In the MO multiplier, to have strong input signals and have a better implementation, the row of AND gates are implemented by using inverter and NOR components.
Universal gates such as NOR, NAND and MAJORITY-NOT gates are implemented with a set of inverters and non-conventional implementation of them.
In Benea-Chelmus and colleagues' experiment, these gates are implemented by auxiliary ultrashort pulses of near-infrared light that interact with the vacuum in a nonlinear optical crystal.
Reversible logic gates are implemented in an optical domain as it provides high speed and low energy computations.
In this contribution we discuss a proposal based on small-capacitance Josephson junctions in the charge regime in which quantum gates are implemented by means of adiabatic geometric phases.
Please notice that this multi inputs NOR gate is implemented by only one minimum size inverter and several nanoelements while for the implementation of the same function in CMOS technology several NMOS and PMOS transistors are needed.
In particular, single qubit gates and the CNOT-gate are implemented as OQWs on fully connected graphs.
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In the first, we illustrate how to realize the Hadamard gate in a single-qubit system, while in the second, the controlled-NOT (CNOT) gate is implemented in two-qubit systems with the Ising and Heisenberg interactions.
Gating was implemented based on negative control staining profiles.
