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DESIGN OF DESIGN OF REGULAR REGULAR CLASSICAL AND CLASSICAL AND QUANTUM QUANTUM CIRCUITS CIRCUITS

Design of Regular CLASSICAL AND Quantum Circuits

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Design of Regular CLASSICAL AND Quantum Circuits. CLASSICAL LOGIC. Design of SRFPGA cell. General idea of SRFPGA architecture. SRFPGA layout With I/O pins. 1. Faults observed during column test C = 2. Test output. 0. - PowerPoint PPT Presentation

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Page 1: Design  of  Regular CLASSICAL AND Quantum Circuits

DESIGN OF DESIGN OF REGULAR REGULAR

CLASSICAL AND CLASSICAL AND QUANTUM QUANTUM CIRCUITSCIRCUITS

Page 2: Design  of  Regular CLASSICAL AND Quantum Circuits

CLASSICACLASSICAL LOGICL LOGIC

2

Page 3: Design  of  Regular CLASSICAL AND Quantum Circuits

3

Page 4: Design  of  Regular CLASSICAL AND Quantum Circuits

4

Page 5: Design  of  Regular CLASSICAL AND Quantum Circuits

5

SRFPGA layoutWith I/O pins

Page 6: Design  of  Regular CLASSICAL AND Quantum Circuits

6

Var1

var2

var3

var4

var5

var6

var7

var8

var9

var10

var11

var12

var13

var14

var15

var16

1 1 1 1 1 1 1 1 1 1 1 1 1 1 1 1

1 1 1 1 1 1 1 1 1 1 1 0 1 0 1 1

1

1

1

1

1

1

1

1

1

1

1

1

1

1

1

1

1

1

0

1

1

1

1

1

1

1

1

1

1

1

1

0

Input test vector

Inputtestvector

Test output

Testoutput

Faults observed during column testC = 2.

Faults observed during

diagonal testD = 2

Total number ofFaults N = C * D= 2 * 2 = 4.

Page 7: Design  of  Regular CLASSICAL AND Quantum Circuits

REVERSIBLE REVERSIBLE LOGICLOGIC

7

Page 8: Design  of  Regular CLASSICAL AND Quantum Circuits

A logic gate is reversible if Each input is mapped to a unique output It permutes the set of input values

A combinational logic circuit is reversible if it satisfies the following:

Has only one Fanout, Uses only reversible gates, No feedback path, has as many input wires as output wires, and

permutes the input values.8

Page 9: Design  of  Regular CLASSICAL AND Quantum Circuits

a a

aa

bbac

9

NOT gate

a b a c0 0 0 00 1 0 11 0 1 11 1 1 0

Controlled-NOT or Feynman gate

Page 10: Design  of  Regular CLASSICAL AND Quantum Circuits

a

c

b

a

b

cabf

10

a b c a b f0 0 0 0 0 00 0 1 0 0 10 1 0 0 1 00 1 1 0 1 11 0 0 1 0 01 0 1 1 0 11 1 0 1 1 11 1 1 1 1 0

Toffoli gate (Controlled-Controlled NOT gate)

Page 11: Design  of  Regular CLASSICAL AND Quantum Circuits

a

a

b

b

11

Swap gate

Implementation of Swap gate using controlled-NOT

Page 12: Design  of  Regular CLASSICAL AND Quantum Circuits

a

a

b

b

12

Swap gate

Implementation of Swap gate using controlled-NOT

Page 13: Design  of  Regular CLASSICAL AND Quantum Circuits

a

b

c

baacf

abcag

a

b

c

baacf

abcag

13

a b c a f g0 0 0 0 0 00 0 1 0 0 10 1 0 0 1 00 1 1 0 1 11 0 0 1 0 01 0 1 1 1 01 1 0 1 0 11 1 1 1 1 1

Fredkin gate (Controlled SWAP gate)

