for different values of the exponent $\lambda$ a) $\lambda=0$, b) $\lambda=0.2$, c) $\lambda=0.27$ and d) $\lambda=0.3$.[]{data-label="ratiosmT"}](Alice_RmT_000.pdf "fig:") ![Illustration of geometrical scaling in scaling variable $\tau_{\tilde{m}_{\rm T}}$. Multiplicity ratios $R_{W_{1}/W_{2}}$ for $W_{1}=7$ TeV are plotted as functions of scaling variable $\tau_{\tilde{m_{\rm T}}}$ for pions (red triangles: “up” for $W_{2}
=2.76$ TeV, “down” for $W_{2}=0.9$ TeV) kaons (blue triangles: “right” for $W_{2} =2.76$ TeV, “left” for $W_{2}=0.9$ TeV) and protons (back circles for $W_{2} =2.76$ TeV and black squares $W_{2}=0.9$ TeV) for different values of the exponent $\lambda$ a) $\lambda=0$, b) $\lambda=0.2$, c) $\lambda=0.27$ and d) $\lambda=0.3$.[]{data-label="ratiosmT"}](Alice_RmT_020.pdf "fig:")\
![Illustration of geometrical scaling in scaling variable $\tau_{\tilde{m}_{\rm T}}$. Multiplicity ratios $R_{W_{1}/W_{2}}$ for $W_{1}=7$ TeV are plotted as functions of scaling variable $\tau_{\tilde{m_{\rm T}}}$ for pions (red triangles: “up” for $W_{2}
=2.76$ TeV, “down” for $W_{2}=0.9$ TeV) kaons (blue triangles: “right” for $W_{2} =2.76$ TeV, “left” for $W_{2}=0.9$ TeV) and protons (back circles for $W_{2} =2.76$ TeV and black squares $W_{2}=0.9$ TeV) for different values of the exponent $\lambda$ a) $\lambda=0$, b) $\lambda=0.2$, c) $\lambda=0.27$ and d) $\lambda=0.3$.[]{data-label="ratiosmT"}](Alice_RmT_027.pdf "fig:") ![Illustration of geometrical scaling in scaling variable $\tau_{\tilde{m}_{\rm T}}$. Multiplicity ratios $R_{W_{1}/W_{2}}$ for $W_{1}=7$ TeV are plotted as functions of scaling variable $\tau_{\tilde{m_{\rm T}}}$ for 