| * SKY130 Spice File. |
| .param sky130_fd_pr__res_high_po__slope_spectre = 0.0 |
| .param sky130_fd_pr__res_high_po__con_slope_spectre = 0.0 |
| * statistics { |
| * mismatch { |
| * vary sky130_fd_pr__res_high_po__slope_spectre dist=gauss std=1.0 |
| * vary sky130_fd_pr__res_high_po__con_slope_spectre dist=gauss std=1.0 |
| * } |
| * process { |
| * vary sky130_fd_pr__res_xhigh_po__var_mult dist=gauss std=0.025 |
| * vary sky130_fd_pr__res_high_po__var dist=gauss std=0.025 |
| * } |
| * } |
| .subckt sky130_fd_pr__model__parasitic__res_po r0 r1 sub |
| + w=1 l=1 |
| c0 r0 sub c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_1_1*1e-6)/2} |
| c1 r1 sub c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_1_1*1e-6)/2} |
| .ends sky130_fd_pr__model__parasitic__res_po |
| .subckt sky130_fd_pr__res_xhigh_po r0 r1 sub |
| + w=1 l=1 |
| .param mult = 1.0 |
| + rsheet = 2000.0 |
| + rend_mm = {0.0472/sqrt(w)} |
| + leff = {l-0.0592} |
| + weff = {w-0.056} |
| * $ Resistor voltco fitting parameters |
| + bp2 = -0.1228 |
| + bq2 = 1.304 |
| + bp22 = -0.2874 |
| + bp23 = 0.5252 |
| * $ Substrate voltco fitting parameters |
| + sub1 = 1.2 |
| + sub2 = 41.26e-3 |
| + sub3 = 8.697e-3 |
| + sub4 = 24.0 |
| + sub5 = 39.86 |
| + body_pelgrom = 0.0347 |
| + res_match = {(body_pelgrom/sqrt(w*l*mult))*sky130_fd_pr__res_high_po__slope_spectre} |
| + rhead0 = {188.2/(weff-0.0672*max(0.69-w,0)+1.41)} |
| + rbody0 = {rsheet*leff/(weff-0.0672*max(0.69-w,0))} |
| + rhead = {rhead0*(1+sky130_fd_pr__res_xhigh_po__var_mult)*(1+rend_mm/sqrt(mult)*sky130_fd_pr__res_high_po__con_slope_spectre)} |
| + rbody = {rbody0*(1+sky130_fd_pr__res_xhigh_po__var_mult)*(1+res_match)} |
| + Efac = {1/leff*(1+bp22/w+bp23*min(0.2,leff-0.5)*log(leff/w))} |
| rend1 r0 t1 reshead r = {rhead} |
| rend2 t2 r1 reshead r = {rhead} |
| xc0 r0 r1 sub sky130_fd_pr__model__parasitic__res_po w = {w} l = {l} |
| rbody t1 t2 resbody r = {rbody*(1-bp2+bp2*sqrt(1+(bq2*abs(v(t1,t2))*Efac)**2))*} |
| + (sub1+sub2*tanh(sub3*(min(v(b,r1)+v(b,r2),sub4)+sub5)))=1 /=1 (sub1+sub2*tanh(sub3*sub5))=1 |
| .model resbody r |
| .param tc1 = {-1.47e-3-5e-7*sky130_fd_pr__res_xhigh_po__var_mult*rsheet} tc2 = 2.7e-6 tnom = 25.0 |
| .model reshead r tc1 = -4.3e-4 tc2 = -1.3e-5 tnom = 25.0 |
| .ends sky130_fd_pr__res_xhigh_po |
| .subckt sky130_fd_pr__res_high_po r0 r1 b |
| + w=1 l=1 |
| .param mult = 1.0 |
| + rsheet = 317.3885 |
| + rbody_dw = -0.001 |
| + rhead_ps = 345.8312 |
| + mm_const = {(w<0.69)?0.1:0.2} |