Page 14: Design  of  Regular CLASSICAL AND Quantum Circuits

14

ALGORITHMS FOR ALGORITHMS FOR SYNTHESIS OF SYNTHESIS OF REVERSIBLE LOGIC REVERSIBLE LOGIC CIRCUITSCIRCUITS

Page 15: Design  of  Regular CLASSICAL AND Quantum Circuits

MMD: Transformation based

Gupta-Agrawal-Jha: PPRM based

Mishchenko-Perkowski: Reversible wave cascade

Kerntopf: Heuristics based

Wille: BDD based synthesis

15

Page 16: Design  of  Regular CLASSICAL AND Quantum Circuits

16

c b a co bo ao

0 0 0 0 0 1

0 0 1 0 0 0

0 1 0 1 1 1

0 1 1 0 1 0

1 0 0 0 0 1

1 0 1 1 0 0

1 1 0 1 0 1

1 1 1 1 1 0

PPRM form for each output in terms ofInput variables are given as follows and node is created

PPRM form for each output in terms ofInput variables are given as follows and node is created

acabbc 0

accbb 0

10 aa

Page 17: Design  of  Regular CLASSICAL AND Quantum Circuits

Parent node is explored by examining each output variable in the PPRM expansion.

Factors are searched in the PPRM expansions that do not contain the same input variable.

For example in the expansion below appropriate terms are “c” and “ac”

The substitution is performed as In this example OR

accbb 0

factorvv ii

17

cbb acbb

Page 18: Design  of  Regular CLASSICAL AND Quantum Circuits

acabbc 0

accbb 0

10 aa

Node0

PQ head Node0

1aa

Algorithm identifies three possible substitutions

1. 2. 3.

cbb acbb

18

Page 19: Design  of  Regular CLASSICAL AND Quantum Circuits

1aa acbb cbb

aa 0

acbb 0

acabbc 0

10 aa

accbb 0

acabbc 0

acabbc 0

cbb 0

10 aa

abbcc 0

acbb 0

10 aa

PQ head Node 1.0 Node 1.1 Node 1.2

Node 1.0 Node 1.1 Node 1.2

19

New nodes are created based on substitution

Page 20: Design  of  Regular CLASSICAL AND Quantum Circuits

20

1aa cbb

aa 0

acbb 0

acabbc 0

10 aa

accbb 0

acabbc 0

acabbc 0

cbb 0

10 aa

abbcc 0

acbb 0

10 aa

Node 1.0

Node 1.1 Node 1.2

acbb

acbb abcc

abcc 0

bb 0

aa 0

acabcc 0

acabbb 0

aa 0

Node 2.0 Node 2.1

PQ head Node 2.0 Node 1.1 Node 1.2 Node 2.1

Page 21: Design  of  Regular CLASSICAL AND Quantum Circuits

21

1aa cbb

aa 0

acbb 0

acabbc 0

10 aa

accbb 0

acabbc 0

acabbc 0

cbb 0

10 aa

abbcc 0

acbb 0

10 aa

Node 1.0

Node 1.1 Node 1.2

acbb

acbb abcc

abcc 0

bb 0

aa 0

acabcc 0

acabbb 0

aa 0

Node 2.0 Node 2.1

abcc

00 cc bb 0

aa 0

Node 3.0

PQ head Node 1.1 Node 1.2 Node 2.1

Page 22: Design  of  Regular CLASSICAL AND Quantum Circuits

22

1aa

aa 0

acbb 0

acabbc 0

10 aa

accbb 0

acabbc 0

Node 1.0

acbb

abcc 0

bb 0

aa 0

Node 2.0

abcc

00 cc bb 0

aa 0

Node 3.0

Node0

a

c

b acbb

a

b

c abcc

a

b

c

ao

bo

co

Final circuit

Page 23: Design  of  Regular CLASSICAL AND Quantum Circuits

Common problem with current approaches: they invariably use nxn Toffoli gates, that might imposes technological limitations.

High Quantum cost of Toffoli gates with many inputs.

