Abstract

A novel dual-channel chaotic synchronization configuration is proposed. This system is constructed on the basis of two unidirectionally coupled vertical-cavity surface-emitting lasers (VCSELs), where a VCSEL subjected to polarization-rotated optical feedback is used as a transmitter and the other VCSEL subjected to polarization-rotated optical injection is used as a receiver. The synchronization and communication performances of such a system are numerically investigated. The results show that, similar to polarization-preserved coupled system with polarization-preserved optical feedback at the T-VCSEL port and polarization-preserved optical injection at the R-VCSEL port, such polarization-rotated coupled system can also realize complete synchronization between each pair of linear polarization (LP) modes and the total output of T-VCSEL and R-VCSEL. Compared with the polarization-preserved coupled system, this proposed system has higher tolerance to mismatched parameters. Furthermore, the average intensities of two orthogonal LP modes are almost the same so that this framework may be used to realize dual-channel chaos communication. Under the additive chaos modulation (ACM) encryption scheme, the encoded messages can be successfully extracted for both of orthogonal LP modes.

© 2009 OSA

Full Article  |  PDF Article

References

  • View by:
  • |
  • |
  • |

  1. L. M. Pecora and T. L. Carroll, “Synchronization in chaotic systems,” Phys. Rev. Lett. 64(8), 821–824 (1990).
    [CrossRef] [PubMed]
  2. C. Masoller, “Anticipation in the synchronization of chaotic semiconductor lasers with optical feedback,” Phys. Rev. Lett. 86(13), 2782–2785 (2001).
    [CrossRef] [PubMed]
  3. A. Sanchez-Diaz, C. R. Mirasso, P. Colet, and P. Garcia-Fernandez, “Encoded Gbit/s digital communications with synchronized chaotic semiconductor lasers,” IEEE J. Quantum Electron. 35(3), 292–297 (1999).
    [CrossRef]
  4. G. Q. Xia, Z. M. Wu, and J. G. Wu, “Theory and simulation of dual-channel optical chaotic communication system,” Opt. Express 13(9), 3445–3453 (2005).
    [CrossRef] [PubMed]
  5. F. Rogister, A. Locquet, D. Pieroux, M. Sciamanna, O. Deparis, P. Mégret, and M. Blondel, “Secure communication scheme using chaotic laser diodes subject to incoherent optical feedback and incoherent optical injection,” Opt. Lett. 26(19), 1486–1488 (2001).
    [CrossRef]
  6. J. M. Buldú, J. García-Ojalvo, and M. C. Torrent, “Multimode synchronization and communication using unidirectionally coupled semiconductor lasers,” IEEE J. Quantum Electron. 40(6), 640–650 (2004).
    [CrossRef]
  7. M. S. Torre, C. Masoller, and K. A. Shore, “Synchronization of unidirectionally coupled multi-transverse-mode vertical-cavity surface-emitting lasers,” J. Opt. Soc. Am. B 21(10), 1772–1780 (2004).
    [CrossRef]
  8. I. Gatare, M. Sciamanna, A. Locquet, and K. Panajotov, “Influence of polarization mode competition on the synchronization of two unidirectionally coupled vertical-cavity surface-emitting lasers,” Opt. Lett. 32(12), 1629–1631 (2007).
    [CrossRef] [PubMed]
  9. D. Z. Zhong, G. Q. Xia, Z. M. Wu, and X. H. Jia, “Complete chaotic synchronization characteristics of the linear-polarization mode of vertical-cavity surface-emitting semiconductor lasers with isotropic optical feedback,” Opt. Commun. 281(6), 1698–1709 (2008).
    [CrossRef]
  10. Y. H. Hong, M. W. Lee, J. Paul, P. S. Spencer, and K. A. Shore, “Enhanced chaos synchronization in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers with polarization-preserved injection,” Opt. Lett. 33(6), 587–589 (2008).
    [CrossRef] [PubMed]
  11. Y. H. Hong, M. W. Lee, P. S. Spencer, and K. A. Shore, “Synchronization of chaos in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers,” Opt. Lett. 29(11), 1215–1217 (2004).
    [CrossRef] [PubMed]
  12. M. W. Lee, Y. Hong, and K. A. Shore, “Experimental demonstration of VCSEL-based chaotic optical communications,” IEEE Photon. Technol. Lett. 16(10), 2392–2394 (2004).
    [CrossRef]
  13. R. Ju, P. S. Spencer, and K. A. Shore, “Polarization-preserved and polarization-rotated synchronization of chaotic vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 41(12), 1461–1467 (2005).
    [CrossRef]
  14. M. Sciamanna, I. Gatare, A. Locquet, and K. Panajotov, “Polarization synchronization in unidirectionally coupled vertical-cavity surface-emitting lasers with orthogonal optical injection,” Phys. Rev. E 75, 056213–1-10 (2007).
  15. W. L. Zhang, W. Pan, B. Luo, X. F. Li, X. H. Zou, and M. Y. Wang, “Separate polarization modes synchronization and synchronization switches between vertical-cavity surface-emitting lasers,” Opt. Rev. 13(6), 443–448 (2006).
    [CrossRef]
  16. D. Z. Zhong and Z. M. Wu, “Complete chaotic synchronization mechanism of polarization mode of VCSEL with anisotropic optical feedback,” Opt. Commun. 282(8), 1631–1639 (2009).
    [CrossRef]
  17. D. Kanakidis, A. Argyris, A. Bogris, and D. Syvridis, ““Influence of the decoding process on the performance of chaos encrypted optical communication systems,” J. Lightwave Technol. 24, 335–341 (2006).
  18. M. W. Lee, J. Paul, C. Masoller, and K. A. Shore, “Observation of cascade complete chaos synchronisation with zero time lag in laser diodes,” J. Opt. Soc. Am. B 23(5), 846–851 (2006).
    [CrossRef]
  19. A. Locquet, C. Masoller, and C. R. Mirasso, “Synchronization regimes of optical-feedback-induced chaos in unidirectionally coupled semiconductor lasers,” Phys. Rev. E. 65, 056205–1-12 (2002).
  20. G. Q. Xia, Z. M. Wu, and J. F. Liao, “Theoretical investigations of cascaded chaotic synchronization and communication based on optoelectronic negative feedback semiconductor lasers,” Opt. Commun. 282(5), 1009–1015 (2009).
    [CrossRef]
  21. J. M. Liu, H. F. Chen, and S. Tang, “Synchronized chaotic optical communications at high bit-rates,” IEEE J. Quantum Electron. 38(9), 1184–1196 (2002).
    [CrossRef]
  22. C. Mirasso, J. Mulet, and C. Masoller, “Chaos shift keying encryption in chaotic external-cavity semiconductor lasers using a single-receiver scheme,” IEEE Photon. Technol. Lett. 14(4), 456–458 (2002).
    [CrossRef]
  23. T. Deng, G. Q. Xia, L. P. Cao, J. G. Chen, X. D. Lin, and Z. M. Wu, “Bidirectional chaos synchronization and communication in semiconductor lasers with optoelectronic feedback,” Opt. Commun. 282(11), 2243–2249 (2009).
    [CrossRef]
  24. S. Sivaprakasam and K. A. Shore, “Signal masking for chaotic optical communication using external-cavity diode lasers,” Opt. Lett. 24(17), 1200–1202 (1999).
    [CrossRef]
  25. J. M. Regalado, F. Prati, M. S. Miguel, and N. B. Abraham, “Polarization properties of vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 33(5), 765–783 (1997).
    [CrossRef]