| + body_pelgrom = 0.03552 |
| + head_pelgrom = 0.0761 |
| + num_con_row = {max(round((w-0.33)/0.36),1)} |
| + rbody_match = {body_pelgrom/sqrt(w*l*mult)*sky130_fd_pr__res_high_po__slope_spectre} |
| + rend_match = {head_pelgrom/sqrt((w+0.525)*num_con_row*mult)*sky130_fd_pr__res_high_po__con_slope_spectre} |
| + weff = {w+rbody_dw-0.0672*max(0.69-w,0)} |
| + leff = {l+0.247} |
| + res_match = {(body_pelgrom/sqrt(w*l*mult))*sky130_fd_pr__res_high_po__slope_spectre} |
| rhead r0 rb rhead_model w = {weff+0.1558} l = 1.0 |
| rbody rb r1 rbody_model w = {weff} l = {leff} |
| xc0 r0 r1 b sky130_fd_pr__model__parasitic__res_po w = {w} l = {l} |
| .model rhead_model r2 sw_et = {no} isnoisy = {no} |
| + rsh = {345.8312*(1+sky130_fd_pr__res_high_po__var)*(1+rend_match)} |
| + p2 = {-80.87e-3/cosh(6.34e-3*} $ weff*weff)*(1-exp(-1.554/leff)) |
| + q2 = {10.13/cosh(0.0898*weff*weff)} |
| + tc1 = -4.3e-4 tc2 = 12e-6 tnom = 30.0 |
| .model rbody_model r2 sw_et = {no} isnoisy = {no} |
| + rsh = {rsheet*(1+sky130_fd_pr__res_high_po__var)*(1+res_match)} |
| + p2 = {(w>0.6)?130.8e3*(1-exp(-1.818e-3*leff/weff))-867.4/weff+2236*weff/leff:300*(1-exp(-0.1124*leff/weff))+304.8*weff/leff} |
| + q2 = {(w>0.6)?6.11*(1-exp(-852.8e-6*leff/weff))+1.375e-3*weff:0.5*0.3155*(1-exp(-0.05518*leff/weff))+1.19E-05*weff} |
| + p3 = {(w>0.6)?380.3*weff/leff:0} |
| + q3 = {(w>0.6)?42.62e-3*weff/leff:0} |
| + tc1 = {tc1rpolybody} tc2 = {tc2rpolybody} tnom = 30.0 |
| .ends sky130_fd_pr__res_high_po |
| .subckt sky130_fd_pr__res_xhigh_po_0p35 r0 r1 b |
| + |
| .param w = 0.35 l = 5 mult = 1.0 |
| sky130_fd_pr__res_xhigh_po_0p35 r0 r1 b sky130_fd_pr__res_xhigh_po__base w = {w} l = {l} mult = {mult} |
| .ends sky130_fd_pr__res_xhigh_po_0p35 |
| .subckt sky130_fd_pr__res_xhigh_po_0p69 r0 r1 b |
| + |
| .param w = 0.69 l = 5 mult = 1.0 |
| sky130_fd_pr__res_xhigh_po_0p69 r0 r1 b sky130_fd_pr__res_xhigh_po__base w = {w} l = {l} mult = {mult} |
| .ends sky130_fd_pr__res_xhigh_po_0p69 |
| .subckt sky130_fd_pr__res_xhigh_po_1p41 r0 r1 b |
| + |
| .param w = 1.41 l = 5 mult = 1.0 |
| sky130_fd_pr__res_xhigh_po_1p41 r0 r1 b sky130_fd_pr__res_xhigh_po__base w = {w} l = {l} mult = {mult} |
| .ends sky130_fd_pr__res_xhigh_po_1p41 |
| .subckt sky130_fd_pr__res_xhigh_po_2p85 r0 r1 b |
| + |
| .param w = 2.85 l = 5 mult = 1.0 |
| sky130_fd_pr__res_xhigh_po_2p85 r0 r1 b sky130_fd_pr__res_xhigh_po__base w = {w} l = {l} mult = {mult} |
| .ends sky130_fd_pr__res_xhigh_po_2p85 |