Synthesize only reversible functions, not Boolean functions that is not reversible.

23

Page 24: Design  of  Regular CLASSICAL AND Quantum Circuits

24

Implementation of 4x4 Toffoli gate with Quantum realizable 2x2 primitives such as controlled-V, controlled-NOT, controlled-V+.

Implementation of 4x4 Toffoli gate with Quantum realizable 2x2 primitives such as controlled-V, controlled-NOT, controlled-V+.

a

b

0

c

d

a

b

d

c

V V V+

V V V+

V V V+

a

b

0

c

d

Page 25: Design  of  Regular CLASSICAL AND Quantum Circuits

CREATING CREATING QUANTUM QUANTUM

ARRAY FROM ARRAY FROM LATTICELATTICE

25

Page 26: Design  of  Regular CLASSICAL AND Quantum Circuits

26

zbby

r sbb b b

x y z v

r sbb b b

xv

RULE (S, S)

r sb1 b

x y z v

r sb1 b

x

zbby

RULE (pD, pD)1

vzy

1

r sb1

x y z v

r sb b

x

zbby

RULE (nD, nD)1

vzy

b 11

r sb

x y z v

r sb

x

zbby

RULE (s, pD)1

vzy

1b b b b

r sb

x y z v

r sb

x

zbby

RULE (pD, s)1

vzy

1b b b b

Positive Davio Tree can be created by expanding PPRM function using positive Davio expansion.

Positive Davio Lattice is created by performing joining operation for neighboring cells at every level.

Other Lattices can be created using similar method but using expansions such as Shannon or Negative Davio expansions or combination of them.

Page 27: Design  of  Regular CLASSICAL AND Quantum Circuits

On the previous foils I showed representation of the Davio and Shannon cells as cascade of reversible gates.

Next I present unique method to create Quantum Array from Positive Davio Lattice.

The same approach can be used for other Lattices.

27

Page 28: Design  of  Regular CLASSICAL AND Quantum Circuits

a

c

b

a

b

cabd

a

bc cabd

Positive Davio cell

Positive Davio cell representation with

Toffoli gate

28

bcdcdbcacabdbdad 1

abdbdad 1 bddba

abdba abb 1

ad1 a1

d

a

1 c

1 d 1 d

1 b 1 b

1 a 1 a 1 a

1 d

1

11

1

1 1

10

0

Each node represents pDv cell.

Page 29: Design  of  Regular CLASSICAL AND Quantum Circuits

29

+

+ +

++

+ ++

+

0

d

1

11

1

1

1

1 1

1

111

1

d

a

d

bb

1

a a

c

1

Page 30: Design  of  Regular CLASSICAL AND Quantum Circuits

30

abcd

0

1

1

1

0

1

a1

ad1

bab1

d

a aabdb

adabddb1

bddab

bcdcdacbcabdaddb1

garbage

garbage

garbage

garbage

garbage

function

Page 31: Design  of  Regular CLASSICAL AND Quantum Circuits

31

abcd

0

1

1

1

0

1

a1

ad1

bab1

d

a aabdb

adabddb1

bddab

bcdcdacbcabdaddb1

garbage

garbage

garbage

garbage

garbage

function

Page 32: Design  of  Regular CLASSICAL AND Quantum Circuits

a

c

b

a

b

cabd

a

bc cabd

Positive Davio cell

Positive Davio cell representation with

Toffoli gate

32

Each node represents pDv cell.

Page 33: Design  of  Regular CLASSICAL AND Quantum Circuits

33

Page 34: Design  of  Regular CLASSICAL AND Quantum Circuits

Reversible circuit synthesized with only 3x3 Toffoli gates.

Generates reversible circuit for any ESOP.

Adds ancilla bits but overall cost of the circuit will be lower due to use of low cost 3x3 Toffoli gates.

