IC design for spread spectrum communication exploiting chaos
Abstract
This paper presents a 2.4 /spl mu/m CMOS IC prototype which includes a programmable chaotic generator and some interface circuitry for chaotic encryption. It realizes a member of the family of the canonical Chua's state equation. It exhibits several bifurcation parameters by changing a few external bias currents and can be used for the chaotic encryption of audio signals.
Full text
IC
design
o
sp ead spec um communica ion exploi ing chaos
Manuel Delgado-Res i u o, Ma ias Li ian and Angel Rod iguez-Vhzquez
Cen o Nacional de Mic oelec 6nica (CNM)
Ed. CICA, A da. Reina Me cedes s/n
41012
-
Se ille, SPAIN.
Abs ac
-
This pape p esen s a 2.4pm CMOS IC
p o o ype which includes a p og ammable chao ic
gene a o and some in e ace ci cui y o chao ic en-
c yp ion. I ealizes a membe o he amily o he ca-
nonical Chua’s s a e equa ion. I exhibi s se e al
bi u ca ion pa ame e s by changing a ew ex e nal
bias cu en s and can be used o he chao ic enc yp-
ion o audio signals.
1.In oduc ion
This pape ollows a p e ious pape o he au-
ho s in
[l].
The e he undamen als o design chao ic
oscilla o s using
Gm-C
echniques we e es ablished
and a IC p o o ype o he Chua’s ci cui buil . I was
able o gene a e a numbe o chao ic oscilla o s by he
i s ime using a ully monoli hic con inuous ime IC.
Howe e , i s con ollabili y was a he icky. Hence,
i was nei he con enien o expe imen al demon-
s a ion o chao ic phenomena no o chao ic enc yp-
ion.
This pape p esen s a new chao ic CMOS chip al-
so
in
2.4pm echnology. The new chip has much be -
e con ollabili y han he p e ious. We p esen i s
a chi ec u e and a numbe o measu emen s o illus-
a e i s pe o mance.
II.Chip A chi ec u e
ses he ollowing blocks:
Fig.
1
shows he chip a chi ec u e which comp is-
A
co e
Gm-C
chao ic oscilla o .
A
Gm-C
e e ence in eg a o .
Th ee ol age bu e s.
As
Fig. 1 illus a es, he chip has 14 pins g ouped
2
supply ol ages.
1
analog g ound.
3
con ol
inpu s
(low impedance).
2 uning pins.
3
unbu e ed ou pu pins (one pe s a e a i-
3 bu e ed ou pu pins (one pe s a e a iable).
as ollows:
able).
As s a ed in [l], he design o he monoli hic
Chua’
s
oscilla o is educed o ansis o le el imple-
men a ion o one single ansconduc ance ampli ie o
g,,
gain and a nonlinea ansconduc o . The
ansconduc o uni has a olded-cascode s uc u e,
a
X
Y
Z
Xbu
Ybu
Zbu
~~
FIGURE
1.
Chip a chi ec u e.
whose inpu s age p esen s a linea iza ion scheme
h ough sou ce degene a ion
[2]
cha ac e ized by an
ample ange o linea i y in he ol age-cu en con-
e sion, low sys ema ic o se , and e y high ou pu
esis ance. The ansconduc ance alue is con olled
by he biasing cu en
Icon ,
applied o pin
can l.
The
nonlinea i y o he cha ac e is ics is less han
1
.O%
e -
o in he inpu ol age anging om -1.5 o 1.5 ,
assuming a symme ical biasing o
+.
2.5~. Ob iously,
p ope ope a ion o he ci cui implies ha he chao ic
a ac o be comp ised inside his ange.
The nonlinea ansconduc o has been imple-
men ed ia he cascaded connec ion o a uni ans-
conduc o and a cu en -mode PWL block, as
explained in
[l]
and [3]. Fig.2(a) and (b) show he
a ia ion o he nonlinea cha ac e is ics o di e en
slopes so and s1
o
he cen al and ou e pieces, e-
spec i ely. They can be ex e nally con olled h ough
biasing cu en s
Icon 2
and
Icon 3
applied o pins
con z and
con ,
. The alues o hese cu en s can be
ega ded as he c yp og aphic key o he secu e com-
munica ion scheme.
III.Chip Measu emen s
Figs.6 and
7
show a bi u ca ion sequence ob-
ained by changing he biasing cu en
Icon 2.
A
dou-
ble sc oll is ob ained h ough a pe iod-doubling ou e
o chaos.
A
Rossle -like chao ic a ac o and se e al
pe iodic windows a e obse ed as well.
Fig.3 and Fig.4 demons a e he easibili y
o
0-7803-3073-0/96/$5
.OO
O1996
IEEE
178
Nonlinea T ansconduc o
D i ing-Poin Cha ac e is ic
c)
I
.o
.o
‘ii
-3.0
11
11
1
I
11
I
-2.5 -1.5 -0.5
0.5
1.5
2.5
Inpu Vol age
(V)
0.5
ldi
(a>
3
-3
Nonlinea T ansconduc o
D i ing-Poin Cha ac e is ic
-2.5
-1.5
-0.5
0.5
1.5
2.5
Inpu Vol age (V)
0.5
ldi
FIGURE
2.
Nonlinea T ansconduc o . Va ia ion
o
he PWL
cha ac e is ics wi h: (a) he cen al slope, so (con ol a iable
!con 2); and (b) he ou e slopes,
s1
(con ol a iable
1cnn 3
chao ic synch oniza ion be ween wo o he manu ac-
u ed IC p o o ypes. Fig.3(a) conside s a linea di u-
sion coupling be ween equi alen s a e a iables o
he wo chao ic oscilla o s [4]. I shows he phase
plo s ob ained om a y-coupled expe imen al se -up,
buil in p ac ice by inse ing an
Ry
linea esis o be-
ween he
y
e minals o bo h p o o ypes (see Fig.1).