| .subckt sky130_fd_pr__res_xhigh_po_5p73 r0 r1 b |
| + |
| .param w = 5.73 l = 5 mult = 1.0 |
| sky130_fd_pr__res_xhigh_po_5p73 r0 r1 b sky130_fd_pr__res_xhigh_po__base w = {w} l = {l} mult = {mult} |
| .ends sky130_fd_pr__res_xhigh_po_5p73 |
| .subckt sky130_fd_pr__res_xhigh_po__base r1 r2 b |
| + |
| + w=1 l=1 mult=1 |
| + |
| .param rsheet = 2000.0 |
| + vc1_body = -1.00e-3 |
| + vc2_body = -1.00e-4 |
| + vc1_raw_end = -2.02e-2 |
| + vc2_raw_end = 1.55e-1 |
| + vc3_raw_end = 4.61e-2 |
| + body_pelgrom = 0.0347 |
| + r0_var = {17.23/w+2.318} |
| + r1_var = {11.76/w} |
| + rcon = {-46.62/(w*w)+331.73/w+20.576} |
| + rend_mm = {0.0472/sqrt(w)} |
| + tc1_voltco = -7.1e-3 |
| + rend_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2)*r0_var} |
| + rtot_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2*pow(r0_var,2)+pow((r1_var*l),2))} |
| + res_match = {(body_pelgrom/sqrt(w*l*mult))*sky130_fd_pr__res_high_po__slope_spectre} |
| + rbody_var = {rtot_var-rend_var} |
| + rend = {(rcon+rend_var)*(1+rend_mm/sqrt(mult)*sky130_fd_pr__res_high_po__con_slope_spectre)} |
| + vc1_end = {vc1_raw_end/pwr(l,0.5)*(1+tc1_voltco*(temp-30))} |
| + vc2_end = {vc2_raw_end/pwr(l,0.5)*(1+tc1_voltco*(temp-30))} |
| + vc3_end = {vc3_raw_end/pwr(l,0.5)*(1+tc1_voltco*(temp-30))} |
| + rbody = {(l*rsheet+rbody_var)*(1+res_match)/w} |
| rbody ra r2 resbody r = {rbody*(1+abs(v(r1,r2))*vc1_body+abs(v(r1,r2))*abs(v(r1,r2))/(l*l)*vc2_body)} |
| rend r1 ra r = {rend*(1+vc1_raw_end*(1-exp(-abs(v(r2,r1))))} |
| + +=1 vc2_raw_end*(1=1 -=1 exp(-abs(v(r2,r1))))=1 *=1 (1=1 -=1 exp(-abs(v(r2,r1))))=1 )=1 |
| + +=1 vc3_raw_end*(1=1 -=1 exp(-abs(v(r2,r1))))=1 *=1 (1=1 -=1 exp(-abs(v(r2,r1))))=1 *=1 (1=1 -=1 exp(-abs(v(r2,r1))))=1 )=1 |
| c1 r2 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_1_1*1e-6)/2} |
| c2 r1 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_1_1*1e-6)/2} |
| .model resbody r tc1 = -1.47e-3 tc2 = 2.7e-6 tnom = 30.0 |
| .ends sky130_fd_pr__res_xhigh_po__base |
| .subckt sky130_fd_pr__res_high_po_0p35 r0 r1 b |
| + |
| .param w = 0.350 l = 5 mult = 1.0 |
| + |
| + body_pelgrom = 0.0347 |
| + rend_mm = 0.085 |
| + rcon = 589.99 |
| + rsheet = 1112.41 |
| + tc1_voltco = -7.1e-3 |
| + vc1_body = -8.46e-3 |
| + vc2_body = 1.97e-3 |
| + vc3_body = 3.30e-5 |
| + vc1_raw_end = -2.02e-2 |
| + vc2_raw_end = 1.55e-1 |
| + vc3_raw_end = 4.61e-2 |
| + r0_var = 50.97 |
| + r1_var = 34.74 |
| + vc1_end = {vc1_raw_end/pwr(l,0.5)*(1+tc1_voltco*(temp-30))} |
