TIBTIDNotes/TIBTIDGndingNote/my_macros.tex

%
% My Macros
%
% Macro declarations
%
%---- SLASH
\def\slasha#1{#1\hskip-0.65em /}  %slasha per caratteri piccoli
\def\slashb#1{#1\hskip-1.3em /}   %slashb per quelli grandi
\def\slashc#1{#1\hskip-.4em /}
%
%---- UNITA` DI MISURA
\def \pb        {{\rm \, pb}}
\def \fb        {{\rm \, fb}}
\def \ipb       {{\rm \, pb^{-1}}}
\def \ifb       {{\rm \, fb^{-1}}}
\def \eV        {{\rm \,  eV}}
\def \keV       {{\rm \, keV}}
\def \MeV       {{\rm \, MeV}}
\def \GeV       {{\rm \, GeV}}
\def \TeV       {{\rm \, TeV}}
\def \TeVc      {\TeV/c}
\def \TeVcc     {\TeV/c^2}
\def \GeVc      {\GeV/c}
\def \GeVcc     {\GeV/c^2}
\def \MeVc      {\MeV/c}
\def \MeVcc     {\MeV/c^2}
%
%---- SIMBOLI
\def\ga{\mathrel{\raise.3ex\hbox{$>$\kern-.75em\lower1ex\hbox{$\sim$}}}}
\def\la{\mathrel{\raise.3ex\hbox{$<$\kern-.75em\lower1ex\hbox{$\sim$}}}}
\newcommand {\lesssim}
     {\,\raisebox{-0.6ex}{$\stackrel{\textstyle<}{\textstyle\sim}$}\,}
\newcommand {\gtrsim}
     {\,\raisebox{-0.6ex}{$\stackrel{\textstyle>}{\textstyle\sim}$}\,}
\newcommand{\ckm}{$\checkmark$}
%
%---- MISCELLANEA
\newcommand {\slashed}[1] { \mbox{\rlap{\hbox{/}} #1 }}
\newcommand {\onehalf}    {\raisebox{0.1ex}{${\frac{1}{2}}$}}
\newcommand {\fivethirds} {\raisebox{0.1ex}{${\frac{5}{3}}$}}
\newcommand {\OR}         {{\tt OR}\,}
\newcommand {\BR}         {{\rm BR}\,}
\newcommand {\rts}        {\sqrt{s}}
\newcommand {\lumi}       {\mathcal{L}}
\newcommand {\Lumi}       {\int\lumi\mathrm{d}t}
\newcommand {\gradi}    {^\circ}
\newcommand {\de}         {\partial}
\newcommand {\um}         {\, \mu \rm m}
\newcommand {\nm}         {\rm \, nm}
\newcommand {\mrad}         {\rm \, mrad}
\newcommand {\us}         {\, \mu \rm s}
\newcommand {\cm}         {\rm \, cm}
\newcommand {\mm}         {\rm \, mm}
\newcommand {\mA}         {\rm \, mA}
\newcommand {\muF}         {\rm \, \mu F}
\newcommand {\uV}         {\rm \, \mu V}
\newcommand {\mV}         {\rm \, mV}
\newcommand {\m}          {\rm \, m}
\newcommand {\km}         {\rm \, km}
\newcommand {\V}          {\rm \, V}
\newcommand {\T}          {\rm \, T}
\newcommand {\kV}         {\rm \, kV}
\newcommand {\kVm}        {\rm \, kV\! / \! m} 
\newcommand {\MVm}        {\rm \, MV\! / \! m} 
\newcommand {\MHz}        {\rm \, MHz} 
\newcommand {\kHz}        {\rm \, kHz} 
\newcommand {\ohm}        {\, \Omega} 
\newcommand {\ns}         {\rm \, ns} 
\newcommand {\ps}         {\rm \, ps} 
%
%---- THEORY groups & AOB
\newcommand {\gws}        {\mathrm{SU(2)_L \otimes U(1)_Y}}
\newcommand {\sul}        {\mathrm{SU(2)_L}}
\newcommand {\suc}        {\mathrm{SU(3)_C}}
\newcommand {\ul}         {\mathrm{U(1)_Y}}
\newcommand {\uem}        {\mathrm{U(1)_{em}}}
\newcommand {\sigmabar}   {\overline{\sigma}}
\newcommand {\gmunu}      {g^{\mu \nu}}
\newcommand {\munu}       {{\mu \nu}}
\newcommand {\obra}       {\langle 0 |}
\newcommand {\oket}       {| 0 \rangle}
%
%---- THEORY lepton fields
\newcommand {\LL}         {L^{\alpha}_{\mathrm L}}
\newcommand {\LLd}        {L^{\dagger \alpha}_{\mathrm L}}
\newcommand {\lL}         {\ell^{\alpha}_{\mathrm L}}
\newcommand {\lLd}        {\ell^{\dagger \alpha}_{\mathrm L}}
\newcommand {\ld}         {\ell^{\dagger \alpha}}