I was ound ha whene e he coupling esis ance is
Ry
<
27k0, he
(xl,
x2)
phase plo ollows a nea ly
pe ec s aigh line, hus con i ming synch oniza ion
in spi e
o
he chao ic beha io exhibi ed by he oscil-
la o s, as he
(xl,
21)
phase plo illus a es.
A
simila
se -up was buil by inse ing an
R,
linea esis o be-
ween he
x
e minals o he oscilla o s, hus leading
o an x-coupled sys em.
In
his case, ajec o ies o
bo h ci cui s app oach each o he asymp o ically i
R,
<
745
k0,
o he same in e nal con igu a ions as
be o e. A z-coupled con igu a ion was also buil in
he labo a o y, bu , in his case, he sys em exhibi s
spo adic losses
o
synch oniza ion.
Fig.T)(b) conside s a d i e- esponse scheme as
o iginally p oposed by Peco a and Ca oll [4]. I
shows he phase plo s ob ained om a x-d i e expe -
imen al se -up, buil by inse ing a ol age bu e
om he
x
e minal o he d i ing p o o ype o he
same e minal a he ecei ing sys em. As can be seen
om he (yl, y2) phase plo , nea ly ideal synch oniza-
ion
is
ob ained. The same conclusion also applies
when conside ing a y-d i e scheme, bu no o a
z-
(a) (b)
FIGURE
3.
(a) y-coupled synch oniza ion esul s.
Ho .
axis: xl. Ve . axis: xz a he op,
z1
a he bo om.
(b)
-d i e synch oniza ion esul s.
Ho .
axis:
yp
Ve . axis:
yz
a he op,
l
a he bo om.
d i e con igu a ion as p edic ed by heo y [4]. Fig.4
illus a es he pe o mance o he whole secu e com-
munica ion scheme. Inpu signal (FigA(a)) consis s o
a segmen o speech. The wo s -case signal o noise
a io o he eco e ed signal (Fig.4(b)) is g ea e han
+40dB ( his occu s a e y low equencies) wi h less
han -0.2dB
loss
o he inpu signal powe . A highe
equencies, he signal- o-noise a io ises up o
+60dB, while e aining simila losses a he ecei e .
As can be seen om Fig.4, he ansmi ed signal
(Fig.4(c)) keeps no esemblance o he in o ma ion
con en .
1V.Re e ences
[
11
A.
Rod iguez-VBzquez and M. Delgado-Res i u-
o: “CMOS Design o Chao ic Oscilla o s Using
S a e Va iables:
A
Monoli hic Chua’s Ci cui ”.
IEEE T ansac ions
on
Ci cui s and Sys ems
II,
[2]
E
K ummenache and
N.
Joehl: “A 4MHz
CMOS Con inuous-Time Fil e wi h On-Chip
Au oma ic Tunings”.
IEEE
J.
Solid-s a e Ci -
cui s,
SC-23, pp. 750-758, 1988.
[3] M. Delgado-Res i u o and A. Rod iguez-VBzqu-
ez: “Swi ched-Cu en Chao ic Neu ons”.
Elec-
onics Le e s,
Vo1.30,
N.5,
pp. 429-430.
[4] M. Ogo zalek: “Taming Chaos--Pa I: Synch o-
niza ion”.
IEEE T ansac ions
on
Ci cui s and
Sys ems
I,
Vol.
40, N.lO, pp. 693-699, Oc . 1993.
V01.40, N.lO, pp. 596-613, Oc . 1993.
Chao ic Enc yp ion
-5.0
1
‘
,..-
O.0ms 100.0ms 200.0ms
Time (20msldi )
FIGURE
4.
Audio T ansmission Sys em.
179
ni
u:
START
0.001
n
20.00
10.00
STOP
PO
000 000
H
HEW:
100
1-L
ST:
44
6
sec
RAF.GE'
1-
..O,
T--lObBm
JIV
DIY
s ~n
0.001
H
10
00
10.00
STOP
20
000.000
H
R8h
100
H
S1-
44
6
5cc
RANGE.
8-
10.
T-
iOdBm
(e)
FIGURE
5.
Expe imen al Lissajous igu es (p ojec ions on o he (x,
y)
and
(x,z)
planes), and powe spec a
o :
(a)
Icon 2
=
1.0
PA
;
(b)
=
1.05
PA
;
(c)
Icon 2
=
1.125
PA
;
(d)
Icon 2
=
1.2
PA
;(e)
Icon 2
=
1.35
PA.
180
A
REF
@REF
lo
00
-10
00
'
dBm
1
[
~-
1
I-
DIY
OIV
STAili
0.001
Pi
10.00
20.00
STOP
PO
000
000
Hi
RBW:
10'2
HZ
ST:
44.6
sec
RANGC.
1-
10,
T-
-1OdOm
oi
OIV
B an-
0
001
iz
IO
00
30.00
STOP
20
000.000
WZ
i~Bn:
100
h7 8'?:44.6
DEC
UAhGF'2::
10
'i-?OOH71
(i)
FIGURE
6.
Expe imen al Lissajous
igu es
(p ojec ions on o he
(x,
y)
and
(x,z)
planes), and powe spec a
o :
(0
Zcon 2
=
1.52
pA
;
(g)
Zcon 2
=
1.67 pA
;(h)
Zcon 2
=
1.7
pA
;
(i)
Zcon 2
=
1.912
pA
;
(j)
=
1.97
PA.
181