| + vc2_end = {vc2_raw_end/pwr(l,0.5)*(1+tc1_voltco*(temp-30))} |
| + vc3_end = {vc3_raw_end/pwr(l,0.5)*(1+tc1_voltco*(temp-30))} |
| + rtot_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2*pow(r0_var,2)+pow((r1_var*l),2))} |
| + rend_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2)*r0_var} |
| + rbody_var = {rtot_var-rend_var} |
| + res_match = {(body_pelgrom/sqrt(w*l*mult))*sky130_fd_pr__res_high_po__slope_spectre} |
| + rend = {(rcon+rend_var)*(1+rend_mm/sqrt(mult)*sky130_fd_pr__res_high_po__con_slope_spectre)} |
| + rbody = {(l*rsheet+rbody_var)*(1+res_match)} |
| rend r0 ra r = {rend*(1+min((abs(v(r0,r1))-1.7),0.3)*vc1_end+pow(min(abs(v(r0,r1))-1.7,0.3),2)*vc2_end+pow(min(abs(v(r0,r1))-1.7,0.3),3)*vc3_end)} |
| rhrpoly_0p35 ra r1 resbody r = {rbody*(1+abs(v(r0,r1))*vc1_body+pow(abs(v(r0,r1)),2)*vc2_body+pow(abs(v(r0,r1)),3)*vc3_body)} |
| c1 r0 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_1_1*1e-6)/2} |
| c2 r1 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_1_1*1e-6)/2} |
| .model resbody r tc1 = {tc1rpolybody} tc2 = {tc2rpolybody} tnom = 30.0 |
| .ends sky130_fd_pr__res_high_po_0p35 |
| .subckt sky130_fd_pr__res_high_po_0p69 r0 r1 b |
| + |
| .param w = 0.690 l = 5 mult = 1.0 |
| + |
| + body_pelgrom = 0.0317 |
| + rend_mm = 0.064 |
| + rcon = 389.90 |
| + rsheet = 491.36 |
| + tc1_voltco = -4.27e-3 |
| + vc1_body = 1.92e-4 |
| + vc2_body = 2.86e-4 |
| + vc3_body = 3.48e-5 |
| + vc1_raw_end = -3.90e-4 |
| + vc2_raw_end = 1.37e-1 |
| + vc3_raw_end = 4.52e-2 |
| + r0_var = 28.13 |
| + r1_var = 15.71 |
| + vc1_end = {vc1_raw_end/l*(1+tc1_voltco*(temp-30))} |
| + vc2_end = {vc2_raw_end/l*(1+tc1_voltco*(temp-30))} |
| + vc3_end = {vc3_raw_end/l*(1+tc1_voltco*(temp-30))} |
| + rtot_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2*pow(r0_var,2)+pow((r1_var*l),2))} |
| + rend_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2)*r0_var} |
| + rbody_var = {rtot_var-rend_var} |
| + res_match = {(body_pelgrom/sqrt(w*l*mult))*sky130_fd_pr__res_high_po__slope_spectre} |
| + rend = {(rcon+rend_var)*(1+rend_mm/sqrt(mult)*sky130_fd_pr__res_high_po__con_slope_spectre)} |
| + rbody = {(l*rsheet+rbody_var)*(1+res_match)} |
| rend r0 ra r = {rend*(1+min((abs(v(r0,r1))-1.7),0.3)*vc1_end+pow(min(abs(v(r0,r1))-1.7,0.3),2)*vc2_end+pow(min(abs(v(r0,r1))-1.7,0.3),3)*vc3_end)} |
| rhrpoly_0p69 ra r1 resbody r = {rbody*(1+abs(v(r0,r1))*vc1_body+pow(abs(v(r0,r1)),2)*vc2_body+pow(abs(v(r0,r1)),3)*vc3_body)} |
| c1 r0 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_2_1*1e-6)/2} |