\newcommand {\lb}         {\overline{\ell}^{\alpha}}
\newcommand {\lR}         {\ell^{\alpha}_{\mathrm R}}
\newcommand {\lRd}        {\ell^{\dagger \alpha}_{\mathrm R}}
\newcommand {\nuL}        {\nu^{\alpha}_{\mathrm L}}
\newcommand {\nuLb}       {\overline{\nu}^{\alpha}_{\mathrm L}}
\newcommand {\nub}        {\overline{\nu}^{\alpha}}
\newcommand {\lept}       {\ell^\alpha}
\newcommand {\neut}       {\nu^{\alpha}}
\newcommand {\nuLd}       {\nu^{\dagger \alpha}_{\mathrm L}}
\newcommand {\Phid}       {\Phi^\dagger}
%
%---- THEORY quark fields
\newcommand {\up}         {u^{\alpha}}
\newcommand {\ub}         {\overline{u}^{\alpha}}
\newcommand {\down}       {d^{\alpha}}
\newcommand {\db}         {\overline{d}^{\alpha}}
\newcommand {\QL}         {Q^{\alpha}_{\mathrm L}}
\newcommand {\QLd}        {Q^{\dagger \alpha}_{\mathrm L}}
\newcommand {\UL}         {U^{\alpha}_{\mathrm L}}
\newcommand {\ULd}        {U^{\dagger \alpha}_{\mathrm L}}
\newcommand {\UR}         {U^{\alpha}_{\mathrm R}}
\newcommand {\URd}        {U^{\dagger \alpha}_{\mathrm R}}
\newcommand {\DL}         {D^{\alpha}_{\mathrm L}}
\newcommand {\DLd}        {D^{\dagger \alpha}_{\mathrm L}}
\newcommand {\DR}         {D^{\alpha}_{\mathrm R}}
\newcommand {\DRd}        {D^{\dagger \alpha}_{\mathrm R}}
\newcommand {\bfell}      {\ell\kern-0.4em
                           \ell\kern-0.4em
                           \ell\kern-0.4em
                           \ell }
\newcommand {\obfell}     {\overline{\ell}\kern-0.4em
                           \overline{\ell}\kern-0.4em
                           \overline{\ell}\kern-0.4em
                           \overline{\ell}}
\newcommand {\bfH}      {\, {\cal H}\kern-0.5em \kern-0.4em
                           {\cal H}\kern-0.5em \kern-0.4em
                           {\cal H}\kern0.1em }
\newcommand {\obfH}     {\, \overline{\cal H}\kern-0.5em \kern-0.4em 
                           \overline{\cal H}\kern-0.5em \kern-0.4em 
                           \overline{\cal H}\kern0.1em }
%
%---- PARTICELLE
\def \b             {{\mathrm b}}
\def \t             {{\mathrm t}}
\def \charm         {{\mathrm c}}
\def \d             {{\mathrm d}}
\def \u             {{\mathrm u}}
\def \e             {{\mathrm e}}
\def \q             {{\mathrm q}}
\def \g             {{\mathrm g}}
\def \p             {{\mathrm p}}
\def \s             {{\mathrm s}}
\def \n             {{\mathrm n}}
\def \h             {{\mathrm h}}
\def \l             {\ell} 
\def \f             {{\mathrm f}} 
%\def \f             {{f}} 
\def \A             {{\mathrm A}}
\def \B             {{\mathrm B}}
\def \D             {{\mathrm D}}
\def \K             {{\mathrm K}}
\def \X             {{\mathrm X}}
\def \Y             {{\mathrm Y}}
\def \W             {{\mathrm W}}
\def \H             {{\mathrm H}}
\def \Z             {{\mathrm Z}}
\def \S             {{\mathrm S}}
\def \N             {{\mathrm N}}
\def \L             {{\mathrm L}}
\def \R             {{\mathrm R}}
\def \P             {{\mathrm P}}
\def \G             {{\mathrm G}}
%
%---- Higgs
\newcommand {\ho}         {{\h^0}}
\newcommand {\Ho}         {{\H^0}}
\newcommand {\Ao}         {{\A^0}}
\newcommand {\Hpm}        {{\H^\pm}}
\newcommand {\clsb}       {{\mathrm CL_{\rm s+b}}}
