\newcommand{\pvdisqsqI}{1.085}
\newcommand{\pvdisqsqII}{1.901}
\newcommand{\pvdisDqsqI}{0.008} % Q2 uncertainties
\newcommand{\pvdisDqsqII}{0.012}
\newcommand{\pvdisXbjI}{0.241}
\newcommand{\pvdisXbjII}{0.295}

\newcommand{\pvdisASMI}{-92.05\pm 0.15} % SM estimation of Apv, MRST2006nnlo + CTEQ6M
\newcommand{\pvdisASMHTI}{-91.19\pm 0.18} % SM estimation of Apv with HT correction
\newcommand{\pvdisASMII}{-161.64\pm 0.07} 
\newcommand{\pvdisASMHTII}{-160.50\pm 0.21} 


%experimental and corrections to asymmetries
\newcommand{\pvdisExpNpairI}{0.93\times 10^7} % number of helicity pairs for e- DIS % Kais entry #102
\newcommand{\pvdisExpNpairII}{2.3\times 10^7} % number of helicity pairs for e- DIS
\newcommand{\pvdisExpABI}{xxx} % asym of beam intensity in ppm
\newcommand{\pvdisExpABE}{xxx} % asym of beam energy in ppm
\newcommand{\pvdisExpABP}{xxx} % asym of beam position in nm
\newcommand{\pvdisExpPbM}{(88.5\pm 1.8)\%} %Beam polarization from Moller
\newcommand{\pvdisExpPbC}{(90.2\pm 1.8)\%} %Beam polarization from Compton
\newcommand{\pvdisExpEeff}{95\%} % DAQ electron efficiency
\newcommand{\pvdisExpPirej}{xxx} % DAQ pion rejection

\newcommand{\pvdisExpDTI}{(3.0\pm 0.6)\%} % DAQ deadtime correction in %
\newcommand{\pvdisExpDTII}{(1.0\pm 0.2)\%} % DAQ deadtime correction in %

\newcommand{\pvdisExpPiI}{(3.5\pm 0.1)\times 10^{-4}} % correction to asymmetry due to pion dilution
\newcommand{\pvdisExpPiII}{(1.5\pm 0.1)\times 10^{-4}}
\newcommand{\pvdisExpPosI}{xxx} % correction to asymmetry due to pair production (positron)
\newcommand{\pvdisExpPosII}{xxx}

\newcommand{\pvdisExpRCI}{xxx\pm xxx} % radiative corrections to asymmetry
\newcommand{\pvdisExpRCII}{xxx\pm xxx} 

\newcommand{\pvdisExpAlI}{(0.02\pm 0.20)\%} %correction to Apv due to Al endcaps, in ppm
\newcommand{\pvdisExpAlII}{(0.02\pm 0.20)\%}

%final results, pions
\newcommand{\pvdisApiI}{xxx} % final result pion Apv low Q2
\newcommand{\pvdisApiII}{xxx} % final result pion Apv high Q2
\newcommand{\pvdisdApiStatI}{xxx} % final result pion Apv low Q2
\newcommand{\pvdisdApiStatII}{xxx} % final result pion Apv high Q2
\newcommand{\pvdisdApiSystI}{xxx} % final result pion Apv low Q2
\newcommand{\pvdisdApiSystII}{xxx} % final result pion Apv high Q2

%final results, others
\newcommand{\pvdisATI}{26.9 \pm 15.7}
\newcommand{\pvdisATII}{11.8 \pm 49.8}

%final results, electrons
\newcommand{\pvdisArawI}{xxx} % raw A low Q2
\newcommand{\pvdisArawII}{xxx} % raw A high Q2
\newcommand{\pvdisApvI}{xxx} % final result Apv low Q2
\newcommand{\pvdisApvII}{xxx} % final result Apv high Q2

\newcommand{\pvdisCI}{xxx} % final result 2C2u-C2d low Q2
\newcommand{\pvdisCII}{xxx} % final results 2C2u-C2d high Q2
\newcommand{\pvdisCSM}{xxx} % Standard Model expectation
\newcommand{\pvdisCdevI}{xxx} % Deviation of C2 from SM value
\newcommand{\pvdisCdevII}{xxx} %  Deviation of C2 from SM value
\newcommand{\pvdisHT}{xxx\%} % HT correction extracted from low Q2 result

%statistical uncertainty
\newcommand{\pvdisDArawStatI}{xxx}
\newcommand{\pvdisDArawStatII}{xxx}
\newcommand{\pvdisDApvStatI}{xxx}
\newcommand{\pvdisDApvStatII}{xxx}
\newcommand{\pvdisDCStatI}{xxx}
\newcommand{\pvdisDCStatII}{xxx}

%systematical uncertainty
\newcommand{\pvdisDApvSystI}{xxx}
\newcommand{\pvdisDApvSystII}{xxx}
\newcommand{\pvdisDCSystI}{xxx}
\newcommand{\pvdisDCSystII}{xxx}
\newcommand{\pvdisDCModI}{xxx}
\newcommand{\pvdisDCModII}{xxx}


\newcommand{\pvdis}{xxx}

%