| c2 r1 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_2_1*1e-6)/2} |
| .model resbody r tc1 = {tc1rpolybody} tc2 = {tc2rpolybody} tnom = 30.0 |
| .ends sky130_fd_pr__res_high_po_0p69 |
| .subckt sky130_fd_pr__res_high_po_1p41 r0 r1 b |
| + |
| .param w = 1.410 l = 5 mult = 1.0 |
| + |
| + body_pelgrom = 0.0354 |
| + rend_mm = 0.033 |
| + rcon = 254.77 |
| + rsheet = 230.05 |
| + tc1_voltco = -4.68e-3 |
| + vc1_body = -1.24e-4 |
| + vc2_body = 2.41e-4 |
| + vc1_raw_end = -7.62e-2 |
| + vc2_raw_end = 0.198 |
| + vc3_raw_end = 8.81e-2 |
| + r0_var = 15.43 |
| + r1_var = 6.96 |
| + vc1_end = {vc1_raw_end*0.705/l*(1+tc1_voltco*(temp-30))} |
| + vc2_end = {vc2_raw_end*0.705/l*(1+tc1_voltco*(temp-30))} |
| + vc3_end = {vc3_raw_end*0.705/l*(1+tc1_voltco*(temp-30))} |
| + rtot_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2*pow(r0_var,2)+pow((r1_var*l),2))/m} |
| + rend_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2)*r0_var/m} |
| + rbody_var = {rtot_var-rend_var} |
| + res_match = {(body_pelgrom/sqrt(w*l*mult))*sky130_fd_pr__res_high_po__slope_spectre} |
| + rend = {(rcon+rend_var)*(1+rend_mm/sqrt(mult)*sky130_fd_pr__res_high_po__con_slope_spectre)} |
| + rbody = {(l*rsheet+rbody_var)*(1+res_match)} |
| rend r0 ra r = {rend*(1+min((abs(v(r0,r1))-1.4),0.6)*vc1_end+pow(min(abs(v(r0,r1))-1.4,0.6),2)*vc2_end+pow(min(abs(v(r0,r1))-1.4,0.6),3)*vc3_end)} |
| rhrpoly_1p41 ra r1 resbody r = {rbody*(1+abs(v(r0,r1))*vc1_body+pow(abs(v(r0,r1)),2)*vc2_body)} |
| c1 r0 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_4_1*1e-6)/2} |
| c2 r1 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_4_1*1e-6)/2} |
| .model resbody r tc1 = {tc1rpolybody} tc2 = {tc2rpolybody} tnom = 30.0 |
| .ends sky130_fd_pr__res_high_po_1p41 |
| .subckt sky130_fd_pr__res_high_po_2p85 r0 r1 b |
| + |
| .param w = 2.850 l = 5 mult = 1.0 |
| + |
| + body_pelgrom = 0.0388 |
| + rend_mm = 0.015 |
| + rcon = 130.36 |
| + rsheet = 113.56 |
| + tc1_voltco = -9.36e-3 |
| + vc1_body = 3.21e-4 |
| + vc2_body = 4.95e-5 |
| + vc1_raw_end = 1.47e-2 |
| + vc2_raw_end = 0.136 |
| + vc3_raw_end = 5.29e-2 |
| + r0_var = 8.23 |
| + r1_var = 3.29 |
| + vc1_end = {vc1_raw_end*1.425/l*(1+tc1_voltco*min((temp-30),0))} |
| + vc2_end = {vc2_raw_end*1.425/l*(1+tc1_voltco*min((temp-30),0))} |
| + vc3_end = {vc3_raw_end*1.425/l*(1+tc1_voltco*min((temp-30),0))} |
| + rtot_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2*pow(r0_var,2)+pow((r1_var*l),2))/m} |
