adaptation_specialization_material/output/etm_20_pretrained/top_change.tex

\begin{table}[H]
\centering
\caption{Physicists with the highest change scores $c_a$. $D(\bm{I_a})$ and $D(\bm{S_a})$ measure the diversity of intellectual and social capital. Numbers in parentheses indicate the share of attention dedicated to each research area during each time-period. Asterisks ($\ast$) indicate physicists with a permanent position.}
\label{table:top_change}
\begin{tabular}{p{0.15\textwidth}|c|c|c|b{0.25\textwidth}|b{0.25\textwidth}}
\toprule
               Physicist & $c_a$ & $D(\bm{I_a})$ & $D(\bm{S_a})$ &                            Previous main area &                               Current main area \\
\midrule
                T.~Fuchs &  0.93 &          4.38 &          6.50 &                           QCD (0.53$\to$0.00) & Neutrinos \& flavour physics (0.00$\to$0.64)\\ \hline
  N.~G.~Sanchez ($\ast$) &  0.88 &          7.52 &         13.08 &                   Black holes (0.37$\to$0.03) &                  Dark matter (0.00$\to$0.57)\\ \hline
  V.~V.~Braguta ($\ast$) &  0.88 &          5.03 &          8.04 &                       Hadrons (0.45$\to$0.00) &                          QCD (0.05$\to$0.60)\\ \hline
  G.~B.~Cleaver ($\ast$) &  0.83 &          6.34 &         12.22 & String theory \& supergravity (0.40$\to$0.00) &                    Cosmology (0.03$\to$0.62)\\ \hline
      J.~Martin Camalich &  0.82 &          2.34 &          4.57 &                           QCD (0.78$\to$0.03) &                      Hadrons (0.06$\to$0.38)\\ \hline
 Kwei Chou Yang ($\ast$) &  0.81 &          3.58 &          7.80 &                       Hadrons (0.63$\to$0.03) &                  Dark matter (0.00$\to$0.78)\\ \hline
     S.~D.~Katz ($\ast$) &  0.80 &          6.50 &         10.85 &                   Dark matter (0.42$\to$0.03) &                          QCD (0.06$\to$0.47)\\ \hline
    G.~Ferretti ($\ast$) &  0.78 &          5.22 &          6.18 & String theory \& supergravity (0.52$\to$0.00) &           Electroweak sector (0.01$\to$0.58)\\ \hline
         K.~Bhattacharya &  0.78 &         10.79 &         10.59 &  Neutrinos \& flavour physics (0.20$\to$0.00) &                    Cosmology (0.09$\to$0.37)\\ \hline
     H.~Ebrahim ($\ast$) &  0.78 &          3.90 &          6.81 &                   Black holes (0.44$\to$0.06) &                      AdS/CFT (0.02$\to$0.34)\\ \hline
              K.~Narayan &  0.77 &          3.83 &          7.13 & String theory \& supergravity (0.62$\to$0.00) &                      AdS/CFT (0.03$\to$0.52)\\ \hline
        Mario Campanelli &  0.77 &          2.04 &          4.48 &  Neutrinos \& flavour physics (0.79$\to$0.06) &           Electroweak sector (0.09$\to$0.64)\\ \hline
V.~K.~Oikonomou ($\ast$) &  0.76 &          8.05 &          6.18 &                Thermodynamics (0.24$\to$0.02) &                    Cosmology (0.00$\to$0.47)\\ \hline
               K.~Sasaki &  0.76 &          3.14 &          8.87 &              Collider physics (0.68$\to$0.06) &               Thermodynamics (0.00$\to$0.27)\\ \hline
 H.~L.~Verlinde ($\ast$) &  0.74 &          5.32 &          8.88 & String theory \& supergravity (0.60$\to$0.04) &                      AdS/CFT (0.02$\to$0.35)\\ \hline
                  Bin Wu &  0.74 &          5.02 &          8.01 &                           QCD (0.41$\to$0.02) &             Collider physics (0.15$\to$0.56)\\ \hline
    Eiji Nakano ($\ast$) &  0.74 &          6.90 &         10.13 &                           QCD (0.39$\to$0.06) &                      Hadrons (0.04$\to$0.78)\\ \hline
   A.~T.~Suzuki ($\ast$) &  0.73 &          4.36 &          6.43 &          Perturbative methods (0.61$\to$0.04) & Neutrinos \& flavour physics (0.01$\to$0.39)\\ \hline
             A.~Mariotti &  0.73 &          3.81 &          4.91 & String theory \& supergravity (0.63$\to$0.01) &           Electroweak sector (0.01$\to$0.38)\\ \hline
              I.~Scimemi &  0.73 &          6.77 &          8.60 &                       Hadrons (0.36$\to$0.00) &             Collider physics (0.09$\to$0.81)\\ \hline
\bottomrule
\end{tabular}
\end{table}