Consider the circuit below from Chapter 3.3 of Analysis and Design of Analog Integrated Circuits by Gray, Hurst, Meyer, and Lewis (the genesis of this question is my trying to understand whether this amplifier is bilateral or unilateral). Note that \$i_o\$ seems to be placed oddly within the amplifier. I will leave that as drawn and call \$i_2 \$ the current draw into the amplifier as a whole, as per the convention with y-parameter calculations. I'll likewise call \$i_i =: i_1\$, \$v_i =: v_1\$, \$v_o =: v_2\$.
To find \$y_{12} := \frac{i_1}{v_2} \rvert_{v_1 = 0}\$ I'll set \$v_1 = 0\$. From this I obtain by KCL at Node 1 that $$\frac{v_e}{r_e || r_b} = g_mv_e \,\,\,\,\,\,\,\, [1]$$ By KCL at the output node we find that $$g_mv_e + i_2 = v_2/R_c.$$
Further, we obviously have $$i_1 = -v_e/r_e.$$ Now I can't seem to get rid of \$i_2\$ in this calculation. It appears that if I do take \$v_e = 0\$ then I get a consistent solution (and then \$y_{12} = 0\$), but I can't convince myself of why I should have to choose that rather than prove it. Any help would be greatly appreciated.
*Edit: Should the argument be that since $$ \frac{1/g_m}{r_e || r_b} =\frac{r_e+r_b}{g_mr_er_b} = \frac{\alpha_0/g_m+r_b}{\alpha_0r_b} = \frac{1/g_m + r_b/\alpha_0}{r_b} = 1/\alpha_0 + \frac{1}{g_mr_b} > 1 + \frac{1}{g_mr_b} \neq 1 $$ so that equation \$[1]\$ above demands \$v_e = 0\$. Is there an easier way to see this argument?