\newcommand {\clb}        {{\mathrm CL_{\rm b}}}
%
%---- SUSY
\newcommand {\dm}         {\Delta m}
\newcommand {\dM}         {\Delta M}
\newcommand {\ldm}        {\mbox{``low $\dm$''}}
\newcommand {\hdm}        {\mbox{``high $\dm$''}}
\newcommand {\nnc}        {{\overline{\mathrm N}_{95}}}
\newcommand {\snc}        {{\overline{\sigma}_{95}}}
\newcommand {\susy}       {{supersymmetry}}
\newcommand {\susyc}      {{supersymmetric}}
\newcommand {\aj}         {\mbox{\sf AJ}}
\newcommand {\ajl}        {\mbox{\sf AJL}}
\newcommand {\llh}        {\mbox{\sf LLH}}
%
%---- SPARTICELLE
\newcommand {\rpc}     {{\rm RPC}}
\newcommand {\rpv}     {{\rm RPV}}
\newcommand {\sfe}     {{\tilde{\f}}}
\newcommand {\sfL}     {{\tilde{\f}_{\mathrm L}}}
\newcommand {\sfR}     {{\tilde{\f}_{\mathrm R}}}
\newcommand {\sfone}   {{\tilde{\f}_{1}}}
\newcommand {\sftwo}   {{\tilde{\f}_{2}}}
\newcommand {\sneu}    {{\tilde{\nu}}}
\newcommand {\wino}    {{\mathrm{\widetilde{W}}}}
\newcommand {\bino}    {{\mathrm{\widetilde{B}}}}
\newcommand {\se}      {{\mathrm{\tilde{e}}}}
\newcommand {\seR}     {{\mathrm{\tilde{e}_{R}}}}
\newcommand {\seL}     {{\mathrm{\tilde{e}_{L}}}}
\newcommand {\st}      {{\mathrm{\tilde{\tau}}}}
\newcommand {\stR}     {{\mathrm{\tilde{\tau}_{R}}}}
\newcommand {\stL}     {{\mathrm{\tilde{\tau}_{L}}}}
\newcommand {\stone}   {{\mathrm{\tilde{\tau}_{1}}}}
\newcommand {\sttwo}   {{\mathrm{\tilde{\tau}_{2}}}}
\newcommand {\sm}      {{\mathrm{\tilde{\mu}}}}
\newcommand {\smR}     {{\mathrm{\tilde{\mu}_{R}}}}
\newcommand {\smL}     {{\mathrm{\tilde{\mu}_{L}}}}
\newcommand {\Sup}     {{\mathrm{\tilde{u}}}}
\newcommand {\suR}     {{\mathrm{\tilde{u}_{R}}}}
\newcommand {\suL}     {{\mathrm{\tilde{u}_{L}}}}
\newcommand {\sdo}     {{\mathrm{\tilde{d}}}}
\newcommand {\sdR}     {{\mathrm{\tilde{d}_{R}}}}
\newcommand {\sdL}     {{\mathrm{\tilde{d}_{L}}}}
\newcommand {\sch}     {{\mathrm{\tilde{c}}}}
\newcommand {\scR}     {{\mathrm{\tilde{c}_{R}}}}
\newcommand {\scL}     {{\mathrm{\tilde{c}_{L}}}}
\newcommand {\sst}     {{\mathrm{\tilde{s}}}}
\newcommand {\ssR}     {{\mathrm{\tilde{s}_{R}}}}
\newcommand {\ssL}     {{\mathrm{\tilde{s}_{L}}}}
\newcommand {\stopR}   {{\tilde{\mathrm{t}}_{R}}}
\newcommand {\stopL}   {{\tilde{\mathrm{t}}_{L}}}
\newcommand {\stopone} {{\tilde{\mathrm{t}}_{1}}}
\newcommand {\stoptwo} {{\mathrm{\tilde{t}_{2}}}}
\newcommand {\sto}     {{\tilde{\mathrm{t}}}}
\newcommand {\SQ}      {{\mathrm{\widetilde{Q}}}}
\newcommand {\STO}     {{\mathrm{\widetilde{T}}}}
\newcommand {\glu}     {{\mathrm{\tilde{g}}}}
\newcommand {\sbotR}   {{\mathrm{\tilde{b}_{R}}}}
\newcommand {\sbotL}   {{\mathrm{\tilde{b}_{L}}}}
\newcommand {\sbotone} {{\mathrm{\tilde{b}_{1}}}}
\newcommand {\sbottwo} {{\mathrm{\tilde{b}_{2}}}}
\newcommand {\sbot}    {{\tilde{\mathrm{b}}}}
\newcommand {\squa}    {{\tilde{\mathrm{q}}}}
\newcommand {\squal}   {{\tilde{\mathrm{q}}_{\rm L}}}
\newcommand {\squar}   {{\tilde{\mathrm{q}}_{\rm R}}}
\newcommand {\sqL}     {{\tilde{\mathrm{q}}_{\rm L}}}
\newcommand {\sqR}     {{\tilde{\mathrm{q}}_{\rm R}}}
\newcommand {\snu}     {{\tilde{\nu}}}
\newcommand {\snue}    {{\tilde{\nu}_{\mathrm e}}}
\newcommand {\snum}    {{\tilde{\nu}_{\mu}}}
\newcommand {\snut}    {{\tilde{\nu}_{\tau}}}
\newcommand {\neu}     {{\chi}}