34

Page 35: Design  of  Regular CLASSICAL AND Quantum Circuits

35

Page 36: Design  of  Regular CLASSICAL AND Quantum Circuits

36

Page 37: Design  of  Regular CLASSICAL AND Quantum Circuits

37

Page 38: Design  of  Regular CLASSICAL AND Quantum Circuits

DIPAL GATES, DIPAL GATES, DIPAL GATE DIPAL GATE

FAMILIES AND FAMILIES AND THEIR ARRAYSTHEIR ARRAYS

38

Page 39: Design  of  Regular CLASSICAL AND Quantum Circuits

a

c

b

a

b

cabd

a

b

c cabd

a

c

b

a

ba

b

c

cbad cbad

Positive Davio cell

Positive Davio cell representation with Toffoli

gate

Negative Davio cell

Negative Davio cell representation with Toffoli

gate

39

Page 40: Design  of  Regular CLASSICAL AND Quantum Circuits

][

]1[

cbab

acabb

acba

acbaf

40

a

b

c

cabaf a

b

c

cabaf

cb

a

Shannon cell

Dipal cell representation with

reversible gates

There are 23! = 8! = 40320 3x3 Reversible logic functions, however only handful of them shown earlier are useful for synthesis purpose.

Dipal gate is a reversibleequivalent of Shannon cell

Dipal gate is a reversibleequivalent of Shannon cell

Page 41: Design  of  Regular CLASSICAL AND Quantum Circuits

41

a

b

c

bacaf

a

b

c

a

cb

bacaf

Shannon cell with negative variable

Dipal cell with negative variable represented with

reversible gates

Page 42: Design  of  Regular CLASSICAL AND Quantum Circuits

][

]1[

cbab

acabb

acba

acbaf

42

a

b

c

cabaf a

b

c

cabaf

cb

a

Shannon cell

Dipal cell representation with

reversible gates

There are 23! = 8! = 40320 3x3 Reversible logic functions, however only handful of them shown earlier are useful for synthesis purpose.

