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Physical Review Letters

Volumn 74, Issue 25, 1995, Pages 5024-5027

Entrainment and communication with dissipative pseudorandom dynamics

(2) Gershenfeld, N a Grinstein, G b

a MASSACHUSETTS INSTITUTE OF TECHNOLOGY (United States)

b IBM T J WATSON RESEARCH CENTER (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0000271689 PISSN: 00319007 EISSN: None Source Type: Journal
DOI: 10.1103/PhysRevLett.74.5024 Document Type: Article

Times cited : (38)

References (17)

1
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- McGraw-Hill, New York
- (1994) Spread Spectrum Communications Handbook
- Simon, M.K.¹

2
- 84927860885
- Pseudorandom noise is a deterministic signal whose properties mimic those of random noise. See Ref. [c1] for a precise definition.

3
- 84927860884
- This description of modulation schemes omits the possible extra step of modulation and demodulation by a communications carrier. See Ref. [c1].

4
- 0343689904
- (1990) Phys. Rev. Lett. , vol.64 , pp. 821
- Pecora, L.M.¹ Carroll, T.L.²

5
- 84927860883
- Tresser, C.¹ Worfolk, P.²

6
- 12044251580
- (1993) Phys. Rev. Lett. , vol.71 , pp. 65
- Cuomo, K.M.¹ Oppenheim, A.V.²

7
- 0011224204
- A SIMPLE WAY TO SYNCHRONIZE CHAOTIC SYSTEMS WITH APPLICATIONS TO SECURE COMMUNICATION SYSTEMS
- (1993) International Journal of Bifurcation and Chaos , vol.3 , pp. 1619
- Wu, C.H.¹ Chua, L.O.²

8
- 0003424544
- Applied Mathematical Sciences Vol. 68, Springer-Verlag, New York
- (1988) Infinite-Dimensional Dynamical Systems in Mechanics and Physics,
- Temam, R.¹

9
- 33751278790
- (1991) J. Stat. Phys. , vol.65 , pp. 579
- Sauer, T.¹ Yorke, J.A.² Casdagli, M.³

10
- 0003959092
- For secure cryptographic systems see, for example, G. J. Simmons, IEEE Press, Piscataway
- (1992) Contemporary Cryptology: The Science of Information Integrity,

11
- 0002235636
- (1981) Math. Systems Theory , vol.14 , pp. 13
- Toffoli, T.¹

12
- 0027681856
- (1993) IEEE Phot. Tech. Lett. , vol.5 , pp. 1238
- Davidson, F.¹ Field, C.T.²

13
- 84927860882
- With regard to local stability, it is easily shown that the locked state is superstable; i.e., the appropriate Lyapunov exponent is -∞.

14
- 4243489552
- (1990) Phys. Rev. Lett. , vol.64 , pp. 1196
- Ott, E.¹ Grebogi, C.² Yorke, J.A.³

15
- 11944261590
- (1992) Phys. Rev. Lett. , vol.68 , pp. 1259
- Roy, R.¹

16
- 84927860881
- This is a trivial kind of synchronization, similar to a self-synchronizing spread-spectrum configuration; see Ref. [c1].

17
- 84927860880
- One can also satisfy this logical relationship with products instead of sums of lags.

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