\newcommand {\chap}    {{\chi^+}}
\newcommand {\cham}    {{\chi^-}}
\newcommand {\chapm}   {{\chi^\pm}}

%
%---- SUSY PARAMETRI
\newcommand {\thstop} {\mathrm{\theta_{\tilde{t}}}}
\newcommand {\thsbot} {\mathrm{\theta_{\tilde{b}}}}
\newcommand {\thsqua} {\mathrm{\theta_{\tilde{q}}}}
\newcommand {\Mcha}{M_{\chi^\pm}}
\newcommand {\Mchi}{M_\chi}
\newcommand {\Msnu}{M_{\tilde{\nu}}}
\newcommand {\tanb}{\tan\beta}
%
%---- ABBREVIAZIONI

%
%---- PROCESSI FISICI
\newcommand {\rb}    {{\rm R_{\b}}}
\newcommand {\qq}    {{\q \overline{\q}}}
\newcommand {\bb}    {{\b \overline{\b}}}
\newcommand {\cc}    {{\charm \overline{\charm}}}
\newcommand {\ff}    {{\f \overline{\f}}}
\newcommand {\el}    {{\e ^+}}
\newcommand {\po}    {{\e ^-}}
\newcommand {\ee}    {{\e ^+ \e ^-}}
\newcommand {\fbody} {{\sto \to \b \chi {\rm f \bar{f}'}}}
\newcommand {\gaga}  {\gamma\gamma}
\newcommand {\ggqq}  {\gamma\gamma \rightarrow \q\overline{\q}}
\newcommand {\ggtt}  {\gamma\gamma \rightarrow \tau^{+}\tau^{-}}
\newcommand {\qqg}   {\q\overline{\q}\gamma}
\newcommand {\ttg}   {\tau^{+}\tau^{-}\gamma}
\newcommand {\wenu}  {{\rm We\nu_\e}}
\newcommand {\gsZ}   {\gamma^\star\mathrm{Z}}
\newcommand {\ggh}   {\gamma\gamma\rightarrow{\mathrm{hadrons}}}
\newcommand {\ZZg}   {\mathrm ZZ^{*}/\gamma^{*}}
\newcommand {\ZZ}    {{\mathrm ZZ}}
%
%---- VARIABILI
\newcommand {\zo}      {{z_0}}
\newcommand {\ip}      {{d_0}}
%\newcommand {\thr}     {{T_{\rm thrust}}}
\newcommand {\thr}     {{{\rm thrust}}}
\newcommand {\athr}    {{\hat{\rm a}_{\rm thrust}}}
\newcommand {\ththr}   {{\theta_{\rm thrust}}}
\newcommand {\acol}    {{\Phi_{\rm acol}}}
\newcommand {\acop}    {{\Phi_{\rm acop}}}
\newcommand {\acopt}   {{\Phi_{\rm acop_T}}}
\newcommand {\thpoint} {\theta_{\rm point}}
\newcommand {\thscat}  {\theta_{\rm scat}}
\newcommand {\etwelve} {E_{12\gradi}}
\newcommand {\ethirty} {E_{30\gradi}}
\newcommand {\eiso}[1] {E^{\, \triangleleft 30\gradi}_{#1}}
\newcommand {\phimiss} {{\phi_{\vec{p}_{\rm miss}}}}
\newcommand {\ewedge}  {E(\phi_{\vec{p}_{\rm miss}}\pm 15\gradi)}
%\newcommand {\ewedge}  {{E_{\rm w}}}
\newcommand {\evis}    {E_{\rm vis}}
\newcommand {\etot}    {E_{\rm vis}}
\newcommand {\emis}    {E_{\rm miss}}
\newcommand {\mvis}    {M_{\rm vis}}
\newcommand {\mtot}    {M_{\rm vis}}
\newcommand {\mmis}    {M_{\rm miss}}
\newcommand {\mhad}    {M^{\rm ex \, \ell_1}_{\rm vis}}
\newcommand {\mhadtwo} {M^{\rm ex \, \ell_1\ell_2}_{\rm vis}}
\newcommand {\ehad}    {E^{\rm NH}_{\rm vis}}
\newcommand {\epho}    {E^{\gamma}_{\rm vis}}
\newcommand {\echa}    {E^{\rm ch}_{\rm vis}}
\newcommand {\nch}     {{N_{\rm ch}}}
\newcommand {\elept}   {E_{\rm lept}}
\newcommand {\elepone} {E_{\ell _1}}
\newcommand {\eleptwo} {E_{\ell _2}}
\newcommand {\pvis}    {{\vec{p}_{\rm vis}}}
\newcommand {\pmis}    {{\vec{p}_{\rm miss}}}
\newcommand {\thmiss}  {{\theta_{\pmis}}}
\newcommand {\pt}      {{p_{\rm t}}}
\newcommand {\ptch}    {{p_{\rm t}^{\rm ch}}}
\newcommand {\pch}    {{p^{\rm ch}}}
\newcommand {\pz}      {{p_z}}
\newcommand {\ptnoNH}  {{p_{\rm t}^{\rm ex \, NH}}}
\newcommand {\puds}    {{P_{\rm uds}}}
%
\newcommand {\pmiss}   {{P\!\!\!\,\!/ }}
\newcommand {\emiss}   {{E\!\!\!\,\!/ }}
%
%
% no more of Christian's random capitalization!