Dipal gate is a reversibleequivalent of Shannon cell

Dipal gate is a reversibleequivalent of Shannon cell

Page 43: Design  of  Regular CLASSICAL AND Quantum Circuits

c b a a

0 0 0 0 0 0

0 0 1 0 0 1

0 1 0 1 1 0

0 1 1 1 0 1

1 0 0 1 0 0

1 0 1 1 1 1

1 1 0 0 1 0

1 1 1 0 1 1

43

b c

b a[b c] input

output

0 0

1 1

2 6

3 5

4 4

5 7

6 2

7 3

Page 44: Design  of  Regular CLASSICAL AND Quantum Circuits

44

1 0 0 0 0 0 0 0

0 1 0 0 0 0 0 0

0 0 0 0 0 0 1 0

0 0 0 0 0 1 0 0

0 0 0 0 1 0 0 0

0 0 0 0 0 0 0 1

0 0 1 0 0 0 0 0

0 0 0 1 0 0 0 0

000

001

010

011

100

101

110

111

000 001 010 011 100 101 110 111

Page 45: Design  of  Regular CLASSICAL AND Quantum Circuits

45

Page 46: Design  of  Regular CLASSICAL AND Quantum Circuits

EXPERIMENEXPERIMENTAL TAL

RESULTSRESULTS46

Page 47: Design  of  Regular CLASSICAL AND Quantum Circuits

47

Benchmark #Real inputs

#Garbage inputs

#Gates Lattice

Cost Lattice

CPU time Lattice

#Gates DMM

Cost DMM

#Gates AJ

Cost AJ

2to5 5 4 31 107 0.12 15 107 20 100

rd32 3 1 4 8 < 0.01 4 8 4 8

rd53 5 5 11 39 < 0.01 16 75 13 116

3_17 3 1 10 21 < 0.01 6 12 6 14

6sym 10 6 34 150 0.37 20 62 NA NA

5mod5 5 1 14 58 < 0.01 10 90 11 91

4mod5 4 1 6 18 < 0.01 5 13 5 13

ham3 3 0 3 7 < 0.01 5 7 5 9

xor5 5 0 4 4 < 0.01 4 4 4 4

Xnor5 5 1 5 5 < 0.01 -------- ---------- ---------- ----------

decod24 4 2 10 30 < 0.01 -------- ---------- 11 31

Cycle10_2 12 6 180 860 27.9 19 1198 ---------- ----------

ham7 7 5 22 58 0.10 23 81 24 68

Page 48: Design  of  Regular CLASSICAL AND Quantum Circuits

48

Benchmark #Real inputs

#Garbage inputs

#Gates Lattice

Cost Lattice

CPU time Lattice

#Gates DMM

Cost DMM

#Gates AJ

Cost AJ

graycode6 6 5 5 5 < 0.01 5 5 5 5

graycode10 10 9 9 9 < 0.01 9 9 9 9

graycode20 20 19 19 19 < 0.01 19 19 19 19

nth_prime3_inc

3 4 4 6 < 0.01 4 6 ---------- ----------

nth_prime4_inc

4 5 16 48 < 0.01 12 58 ---------- ----------

nth_prime5_inc

5 5 29 91 0.22 26 78 ---------- ----------

alu 5 2 5 17 < 0.01 -------- ---------- 18 114

4_49 4 4 16 52 0.04 16 58 13 61

hwb4 4 4 12 28 < 0.01 17 63 15 35

hwb5 5 5 24 96 1.2 24 104 ---------- ----------

hwb6 6 6 32 128 2.0 42 140 ---------- ----------

pprm1 4 4 9 33 < 0.01 -------- ---------- ---------- ----------

Page 49: Design  of  Regular CLASSICAL AND Quantum Circuits

49

Benchmark #Inputs #Gates pDv Lattice

Cost pDv Lattice

#Gates Shannon Lattice

Cost Shannon Lattice

2to5 5 31 107 41 117

rd32 3 4 8 4 8

rd53 5 11 39 18 46

3_17 3 10 21 15 26

6sym 10 34 150 51 167

5mod5 5 14 58 30 81

4mod5 4 6 18 12 24

Ham3 3 3 7 6 10

xor5 5 4 4 4 4

Xnor5 5 5 5 5 5

Decod24 4 10 30 20 40

Cycle10_2 12 180 860 270 950

Ham7 7 22 58 32 68

Page 50: Design  of  Regular CLASSICAL AND Quantum Circuits

50

Benchmark #Inputs #Gates pDv Lattice

Cost pDv Lattice

#Gates Shannon Lattice

Cost Shannon Lattice

Graycode6 6 5 5 5 5

Graycode10 10 9 9 9 9

Graycode20 20 19 19 19 19

nth_prime3_inc

3 4 6 6 8

nth_prime4_inc

4 16 48 29 61

nth_prime5_inc

5 29 91 39 101

Alu 5 5 17 10 22

4_49 4 16 52 22 58

Hwb4 4 12 28 15 31

Hwb5 5 24 96 38 110

Hwb6 6 32 128 40 134

Pprm1 4 9 33 14 38

Page 51: Design  of  Regular CLASSICAL AND Quantum Circuits

51

Page 52: Design  of  Regular CLASSICAL AND Quantum Circuits

52

Page 53: Design  of  Regular CLASSICAL AND Quantum Circuits

Fig. 2. Circuit for function FX2 created with our method for traditional cost function calculation that does not take Ion Trap technology constraints into account.

53

abcd

0

1

1

1

0

1

a1

ad1

bab1

d

a aabdb

adabddb1

bddab

bcdcdacbcabdaddb1

garbage

garbage

garbage

garbage

garbage

function

Page 54: Design  of  Regular CLASSICAL AND Quantum Circuits

Fig. 3. Circuit from Figure 2 modified with adding SWAP gates for new cost function calculation that does take Ion Trap technology constraints into account, with XX gates added. It has 36 SWAP gates added to realize LNNM.

