Statistical correlation coefficients for double-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet invariant mass ($m_{1,2}$) and the absolute rapidity of the outermost jet ($\left| y \right|_\text{max}$)

Double-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$) and the absolute rapidity of the outermost jet ($\left| y \right|_\text{max}$)

Electroweak corrections to double-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$) and the absolute rapidity of the outermost jet ($\left| y \right|_\text{max}$)

Nonperturbative corrections to double-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$) and the absolute rapidity of the outermost jet ($\left| y \right|_\text{max}$)

Statistical correlation coefficients for double-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$) and the absolute rapidity of the outermost jet ($\left| y \right|_\text{max}$)

Triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Electroweak corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Nonperturbative corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Statistical correlation coefficients for triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Electroweak corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Nonperturbative corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Statistical correlation coefficients for triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet invariant mass ($m_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Electroweak corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Nonperturbative corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Statistical correlation coefficients for triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.4 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Electroweak corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Nonperturbative corrections to triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Statistical correlation coefficients for triple-differential dijet cross section for anti-$k_\text{T}$ jets with R = 0.8 as a function of the dijet average transverse momentum ($\langle p_\text{T} \rangle_{1,2}$), the total boost of dijet system ($y_\text{b}$), and the absolute rapidity separation of the two jets ($y^*$)

Numerical results of $b \bar{b}$- and $c \bar{c}$-dijet cross-sections, $c \bar{c}$/$b \bar{b}$ dijet cross-section ratios and their total uncertainties as a function of the leading jet $p_T$.

Numerical results of $b \bar{b}$- and $c \bar{c}$-dijet cross-sections, $c\bar{c}$/$b \bar{b}$ dijet cross-section ratios and their total uncertainties as a function of $m_{jj}$ (dijet invariant mass).

Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet eta intervals of the $b \bar{b}$-dijet differential cross sections. The unit of all the elements of the matrix is nb$^2$.

Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet eta intervals of the $c \bar{c}$-dijet differential cross sections. The unit of all the elements of the matrix is nb$^2$.

Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet $\eta$ intervals of the $b \bar{b}$ (horizontal) and $c \bar{c}$ (vertical) differential cross sections. The unit of all the elements of the matrix is nb$^2$.

Covariance matrix, corresponding to the total uncertainties, obtained between the $\Delta y^*$ intervals of the $b \bar{b}$-dijet differential cross sections. The unit of all the elements of the matrix is nb$^2$.

Covariance matrix, corresponding to the total uncertainties, obtained between the $\Delta y^*$ intervals of the $c \bar{c}$-dijet differential cross sections. The unit of all the elements of the matrix is nb$^2$.

Covariance matrix, corresponding to the total uncertainties, obtained between the $\Delta y^*$ intervals of the $b \bar{b}$ (horizontal) and $c \bar{c}$ (vertical) differential cross sections. The unit of all the elements of the matrix is nb$^2$.

Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet $p_T$ intervals of the $b \bar{b}$-dijet differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c)^2$ and the $p_T$ intervals are given in GeV$/c$.

Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet $p_T$ intervals of the $c \bar{c}$-dijet differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c)^2$ and the $p_T$ intervals are given in GeV$/$c .

Covariance matrix, corresponding to the total uncertainties, obtained between the leading jet $p_T$ intervals of the $b \bar{b}$ (horizontal) and $c \bar{c}$ (vertical) differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c)^2$ and the $p_T$ intervals are given in GeV$/c$.

Covariance matrix, corresponding to the total uncertainties, obtained between the $m_{jj}$ intervals of the $b \bar{b}$-dijet differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c^2)^2$ and the mass intervals are given in GeV$/c^2$.

Covariance matrix, corresponding to the total uncertainties, obtained between the $m_{jj}$ intervals of the $c \bar{c}$-dijet differential cross sections. The unit of all the elements of the matrix is (nb GeV$/c^2)^2$ and the mass intervals are given in GeV$/c^2$.

Covariance matrix, corresponding to the total uncertainties, obtained between the $m_{jj}$ intervals of the $b \bar{b}$ (horizontal) and $c \bar{c}$ (vertical) differential cross sections. The unit of all the elements of the matrix is $($nb GeV$/c^2)^2$ and the mass intervals are given in GeV$/c^2$.

Ratio of unfolded width of azimuthal angular correlation distributions (P PB/ P P). Different colors correspond to different combinations of p_{T,1} and p_{T,2}

Ratio of unfolded Dijet conditional yields (P PB/ P P). Different colors correspond to different combinations of p_{T,1} and p_{T,2}

Unfolded width of azimuthal angular correlation distributions (Delta p_{T} > 3). Full markers represent p+Pb, open markers p+p

Unfolded Dijet conditional yields (Delta p_{T} > 3). Full markers represent p+Pb, open markers p+p

Ratio of unfolded width of azimuthal angular correlation distributions (P PB/ P P) (Delta p_{T} > 3). Different colors correspond to different combinations of p_{T,1} and p_{T,2}

Ratio of unfolded Dijet conditional yields (P PB/ P P) (Delta p_{T} > 3). Different colors correspond to different combinations of p_{T,1} and p_{T,2}

Unfolded azimuthal angular correlation distributions. Black markers represent p+Pb, red markers p+p

Unfolded azimuthal angular correlation distributions (Delta p_{T} > 3). Black markers represent p+Pb, red markers p+p