% more of mine
\newcommand{\brchal}{\cal{B}($\PCha \rightarrow \ell\nu\PChi\ $)}
\newcommand{\M}{M_{2}}
\newcommand{\Mp}{M_{2}}
\newcommand{\sigbg}{\sigma_{\mathrm{bg}}}
\newcommand{\ww}   {\mathrm {WW}}
\newcommand{\zz}   {\mathrm Z\gamma^{*}}
\newcommand{\ewnu} {\mathrm{eW}\nu}
\newcommand{\eez}  {\mathrm {eeZ}}
\newcommand{\gagall}{{\gamma\gamma\rightarrow \ell\ell }}
\newcommand{\Pstaup}{{\widetilde{\tau}_{1}}}
\newcommand{\Pstaul}{{\widetilde{\tau}_{L}}}
\newcommand{\Pstaur}{{\widetilde{\tau}_{R}}}
\newcommand{\mzero}{m_{0}}
\newcommand{\msnu}{M_{\tilde{\nu}}}
\newcommand{\mcha}{M_{\chi^{\pm}}}
\newcommand{\mchi}{M_{\chi}}
\newcommand{\mstau}{M_{{\widetilde{\tau}_{1}}}}
\newcommand{\atau}{A_{\tau}}
\newcommand{\chsnu}{\PCha \rightarrow \ell \tilde{\nu}}
\newcommand{\chstau}{\PCha \rightarrow \tilde{\tau}_{1}\nu}
\newcommand{\chlep}{\PCha \rightarrow \ell\nu\chi}
\newcommand{\Tcsq}{\mathrm{TeV}/c^2}
% new for thesis
\newcommand{\nobs}{N_{\mathrm{obs}}}
\newcommand{\nlim}{N_{\mathrm{lim}}}
\newcommand{\Brl}{\cal{B}_{\ell}}
\newcommand{\leff} {\mathcal{L}_{\mathrm{eff}}}
\newcommand{\dedx}{{\mathrm{d}}E/{\mathrm{d}}x}
\newcommand{\chtau}{\PCha \rightarrow \tau\nu\chi}
\newcommand{\ssqtw}{\sin^{2}\theta_{\mathrm W}}
%\newcommand{\PSql}{\tilde{\mathrm q}_L}
%\newcommand{\PSqr}{\tilde{\mathrm q}_R}
%\newcommand{\PSq1}{\tilde{\mathrm q}_1}
%\newcommand{\PSq2}{\tilde{\mathrm q}_2}
%\newcommand{\ww}{{\mathrm WW}}
%\newcommand{\zz}{{\mathrm Z\gamma^{*}}}
%\newcommand{\eez}{{\mathrm eeZ}}
\newcommand{\nnz}{{\mathrm \nu\bar{\nu}Z}}
% added by bill
\def \ggll    {\gamma\gamma \rightarrow \ell^{+}{\ell}^{-}}
\def \tautau  {\mathrm \tau^{+}\tau^{-}}
\def \ffg  {f\bar{f}(\gamma)}
\def \lll   {\ell^{+}{\ell}^{-}}
\def \ww   {\mathrm WW}
\def \zz   {\mathrm Z\gamma^{*}}
\def \znn  {\mathrm Z\nu\nu}
\def \zee  {\mathrm Zee}
\def \rts  {\sqrt{s}}
\def \mstop {m_{\tilde{\mathrm{t}}}}
\def \msnu  {m_{\tilde{\nu}}}
\def \elow   {E_{12^{\circ}}}
\def \gev    { \, \mathrm{GeV}/\it{c}^{\mathrm{2}}}
\def \gvm    { \, \mathrm{GeV}/\it{c}}
\def \mx     {M_{\mathrm{eff}}} 
\newcommand{\neutr}{\chi}
%end fabio


%dalla mia pretesi

%\def \X             {\mathrm X} 
%\def \V             {\mathrm V} 
\def \Zcc           {\Z \to \charm \bar{\charm} }
\def \Zbb           {\Z \to \b \bar{\b} }
\def \decDS         {\D^{*+} \to \D^0 \pi^+}
\def \decsDS        {\D^{*+} \to \D^0 \pi^+_s}
\def \deckp         {\D^{0} \to \K^- \pi^+}
\def \deckppp       {\D^{0} \to \K^- \pi^+ \pi^+ \pi^-}
\def \deckpp        {\D^{0} \to \K^- \pi^+ \pi^0}
\def \deckpS        {\D^{0} \to \K^- \pi^+ (\pi^0)}
\def \decskp        {\D^{*+} \to \pi^{+}_{s} \K^- \pi^+}
\def \decskppp      {\D^{*+} \to \pi^{+}_{s} \K^- \pi^+ \pi^+ \pi^-}
\def \decskpp       {\D^{*+} \to \pi^{+}_{s} \K^- \pi^+ \pi^0}
\def \decskpS       {\D^{*+} \to \pi^{+}_{s} \K^- \pi^+ (\pi^0)}
\def \epsc          {\varepsilon_{\charm}}
\def \epsb          {\varepsilon_{\b}}
\def \pctod         {P_{\charm \to \D^*}}
\def \pbtod         {P_{\b \to \D^*}}
%\def \R             {{\mathrm R}}
\def \Gbb           {\Gamma_{\b\bar{\b}}}
\def \Gcc           {\Gamma_{\charm\bar{\charm}}}
\def \Gh            {\Gamma_{\mathrm h}}
%
% End of my macros
%
Revision:	1.3
Committed:	Thu May 14 12:41:54 2009 UTC (15 years, 11 months ago) by sguazz
Content type:	application/x-tex
Branch:	MAIN
CVS Tags:	HEAD
Changes since 1.2:	+3 -0 lines
Log Message:	Go...