54

Page 55: Design  of  Regular CLASSICAL AND Quantum Circuits

55

bcdcdbcacabdbdad 1

abdbdad 1 bddba

abdba abb 1

ad1 a1

d

a

1 c

1 d 1 d

1 b 1 b

1 a 1 a 1 a

1 d

1

11

1

1 1

10

0

Example of Positive Davio Lattice from [Perkowski97d]. Positive Davio Expansion is applied in each node. Variable d is repeated

Page 56: Design  of  Regular CLASSICAL AND Quantum Circuits

56

1

2 3

45 6

7 8 9

a

b

c

f

Garbage

Garbage

Garbage

a

b

c

f

Garbage

Garbage

Garbage

(a)

(b)

Transformation of function F3(a,b,c) from classical Positive Davio Lattice to a Quantum Array with Toffoli and SWAP gates. Each SWAP gate is next replaced with 3 Feynman gates.(a) intermediate form, (b) final Quantum Array.

Page 57: Design  of  Regular CLASSICAL AND Quantum Circuits

1

2 3

45 6

7 8 9

a

b

c

f

Garbage

Garbage

Garbage

Garbage

Garbage

Garbage

57

Page 58: Design  of  Regular CLASSICAL AND Quantum Circuits

a

b

c

f

Garbage

Garbage

Garbage

Garbage

Garbage

Garbage

d1

d2

d3

d4

d5

d6

x

y

z

v

58

Page 59: Design  of  Regular CLASSICAL AND Quantum Circuits

a

b

59

General layout of the layered diagram

Each box represents a gate from family of Dipal gate

Page 60: Design  of  Regular CLASSICAL AND Quantum Circuits

d3

d6

d2

d4

d1

a

b

cx

y

z

v

d5

60

Page 61: Design  of  Regular CLASSICAL AND Quantum Circuits

61

Benchmark #Gates Lattice

Cost Lattice

#Gates with SWAP insertion for Lattice

Cost with SWAP gates for Lattice

#Gates DMM

Cost DMM

#Gates with SWAP insertion for MMD

Cost with SWAP gates for MMD

2to5 31 107 61 197 15 107 31 155

rd32 4 8 8 20 4 8 6 14

rd53 11 39 44 138 16 75 72 273

3_17 10 21 14 33 6 12 8 18

6sym 34 150 56 216 20 62 78 236

5mod5 14 58 17 67 10 90 48 204

4mod5 6 18 10 30 5 13 11 31

Ham3 3 7 3 7 5 7 7 13

Xor5 4 4 4 4 4 4 4 4

Xnor5 5 5 5 5 -------- -------- -------- --------

decod24 10 30 14 42 -------- -------- -------- --------

Cycle10_2 180 860 306 1238 19 1198 199 1738

Ham7 22 58 30 112 23 81 79 249

Page 62: Design  of  Regular CLASSICAL AND Quantum Circuits

62

Benchmark #Gates Lattice

Cost Lattice

#Gates with SWAP insertion for Lattice

Cost with SWAP gates for Lattice

#Gates DMM

Cost DMM

#Gates with SWAP insertion for MMD

Cost with SWAP gates for MMD

Graycode6 5 5 5 5 5 5 5 5

Graycode10 9 9 9 9 9 9 9 9

Graycode20 19 19 19 19 19 19 19 19

Nth_prime3_inc

4 6 5 9 4 6 6 12

Nth_prime4_inc

16 48 20 60 12 58 18 76

Nth_prime5_inc

29 91 39 121 26 78 128 384

Alu 5 17 7 23 -------- -------- ---------- ----------

4_49 16 52 41 127 16 58 40 130

hwb4 12 28 15 40 17 63 39 129

hwb5 24 96 44 156 24 104 64 224

hwb6 32 128 72 248 42 140 144 446

pprm1 9 33 19 63 -------- -------- ---------- ----------

Page 63: Design  of  Regular CLASSICAL AND Quantum Circuits

GENERALIZED GENERALIZED REGULARITIES REGULARITIES FOR QUANTUM FOR QUANTUM

AND NANO-AND NANO-TECHNOLOGIESTECHNOLOGIES

63

Page 64: Design  of  Regular CLASSICAL AND Quantum Circuits

64

(a) (b) (c)

