Quantum Computing. Hafiz Md. Hasan Babu
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Название: Quantum Computing

Автор: Hafiz Md. Hasan Babu

Издательство: Ingram

Жанр: Программы

Серия:

isbn: 9780750327473

isbn:

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      A quantum full-subtractor can be designed using two quantum TR gates, shown in figure 4.7. Figure 4.8 is the optimized version of the full-subtractor. The quantum cost of a quantum full-subtractor is 6 and the delay is 4Δ.

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      Figure 4.7. The quantum full-subtractor by cascading two quantum TR gates.

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      Figure 4.8. The optimized quantum full-subtractor.

      This chapter presents the quantum full-adder and full-subtractor from the half-adder and half-subtractor circuits. The quantum costs of the adder and subtractor circuits are discussed for better understanding of the circuits.

      [1] Babu H M H, Islam M R, Chowdhury S M A and Chowdhury A R 2004 Synthesis of a full-adder circuit using reversible logic Proc. 17th Int. Conf. on VLSI Design (Mumbai) 2004 pp 757–60

      [2] Babu H M H, Islam R, Chowdhury A R and Chowdhury S M A 2003 On the realization of reversible full-adder circuit Int. Conf. on Computer and Information Technology pp 880–3

      [3] Babu H M H, Islam R, Chowdhury A R and Chowdhury S M A 2003 Reversible logic synthesis for minimization of full-adder circuit Proc. Euromicro Symp. on Digital System Design pp 50–4

      [4] Babu H M H, Jamal L and Saleheen N 2013 An efficient approach for designing a reversible fault tolerant n-bit carry look-ahead adder IEEE Int. SOC Conf. pp 98–103

      [5] Cheng K-W and Tseng C-C 2002 Quantum full adder and subtractor Electron. Lett. 38 1343–4

      [6] Cuccaro S A, Draper T G, Kutin S A and Moulton D P 2004 A new quantum ripple-carry addition circuit (arXiv: quant-ph/0410184)

      [7] Khan M H A and Perkowski M A 2007 Quantum ternary parallel adder/subtractor with partially-look-ahead carry J. Syst. Archit. 53 453–64

      [8] Monfared A T and Haghparast M 2016 Design of new quantum/reversible ternary subtractor circuits J. Circuit. Syst. Comp. 25 1650014

      [9] Murali K V R M, Sinha N, Mahesh T S, Levitt M H, Ramanathan K V and Kumar A 2002 Quantum-information processing by nuclear magnetic resonance: experimental implementation of half-adder and subtractor operations using an oriented spin-7/2 system Phys. Rev. A 66 22313

      [10] Takahashi Y 2009 Quantum arithmetic circuits: a survey IEICE Trans. Fundam. Electron. Commun. Comput. Sci. 92 1276–83

      [11] Takahashi Y, Tani S and Kunihiro N 2010 Quantum addition circuits and unbounded fan-out Quantum Inf. Comput. 10 872–90

      IOP Publishing

      Quantum Computing

      A pathway to quantum logic design

      Hafiz Md Hasan Babu

      Chapter 5

      The quantum multiplexer and demultiplexer

      In large-scale computing systems, it is necessary for a single line to carry two or more signals. One signal can be placed on one line at a time. However, the device which will allow us to select and place the signal we choose on a common line, is called a multiplexer (MUX). The purpose of a MUX is to select the input of any n inputs and feed that to one output line. The function of a demultiplexer (DEMUX) is the opposite to the function of the MUX.

      This section presents the design of the quantum multiplexer. The multiplexer causes the transmission of a large number of information units over a smaller number of channels. Architecturally a digital multiplexer is a logic circuit that puts one of several inputs to a single output. A set of selected inputs controls the inputs. Generally a multiplexer has m inputs and n selected inputs where m=2n.

      A 2-to-1 multiplexer is the smallest unit of architecture of a quantum multiplexer. The characteristic function of a multiplexer is s0′I0+s0I1. A quantum Fredkin gate, as shown in figures 5.1(a) and (b), can be used as a 2-to-1 quantum multiplexer as it can map the characteristic function of a multiplexer.

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      Figure 5.1. The quantum Fredkin gate. (a) Quantum circuit of a quantum Fredkin gate. (b) Symbol of a quantum Fredkin gate.

      Let I0 and I1 be the inputs and S0 be the selected input of a 2-to-1 multiplexer. When S0=0, then input I0 transmits to the output Y and when S0=1, then input I1 transmits to the output Y. Figure 5.2 shows the architecture of a quantum 2-to-1 multiplexer using a quantum Fredkin gate. The quantum cost and delay of this quantum 2-to-1 multiplexer are 5 and 5Δ, respectively. Moreover, the number of garbage outputs is two.

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      Figure 5.2. The quantum Fredkin gate as a quantum 2-to-1 multiplexer.

      The quantum 4-to-1 multiplexer has four inputs, two select lines, and one СКАЧАТЬ