#	User	Rev	Content
1	sguazz	1.1	%
2			% My Macros
3			%
4			% Macro declarations
5			%
6			%---- SLASH
7			\def\slasha#1{#1\hskip-0.65em /} %slasha per caratteri piccoli
8			\def\slashb#1{#1\hskip-1.3em /} %slashb per quelli grandi
9			\def\slashc#1{#1\hskip-.4em /}
10			%
11			%---- UNITA` DI MISURA
12			\def \pb {{\rm \, pb}}
13			\def \fb {{\rm \, fb}}
14			\def \ipb {{\rm \, pb^{-1}}}
15			\def \ifb {{\rm \, fb^{-1}}}
16			\def \eV {{\rm \, eV}}
17			\def \keV {{\rm \, keV}}
18			\def \MeV {{\rm \, MeV}}
19			\def \GeV {{\rm \, GeV}}
20			\def \TeV {{\rm \, TeV}}
21			\def \TeVc {\TeV/c}
22			\def \TeVcc {\TeV/c^2}
23			\def \GeVc {\GeV/c}
24			\def \GeVcc {\GeV/c^2}
25			\def \MeVc {\MeV/c}
26			\def \MeVcc {\MeV/c^2}
27			%
28			%---- SIMBOLI
29			\def\ga{\mathrel{\raise.3ex\hbox{$>$\kern-.75em\lower1ex\hbox{$\sim$}}}}
30			\def\la{\mathrel{\raise.3ex\hbox{$<$\kern-.75em\lower1ex\hbox{$\sim$}}}}
31			\newcommand {\lesssim}
32			{\,\raisebox{-0.6ex}{$\stackrel{\textstyle<}{\textstyle\sim}$}\,}
33			\newcommand {\gtrsim}
34			{\,\raisebox{-0.6ex}{$\stackrel{\textstyle>}{\textstyle\sim}$}\,}
35			\newcommand{\ckm}{$\checkmark$}
36			%
37			%---- MISCELLANEA
38			\newcommand {\slashed}[1] { \mbox{\rlap{\hbox{/}} #1 }}
39			\newcommand {\onehalf} {\raisebox{0.1ex}{${\frac{1}{2}}$}}
40			\newcommand {\fivethirds} {\raisebox{0.1ex}{${\frac{5}{3}}$}}
41			\newcommand {\OR} {{\tt OR}\,}
42			\newcommand {\BR} {{\rm BR}\,}
43			\newcommand {\rts} {\sqrt{s}}
44			\newcommand {\lumi} {\mathcal{L}}
45			\newcommand {\Lumi} {\int\lumi\mathrm{d}t}
46			\newcommand {\gradi} {^\circ}
47			\newcommand {\de} {\partial}
48			\newcommand {\um} {\, \mu \rm m}
49			\newcommand {\nm} {\rm \, nm}
50	sguazz	1.3	\newcommand {\mrad} {\rm \, mrad}
51	sguazz	1.1	\newcommand {\us} {\, \mu \rm s}
52			\newcommand {\cm} {\rm \, cm}
53			\newcommand {\mm} {\rm \, mm}
54			\newcommand {\mA} {\rm \, mA}
55			\newcommand {\muF} {\rm \, \mu F}
56	sguazz	1.3	\newcommand {\uV} {\rm \, \mu V}
57			\newcommand {\mV} {\rm \, mV}
58	sguazz	1.1	\newcommand {\m} {\rm \, m}
59			\newcommand {\km} {\rm \, km}
60			\newcommand {\V} {\rm \, V}
61			\newcommand {\T} {\rm \, T}
62			\newcommand {\kV} {\rm \, kV}
63			\newcommand {\kVm} {\rm \, kV\! / \! m}
64			\newcommand {\MVm} {\rm \, MV\! / \! m}
65			\newcommand {\MHz} {\rm \, MHz}
66	sguazz	1.2	\newcommand {\kHz} {\rm \, kHz}
67	sguazz	1.1	\newcommand {\ohm} {\, \Omega}
68			\newcommand {\ns} {\rm \, ns}
69			\newcommand {\ps} {\rm \, ps}
70			%
71			%---- THEORY groups & AOB
72			\newcommand {\gws} {\mathrm{SU(2)_L \otimes U(1)_Y}}
73			\newcommand {\sul} {\mathrm{SU(2)_L}}
74			\newcommand {\suc} {\mathrm{SU(3)_C}}
75			\newcommand {\ul} {\mathrm{U(1)_Y}}
76			\newcommand {\uem} {\mathrm{U(1)_{em}}}
77			\newcommand {\sigmabar} {\overline{\sigma}}
78			\newcommand {\gmunu} {g^{\mu \nu}}
79			\newcommand {\munu} {{\mu \nu}}
80			\newcommand {\obra} {\langle 0 \|}
81			\newcommand {\oket} {\| 0 \rangle}
82			%
83			%---- THEORY lepton fields
84			\newcommand {\LL} {L^{\alpha}_{\mathrm L}}
