\newcommand{\Brl}{\cal{B}_{\ell}}
|
| 353 |
\newcommand{\leff} {\mathcal{L}_{\mathrm{eff}}}
|
| 354 |
\newcommand{\dedx}{{\mathrm{d}}E/{\mathrm{d}}x}
|
| 355 |
\newcommand{\chtau}{\PCha \rightarrow \tau\nu\chi}
|
| 356 |
\newcommand{\ssqtw}{\sin^{2}\theta_{\mathrm W}}
|
| 357 |
%\newcommand{\PSql}{\tilde{\mathrm q}_L}
|
| 358 |
%\newcommand{\PSqr}{\tilde{\mathrm q}_R}
|
| 359 |
%\newcommand{\PSq1}{\tilde{\mathrm q}_1}
|
| 360 |
%\newcommand{\PSq2}{\tilde{\mathrm q}_2}
|
| 361 |
%\newcommand{\ww}{{\mathrm WW}}
|
| 362 |
%\newcommand{\zz}{{\mathrm Z\gamma^{*}}}
|
| 363 |
%\newcommand{\eez}{{\mathrm eeZ}}
|
| 364 |
\newcommand{\nnz}{{\mathrm \nu\bar{\nu}Z}}
|
| 365 |
% added by bill
|
| 366 |
\def \ggll {\gamma\gamma \rightarrow \ell^{+}{\ell}^{-}}
|
| 367 |
\def \tautau {\mathrm \tau^{+}\tau^{-}}
|
| 368 |
\def \ffg {f\bar{f}(\gamma)}
|
| 369 |
\def \lll {\ell^{+}{\ell}^{-}}
|
| 370 |
\def \ww {\mathrm WW}
|
| 371 |
\def \zz {\mathrm Z\gamma^{*}}
|
| 372 |
\def \znn {\mathrm Z\nu\nu}
|
| 373 |
\def \zee {\mathrm Zee}
|
| 374 |
\def \rts {\sqrt{s}}
|
| 375 |
\def \mstop {m_{\tilde{\mathrm{t}}}}
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| 376 |
\def \msnu {m_{\tilde{\nu}}}
|
| 377 |
\def \elow {E_{12^{\circ}}}
|
| 378 |
\def \gev { \, \mathrm{GeV}/\it{c}^{\mathrm{2}}}
|
| 379 |
\def \gvm { \, \mathrm{GeV}/\it{c}}
|
| 380 |
\def \mx {M_{\mathrm{eff}}}
|
| 381 |
\newcommand{\neutr}{\chi}
|
| 382 |
%end fabio
|
| 383 |
|
| 384 |
|
| 385 |
|
| 386 |
%dalla mia pretesi
|
| 387 |
|
| 388 |
%\def \X {\mathrm X}
|
| 389 |
%\def \V {\mathrm V}
|
| 390 |
\def \Zcc {\Z \to \charm \bar{\charm} }
|
| 391 |
\def \Zbb {\Z \to \b \bar{\b} }
|
| 392 |
\def \decDS {\D^{*+} \to \D^0 \pi^+}
|
| 393 |
\def \decsDS {\D^{*+} \to \D^0 \pi^+_s}
|
| 394 |
\def \deckp {\D^{0} \to \K^- \pi^+}
|
| 395 |
\def \deckppp {\D^{0} \to \K^- \pi^+ \pi^+ \pi^-}
|
| 396 |
\def \deckpp {\D^{0} \to \K^- \pi^+ \pi^0}
|
| 397 |
\def \deckpS {\D^{0} \to \K^- \pi^+ (\pi^0)}
|
| 398 |
\def \decskp {\D^{*+} \to \pi^{+}_{s} \K^- \pi^+}
|
| 399 |
\def \decskppp {\D^{*+} \to \pi^{+}_{s} \K^- \pi^+ \pi^+ \pi^-}
|
| 400 |
\def \decskpp {\D^{*+} \to \pi^{+}_{s} \K^- \pi^+ \pi^0}
|
| 401 |
\def \decskpS {\D^{*+} \to \pi^{+}_{s} \K^- \pi^+ (\pi^0)}
|
| 402 |
\def \epsc {\varepsilon_{\charm}}
|
| 403 |
\def \epsb {\varepsilon_{\b}}
|
| 404 |
\def \pctod {P_{\charm \to \D^*}}
|
| 405 |
\def \pbtod {P_{\b \to \D^*}}
|
| 406 |
%\def \R {{\mathrm R}}
|
| 407 |
\def \Gbb {\Gamma_{\b\bar{\b}}}
|
| 408 |
\def \Gcc {\Gamma_{\charm\bar{\charm}}}
|
| 409 |
\def \Gh {\Gamma_{\mathrm h}}
|
| 410 |
%
|
| 411 |
% End of my macros
|
| 412 |
%
|