(d)

Page 65: Design  of  Regular CLASSICAL AND Quantum Circuits

65

Page 66: Design  of  Regular CLASSICAL AND Quantum Circuits

66

Page 67: Design  of  Regular CLASSICAL AND Quantum Circuits

67

Page 68: Design  of  Regular CLASSICAL AND Quantum Circuits

68

Page 69: Design  of  Regular CLASSICAL AND Quantum Circuits

69

Page 70: Design  of  Regular CLASSICAL AND Quantum Circuits

70

Page 71: Design  of  Regular CLASSICAL AND Quantum Circuits

71

Page 72: Design  of  Regular CLASSICAL AND Quantum Circuits

72

Page 73: Design  of  Regular CLASSICAL AND Quantum Circuits

73

Page 74: Design  of  Regular CLASSICAL AND Quantum Circuits

QUANTUM QUANTUM CIRCUITS AND CIRCUITS AND

QUANTUM ARRAYS QUANTUM ARRAYS FROM TRULY FROM TRULY

QUANTUM GATESQUANTUM GATES74

Page 75: Design  of  Regular CLASSICAL AND Quantum Circuits

Basic single qubit quantum gates

75

NOT Pauli x Pauli y Pauli z Hadamard

X Y Z H

01

10x

0

0

i

iy

10

01z

11

11

2

1H

XX YY ZZ HH

(a) (b) (c) (d)

01

10x

0

0

i

iy

10

01z

11

11

2

1H

Phase gate Pseudohadamard gate Inverse pseudohadamard gate

V S h 1h

ii

iiiV

11

1

2

1

ie

S0

01)(

11

11

2

1h

11

11

2

11h

V Gate

VV SS hh 1h 1h

ii

iiiV

11

1

2

1

ie

S0

01)(

11

11

2

1h

11

11

2

11h

(a) (b) (c) (d)

Page 76: Design  of  Regular CLASSICAL AND Quantum Circuits

Transformation of the circuit realized in Fig. 7 using Toffoli gate. Each Toffoli and SWAP gates are replaced by quantum CNOT and CV/CV+ quantum gates and rearranged to satisfy the neighborhood requirements of Ion trap.

 

76

Page 77: Design  of  Regular CLASSICAL AND Quantum Circuits

The transformations of blocks of quantum gates to the pulses level.   77

Page 78: Design  of  Regular CLASSICAL AND Quantum Circuits

CONCLUSIONCONCLUSIONSS

78

Page 79: Design  of  Regular CLASSICAL AND Quantum Circuits

Experimental results proved that our algorithm produced better results in terms of quantum cost compared to other contemporary algorithms for synthesis of reversible logic.

New gate family called Dipal gate

Presented new synthesis method with layered diagrams.

More accurate technology specific cost model for 1D

qubit neighborhood architecture.

79

Page 80: Design  of  Regular CLASSICAL AND Quantum Circuits

A new method based of lattice diagram to synthesize reversible logic circuit with A new method based of lattice diagram to synthesize reversible logic circuit with

3x3 Toffoli gates.3x3 Toffoli gates.

A new family of gates called Dipal Gates.A new family of gates called Dipal Gates.

New diagrams called layered diagram that uses family of Dipal gate for synthesis New diagrams called layered diagram that uses family of Dipal gate for synthesis

of reversible logic function.of reversible logic function.

Software for creating Lattice diagrams and software for creating quantum array Software for creating Lattice diagrams and software for creating quantum array

from Lattice (Lattice to QA).from Lattice (Lattice to QA).

Program to implement a variant of MMD algorithm.Program to implement a variant of MMD algorithm.

80