85			\newcommand {\LLd} {L^{\dagger \alpha}_{\mathrm L}}
86			\newcommand {\lL} {\ell^{\alpha}_{\mathrm L}}
87			\newcommand {\lLd} {\ell^{\dagger \alpha}_{\mathrm L}}
88			\newcommand {\ld} {\ell^{\dagger \alpha}}
89			\newcommand {\lb} {\overline{\ell}^{\alpha}}
90			\newcommand {\lR} {\ell^{\alpha}_{\mathrm R}}
91			\newcommand {\lRd} {\ell^{\dagger \alpha}_{\mathrm R}}
92			\newcommand {\nuL} {\nu^{\alpha}_{\mathrm L}}
93			\newcommand {\nuLb} {\overline{\nu}^{\alpha}_{\mathrm L}}
94			\newcommand {\nub} {\overline{\nu}^{\alpha}}
95			\newcommand {\lept} {\ell^\alpha}
96			\newcommand {\neut} {\nu^{\alpha}}
97			\newcommand {\nuLd} {\nu^{\dagger \alpha}_{\mathrm L}}
98			\newcommand {\Phid} {\Phi^\dagger}
99			%
100			%---- THEORY quark fields
101			\newcommand {\up} {u^{\alpha}}
102			\newcommand {\ub} {\overline{u}^{\alpha}}
103			\newcommand {\down} {d^{\alpha}}
104			\newcommand {\db} {\overline{d}^{\alpha}}
105			\newcommand {\QL} {Q^{\alpha}_{\mathrm L}}
106			\newcommand {\QLd} {Q^{\dagger \alpha}_{\mathrm L}}
107			\newcommand {\UL} {U^{\alpha}_{\mathrm L}}
108			\newcommand {\ULd} {U^{\dagger \alpha}_{\mathrm L}}
109			\newcommand {\UR} {U^{\alpha}_{\mathrm R}}
110			\newcommand {\URd} {U^{\dagger \alpha}_{\mathrm R}}
111			\newcommand {\DL} {D^{\alpha}_{\mathrm L}}
112			\newcommand {\DLd} {D^{\dagger \alpha}_{\mathrm L}}
113			\newcommand {\DR} {D^{\alpha}_{\mathrm R}}
114			\newcommand {\DRd} {D^{\dagger \alpha}_{\mathrm R}}
115			\newcommand {\bfell} {\ell\kern-0.4em
116			\ell\kern-0.4em
117			\ell\kern-0.4em
118			\ell }
119			\newcommand {\obfell} {\overline{\ell}\kern-0.4em
120			\overline{\ell}\kern-0.4em
121			\overline{\ell}\kern-0.4em
122			\overline{\ell}}
123			\newcommand {\bfH} {\, {\cal H}\kern-0.5em \kern-0.4em
124			{\cal H}\kern-0.5em \kern-0.4em
125			{\cal H}\kern0.1em }
126			\newcommand {\obfH} {\, \overline{\cal H}\kern-0.5em \kern-0.4em
127			\overline{\cal H}\kern-0.5em \kern-0.4em
128			\overline{\cal H}\kern0.1em }
129			%
130			%---- PARTICELLE
131			\def \b {{\mathrm b}}
132			\def \t {{\mathrm t}}
133			\def \charm {{\mathrm c}}
134			\def \d {{\mathrm d}}
135			\def \u {{\mathrm u}}
136			\def \e {{\mathrm e}}
137			\def \q {{\mathrm q}}
138			\def \g {{\mathrm g}}
139			\def \p {{\mathrm p}}
140			\def \s {{\mathrm s}}
141			\def \n {{\mathrm n}}
142			\def \h {{\mathrm h}}
143			\def \l {\ell}
144			\def \f {{\mathrm f}}
145			%\def \f {{f}}
146			\def \A {{\mathrm A}}
147			\def \B {{\mathrm B}}
148			\def \D {{\mathrm D}}
149			\def \K {{\mathrm K}}
150			\def \X {{\mathrm X}}
151			\def \Y {{\mathrm Y}}
152			\def \W {{\mathrm W}}
153			\def \H {{\mathrm H}}
154			\def \Z {{\mathrm Z}}
155			\def \S {{\mathrm S}}
156			\def \N {{\mathrm N}}
157			\def \L {{\mathrm L}}
158			\def \R {{\mathrm R}}
159			\def \P {{\mathrm P}}
160			\def \G {{\mathrm G}}
161			%
162			%---- Higgs
163			\newcommand {\ho} {{\h^0}}
164			\newcommand {\Ho} {{\H^0}}
165			\newcommand {\Ao} {{\A^0}}
166			\newcommand {\Hpm} {{\H^\pm}}
