IRJET- Design and Implementation of Combinational Circuits using Reversible Gates

Volume: 06 Issue: 03 | Mar 2019 www.irjet.net p-ISSN: 2395-0072
© 2019, IRJET | Impact Factor value: 7.211 | ISO 9001:2008 Certified Journal | Page 4002
Design and Implementation of Combinational Circuits using Reversible
Gates
1Ms. Ashwini Gaikwad 2Ms. Shweta Patil
1M.Tech Student,Departmentof Electronics Engineering, Walchand College of Engg., Sangli
2Assistant Professor,Department of Electronics Engineering, Walchand College of Engg., Sangli
Abstract - Nowadays, the electronic systems are an
important part of an human’s life. As technology develops,
the complexity of the system also increases. This leads to an
increase in power consumption and causes a great issue
faced in the world of electronics. Reversible logic reduces
power consumption and zero-energy computation. The
design of different combinational circuits like a full adder,
subtract or, multiplexer and binary comparator circuits
using reversible decoder is proposed with less Quantum cost.
Keyword – Quantum Cost, Reversible Gate, Garbage
Outputs, Number of Gate
1. INTRODUCTION
Reversible technology is used in various areas such as low
power CMOS design, Nano-Technology, Quantum & Optical
computing, DSP, etc. It is used for reducing power
consumption and loss of data. In reversible technology
there is no information loss at reversible logic so zero
energy consumption takes place. It will help to avoid heat
generation. In Digital Electronics, for design of
combinational and sequential circuits various techniques
are used. Design of a combinational circuit using binary
decoder is one of them.
2. LITERATURE REVIEW
R. Landauer [1] proposed that the amount of energy (heat)
dissipated for every irreversible bit operation is given by
KTln2, where K is the Boltzmann’s constant (1.3807×10-23
JK-1) and T is the operating temperature. At room
temperature (300 K), KTln2 is approximately 2.8×10-21 J,
this amount of energy is small but not negligible. He also
proposed that only the logically irreversible steps in a
computation carry an unavoidable energy penalty. If we
could compute entirely with reversible operations, there
would be low energy consumption. The amount of energy
dissipated in a system has a direct relationship with the
number of bits erased during computation [2]. If a
computation is carried out in a reversible way then Energy
dissipation would not occur. Ruqaiya Khanam, Abdul
Rahman, Pushpam [3], proposed different applications of
reversible gate. D. Maslov and G. Dueck [4] proposed the
new reversible gates which differ only marginally from the
generalized Toffoli gates. Reversible Cascade logic is used
to minimize the most important factor of the reversible
circuit cost which is the number of garbage output
3. REVERSIBLE LOGICS
A Reversible circuit design can be modelled as number of
input equal to number of output and there is one to one
mapping between them. In reversible circuit sequence of
discrete time slices and depth is a summation of total time
slices. Also it has zero fan-out. The typical model is shown
in Fig 1.
Fig- 1: A n × n Reversible Gate
3.1 Quantum Cost
The quantum cost of a reversible gate is defined by the
total number of elementary quantum gates needed to
realize the given function. Elementary quantum gate such
as 1x1 and 2x2 reversible gates. The quantum costs of all
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056

reversible 1x1 and 2x2 gates are taken as zero and unity
respectively. Since every reversible gate is a combination
of 1 x 1 or 2 x 2 quantum gate, the quantum cost of a
reversible gate can be calculated by counting the numbers
of NOT, Controlled-V, Controlled-V+ and CNOT gates used.
Quantum cost is very important factor in quantum
technology. There are some software tools available which
are used to measure quantum cost of design circuit.
3.2 Garbage Output
Every gate output which not used for further processing is
called as garbage output. The unused output which needs
to maintain reversibility of reversible gate is known as
garbage output.
3.3 Fan In
The maximum number of inputs that a logic gate can
accept is called as fan-in. If number of input exceeds, the
output will be vague or inaccurate
3.4 Fan Out
The fan-out is defined as the maximum number of inputs
(load) that can be connected to the output of a gate
without degrading the normal operation. Fan Out is
calculated from the amount of current available in the
output of a gate and the amount of current needed in each
input of the connecting gate
NOT GATE:
A NOT gate is the single Reversible Logic gate. It is 1×1
Reversible Logic Gate. The outputs of NOT gate are
denoted as P=A’ and Quantum cost of a NOT gate is zero.
Fig- 2: NOT Gate and its Truth Table
FEYNMAN GATE
Feynman gate is also known as 2X2 reversible gate. The
outputs of FEYMAN gate are denoted as P=A, Q=A XOR B
and Quantum cost of a Feynman gate is one.
Fig- 3: Feynman Gate and its Truth Table
DOUBLE FEYNMAN GATE (DFG):
Double Feynman Gate is a 3×3 reversible gate. The outputs
of DOUBLE FEYMAN gate are denoted as P=A, Q=A XOR B,
R=A XOR C and Quantum cost of a Double Feynman gate is
TWO.
Fig- 4: Double Feynman Gate and its Truth Table
TR GATE:
TR Gate is a 3×3 reversible gate. The outputs of TR gate are
denoted as P=A, Q=A XOR B, R=AB’ XOR C and Quantum
cost of a TR gate is four.
Fig- 5: TR Gate and its Truth Table
TOFFOLI GATE
Toffoli Gate is a 3×3 reversible gate. The outputs of Toffoli
gate are denoted P=A, Q=B, R=AB⊕ C and Quantum cost is
five.
Fig- 6: Toffoli Gate and its Truth Table