| + rend_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2)*r0_var/m} |
| + rbody_var = {rtot_var-rend_var} |
| + res_match = {(body_pelgrom/sqrt(w*l*mult))*sky130_fd_pr__res_high_po__slope_spectre} |
| + rend = {(rcon+rend_var)*(1+rend_mm/sqrt(mult)*sky130_fd_pr__res_high_po__con_slope_spectre)} |
| + rbody = {(l*rsheet+rbody_var)*(1+res_match)} |
| rend r0 ra r = {rend*(1+min((abs(v(r0,r1))-1.6),0.4)*vc1_end+pow(min(abs(v(r0,r1))-1.6,0.4),2)*vc2_end+pow(min(abs(v(r0,r1))-1.6,0.4),3)*vc3_end)} |
| rhrpoly_2p85 ra r1 resbody r = {rbody*(1+abs(v(r0,r1))*vc1_body+pow(abs(v(r0,r1)),2)*vc2_body)} |
| c1 r0 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_8_2*1e-6)/2} |
| c2 r1 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_8_2*1e-6)/2} |
| .model resbody r tc1 = {tc1rpolybody} tc2 = {tc2rpolybody} tnom = 30.0 |
| .ends sky130_fd_pr__res_high_po_2p85 |
| .subckt sky130_fd_pr__res_high_po_5p73 r0 r1 b |
| + |
| .param w = 5.730 l = 5 mult = 1.0 |
| + |
| + body_pelgrom = 0.037 |
| + rend_mm = 0.01 |
| + rcon = 68.05 |
| + rsheet = 56.46 |
| + tc1_voltco = 2.35e-2 |
| + vc1_body = -2.62e-5 |
| + vc2_body = 2.25e-5 |
| + vc1_raw_end = 8.74e-4 |
| + vc2_raw_end = -1.34e-2 |
| + vc3_raw_end = 1.72e-2 |
| + r0_var = 4.29 |
| + r1_var = 1.6 |
| + vc1_end = {vc1_raw_end*2.865/l*(1+(tc1_voltco*min((temp-30),0)))} |
| + vc2_end = {vc2_raw_end*2.865/l*(1+(tc1_voltco*min((temp-30),0)))} |
| + vc3_end = {vc3_raw_end*2.865/l*(1+(tc1_voltco*min((temp-30),0)))} |
| + rtot_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2*pow(r0_var,2)+pow((r1_var*l),2))/m} |
| + rend_var = {sky130_fd_pr__res_high_po__var_mult*sqrt(2)*r0_var/m} |
| + rbody_var = {rtot_var-rend_var} |
| + res_match = {(body_pelgrom/sqrt(w*l*mult))*sky130_fd_pr__res_high_po__slope_spectre} |
| + rend = {(rcon+rend_var)*(1+rend_mm/sqrt(mult)*sky130_fd_pr__res_high_po__con_slope_spectre)} |
| + rbody = {(l*rsheet+rbody_var)*(1+res_match)} |
| rend r0 ra r = {rend*(1+min(abs(v(r0,r1)),2.0)*vc1_end+pow(min(abs(v(r0,r1)),2.0),2)*vc2_end+pow(min(abs(v(r0,r1)),2.0),3)*vc3_end)} |
| rhrpoly_5p73 ra r1 resbody r = {rbody*(1+abs(v(r0,r1))*vc1_body+pow(abs(v(r0,r1)),2)*vc2_body)} |
| c1 r0 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_16_2*1e-6)/2} |
| c2 r1 b c = {((l+2*2.08)*w*crpf_precision*1e-12+2*(l+2*2.08+w)*crpfsw_precision_16_2*1e-6)/2} |
| .model resbody r tc1 = {tc1rpolybody} tc2 = {tc2rpolybody} tnom = 30.0 |
| .ends sky130_fd_pr__res_high_po_5p73 |