167			\newcommand {\clsb} {{\mathrm CL_{\rm s+b}}}
168			\newcommand {\clb} {{\mathrm CL_{\rm b}}}
169			%
170			%---- SUSY
171			\newcommand {\dm} {\Delta m}
172			\newcommand {\dM} {\Delta M}
173			\newcommand {\ldm} {\mbox{``low $\dm$''}}
174			\newcommand {\hdm} {\mbox{``high $\dm$''}}
175			\newcommand {\nnc} {{\overline{\mathrm N}_{95}}}
176			\newcommand {\snc} {{\overline{\sigma}_{95}}}
177			\newcommand {\susy} {{supersymmetry}}
178			\newcommand {\susyc} {{supersymmetric}}
179			\newcommand {\aj} {\mbox{\sf AJ}}
180			\newcommand {\ajl} {\mbox{\sf AJL}}
181			\newcommand {\llh} {\mbox{\sf LLH}}
182			%
183			%---- SPARTICELLE
184			\newcommand {\rpc} {{\rm RPC}}
185			\newcommand {\rpv} {{\rm RPV}}
186			\newcommand {\sfe} {{\tilde{\f}}}
187			\newcommand {\sfL} {{\tilde{\f}_{\mathrm L}}}
188			\newcommand {\sfR} {{\tilde{\f}_{\mathrm R}}}
189			\newcommand {\sfone} {{\tilde{\f}_{1}}}
190			\newcommand {\sftwo} {{\tilde{\f}_{2}}}
191			\newcommand {\sneu} {{\tilde{\nu}}}
192			\newcommand {\wino} {{\mathrm{\widetilde{W}}}}
193			\newcommand {\bino} {{\mathrm{\widetilde{B}}}}
194			\newcommand {\se} {{\mathrm{\tilde{e}}}}
195			\newcommand {\seR} {{\mathrm{\tilde{e}_{R}}}}
196			\newcommand {\seL} {{\mathrm{\tilde{e}_{L}}}}
197			\newcommand {\st} {{\mathrm{\tilde{\tau}}}}
198			\newcommand {\stR} {{\mathrm{\tilde{\tau}_{R}}}}
199			\newcommand {\stL} {{\mathrm{\tilde{\tau}_{L}}}}
200			\newcommand {\stone} {{\mathrm{\tilde{\tau}_{1}}}}
201			\newcommand {\sttwo} {{\mathrm{\tilde{\tau}_{2}}}}
202			\newcommand {\sm} {{\mathrm{\tilde{\mu}}}}
203			\newcommand {\smR} {{\mathrm{\tilde{\mu}_{R}}}}
204			\newcommand {\smL} {{\mathrm{\tilde{\mu}_{L}}}}
205			\newcommand {\Sup} {{\mathrm{\tilde{u}}}}
206			\newcommand {\suR} {{\mathrm{\tilde{u}_{R}}}}
207			\newcommand {\suL} {{\mathrm{\tilde{u}_{L}}}}
208			\newcommand {\sdo} {{\mathrm{\tilde{d}}}}
209			\newcommand {\sdR} {{\mathrm{\tilde{d}_{R}}}}
210			\newcommand {\sdL} {{\mathrm{\tilde{d}_{L}}}}
211			\newcommand {\sch} {{\mathrm{\tilde{c}}}}
212			\newcommand {\scR} {{\mathrm{\tilde{c}_{R}}}}
213			\newcommand {\scL} {{\mathrm{\tilde{c}_{L}}}}
214			\newcommand {\sst} {{\mathrm{\tilde{s}}}}
215			\newcommand {\ssR} {{\mathrm{\tilde{s}_{R}}}}
216			\newcommand {\ssL} {{\mathrm{\tilde{s}_{L}}}}
217			\newcommand {\stopR} {{\tilde{\mathrm{t}}_{R}}}
218			\newcommand {\stopL} {{\tilde{\mathrm{t}}_{L}}}
219			\newcommand {\stopone} {{\tilde{\mathrm{t}}_{1}}}
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}}}}
224			\newcommand {\glu} {{\mathrm{\tilde{g}}}}
225			\newcommand {\sbotR} {{\mathrm{\tilde{b}_{R}}}}
226			\newcommand {\sbotL} {{\mathrm{\tilde{b}_{L}}}}
227			\newcommand {\sbotone} {{\mathrm{\tilde{b}_{1}}}}
228			\newcommand {\sbottwo} {{\mathrm{\tilde{b}_{2}}}}
229			\newcommand {\sbot} {{\tilde{\mathrm{b}}}}
230			\newcommand {\squa} {{\tilde{\mathrm{q}}}}
231			\newcommand {\squal} {{\tilde{\mathrm{q}}_{\rm L}}}
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}}}}
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			%