FREDKIN GATE
Fredkin Gate is a 3×3 reversible gate. The outputs of
Fredkin gate are denoted as P=A, Q=A’B XOR AC, R=A’C
XOR AB and Quantum cost of a Fredkin gate is five.
Fig- 7: Fredkin Gate and its Truth Table
PERES GATE
It is also called as 3X3 reversible gate. The output is
defined as P = A, Q = A XOR B and R=AB XOR C and the
Quantum cost of Peres gate is 4.
Fig- 8: Peres Gate and its Truth Table
4. BASIC GATES USING REVERSIBLE GATES
Considering the circuit requirements we need to design
AND gate and OR gate using reversible gates. Here fredkin
gate is used to design AND and OR gates as shown in Fig 9.
Fredkin gate is preferred because it gives optimistic
performance at less Quantum Cost for designing AND and
OR gates.
Fig- 9: AND Gate and or gate using Fredkin
5. REVERSIBLE DECODER
Digital decoder converts a set of digital input signals into
an equivalent decimal code. It changes a code into a set of
signals and does reverse encoding. Decoder means decode
coded information from one format into another. It is used
for Design of a combinational circuit.
Fig-10: 2×4 Decoder
The previous model of 2×4 decoder is shown in Fig. 10.
Replacing Fredkin gates with Peres gate, TR gate, NOT gate
and CNOT gate from the design of 2×4 decoder the
quantum cost can be reduced. The new design of 4×16
decoder using this new 2×4 decoder is shown in Fig 11.
Fig- 11: 4×16 decoder
6. SIMULATION RESULTS
Fig- 12: RTL View of 2 ×4 Decoder

Fig-13: Output Waveform of 2 ×4 Decoder
Fig- 14: RTL Viewof 3 × 8 Decoder
Fig-15: Output Wave form of 3 × 8 Decoder
Fig-16: RTL View of 4 ×16 Decoder
Fig-17: Output Waveform of 4×16 Decoder

7. COMPARATIVE STUDY
Design of reversible decoders are analyzed in terms of
Quantum cost and Garbage outputs.
8. CONCLUSION
Reversible gates can be used to minimize fan-out
limitations, garbage outputs and quantum cost. Different
combinational circuits like full adder, full subtractor,
comparator, multiplexers can be constructed using
reversible decoder with better performance.
REFERENCES
[1] Landauer, R., “Irreversibility and heat generation in the
computing process”, IBM J. Research and Development, vol.
5 (3): pp. 183191, 1961.
[2] Bennett, C.H., “Logical reversibility of computation”,
IBM J. Research and Development, vol. 17: pp. 525-532, 1973
[3] RuqaiyaKhanam, Abdul Rahman,Pushpam “Review on
Reversible Logic Circuits and its Application” International
Conference on Computing, Communication, and Automation
(ICCCA2017)
[4] Gopi Chand Naguboina, k. Anusudha, "Design and
Synthesis of Combinational Circuits using Reversible
decoder in Xilinx", International Conference on Computer
Communication and Signal Processing ICCCSP-17 Chennai
[5] D. Maslov and G. Dueck. “Reversible cascades with
minimal garbage”. IEEE Transactions on CAD, 23(11):1497–
1509, November 2004.
[6] H.G Rangaraju, U. Venugopal, K.N. Muralidhara, K. B.
Raja, “Low power reversible parallel binary
adder/subtractor” International Journal of VLSI design &
Communication Systems (VLSICS) Vol.1, No.3, September
2010.
[7] S.M.Swamynatha, V.Banumathi “Design and Analysis of
FPGA Based 32 Bit ALU Using Reversible Gates”
International Conference on Electrical, Instrumentation, and
CommunicationEngineering (ICEICE2017)2017
[8] Ravish Aradhya H V, Praveen Kumar B V, Muralidhara
K N “Design of Control unit for Low Power ALU Using
Reversible Logic” International Journal of Scientific &
Engineering Research Volume 2, Issue 9, September-2011.
[9] B. Raghu Kanth1, B. Murali Krishna2, G. Phani Kumar3,
J. Poornima4, K. Siva Rama Krishna “A Comparative Study
Of Reversible Logic Gates”International Journal of VLSI &
Signal Processing Applications, Vol.2, Issue 1, Feb 2012,
[10] Y.syamala and A.V.N Tilak “Reversible Arithmetic
Logic Unit” Electronics Computer Technology (ICECT), 2011
3 rd International vol 5 pp207-211, 07 July 2011
CIRCUIT QUANTUM
COST
GARBAGE
OUTPUTS
2 TO 4 DECODER 11 3
3 TO 8 DECODER 31 4
4 TO 16 DECODER 71 5

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