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Table 2 INV gates

From: Quasi-classical modeling of molecular quantum-dot cellular automata multidriver gates

	1,6-heptadiene		1,8-nonadiene		1,4-diallyl butane
P _d	P _o	P _o ^*	P _o	P _o ^*	P _o	P _o ^*
0.0	−0.068	0	−0.058	0	−2.3 E-05	0
0.1	−0.126	−0.101	−0.217	−0.207	−0.987	−0.974
0.2	−0.191	−0.200	−0.398	−0.389	−0.987	−0.993
0.3	−0.260	−0.293	−0.534	−0.536	−0.989	−0.997
0.4	−0.323	−0.378	−0.630	−0.646	−0.990	−0.998
0.5	−0.378	−0.455	−0.695	−0.726	−0.992	−0.998
0.6	−0.423	−0.523	−0.740	−0.785	−0.994	−0.999
0.7	−0.460	−0.582	−0.771	−0.828	−0.996	−0.999
0.8	−0.490	−0.633	−0.793	−0.861	−0.997	−0.999
0.9	−0.513	−0.677	−0.808	−0.885	−0.998	−0.999
1.0	−0.531	−0.715	−0.818	−0.904	−0.999	−0.999
RMSE^*	0.104		0.050		0.006

When there is a single driver, the change in the sign of the input will result in a change in the sign of output polarization. The negative inputs have been omitted to reduce the size of the table.
P_o and P_o^* denote the calculated output polarizations based on the SA/CASSCF and TSM methods respectively.
RMSE^* represents the root mean square errors of P_o and P_o^*.

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