TABLE I: Chemical compositions, hole concentration p , T$_{c}$ , T$_{min}$ and ρ$_{min}$ of Bi2212 samples studied in the present work. Bi$_{2}$Sr$_{2}$$_{−}$$_{x}$La$_{x}$CaCu$_{2}$O$_{8+}$$_{δ}$ p T$_{c}$ (K) T$_{min}$ (K) ρ$_{min}$ (mΩcm) x = 0 . 8 0.03 - 150 5 x = 0 . 7 0.05 - 130 3.2 x = 0 . 6 0.06 - - - Bi$_{2}$Sr$_{2}$Ca$_{0}$$_{.}$$_{8}$Y$_{0}$$_{.}$$_{2}$Cu$_{2}$O$_{8+}$$_{δ}$ 0.075 30 - - -1.0 0 -1.0 0 -1.0 0 -1.0 0 0.6 0.5 0.4 0.3 0.6 0.5 0.4 0.3 0.6 0.5 0.4 0.3 -1.2 -1.0 -0.8 -0.6 -0.4 -0.2 0.0 0.2 0.6 0.5 0.4 0.3 p  = 0.03 p  = 0.05 p  = 0.06 p  = 0.075 Bi$_{2}$(Sr,La)$_{2}$(Ca,Y)Cu$_{2}$O$_{8+}$ Energy relative to  E$_{F}$  (eV) Energy relative to  E F  (eV) k$_{x}$  =  k$_{y}$ = 0.3 k$_{x}$  =  k$_{y}$ = 0.65 k$_{x}$  =  k$_{y}$  ( /a) SS MB SS MB SS MB SS MB SS MB SS MB SS MB SS MB p  = 0.03 p  = 0.05 p  = 0.06 p  = 0.075 high low (e) (a) (b) (c) (d) (f) (g) (h) FIG. 1: ARPES spectra of lightly-doped Bi2212 along the (0,0)-( π, π ) nodal direction in the second BZ. (a)-(d): EDCs. A bold line for each doping indicates the spectrum where the dispersive feature comes closest to E$_{F}$ . (e)-(h): Intensity plot of the spectra in the E - k plane. The features denoted by SS are diffraction replica of the main band ( MB ) due to the Bi-O plane superstructure. 10