2009 (3)

D. Z. Zhong and Z. M. Wu, “Complete chaotic synchronization mechanism of polarization mode of VCSEL with anisotropic optical feedback,” Opt. Commun. 282(8), 1631–1639 (2009).
[CrossRef]

G. Q. Xia, Z. M. Wu, and J. F. Liao, “Theoretical investigations of cascaded chaotic synchronization and communication based on optoelectronic negative feedback semiconductor lasers,” Opt. Commun. 282(5), 1009–1015 (2009).
[CrossRef]

T. Deng, G. Q. Xia, L. P. Cao, J. G. Chen, X. D. Lin, and Z. M. Wu, “Bidirectional chaos synchronization and communication in semiconductor lasers with optoelectronic feedback,” Opt. Commun. 282(11), 2243–2249 (2009).
[CrossRef]

2008 (2)

D. Z. Zhong, G. Q. Xia, Z. M. Wu, and X. H. Jia, “Complete chaotic synchronization characteristics of the linear-polarization mode of vertical-cavity surface-emitting semiconductor lasers with isotropic optical feedback,” Opt. Commun. 281(6), 1698–1709 (2008).
[CrossRef]

Y. H. Hong, M. W. Lee, J. Paul, P. S. Spencer, and K. A. Shore, “Enhanced chaos synchronization in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers with polarization-preserved injection,” Opt. Lett. 33(6), 587–589 (2008).
[CrossRef] [PubMed]

2007 (1)

2006 (3)

M. W. Lee, J. Paul, C. Masoller, and K. A. Shore, “Observation of cascade complete chaos synchronisation with zero time lag in laser diodes,” J. Opt. Soc. Am. B 23(5), 846–851 (2006).
[CrossRef]

W. L. Zhang, W. Pan, B. Luo, X. F. Li, X. H. Zou, and M. Y. Wang, “Separate polarization modes synchronization and synchronization switches between vertical-cavity surface-emitting lasers,” Opt. Rev. 13(6), 443–448 (2006).
[CrossRef]

D. Kanakidis, A. Argyris, A. Bogris, and D. Syvridis, ““Influence of the decoding process on the performance of chaos encrypted optical communication systems,” J. Lightwave Technol. 24, 335–341 (2006).

2005 (2)

R. Ju, P. S. Spencer, and K. A. Shore, “Polarization-preserved and polarization-rotated synchronization of chaotic vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 41(12), 1461–1467 (2005).
[CrossRef]

G. Q. Xia, Z. M. Wu, and J. G. Wu, “Theory and simulation of dual-channel optical chaotic communication system,” Opt. Express 13(9), 3445–3453 (2005).
[CrossRef] [PubMed]

2004 (4)

M. S. Torre, C. Masoller, and K. A. Shore, “Synchronization of unidirectionally coupled multi-transverse-mode vertical-cavity surface-emitting lasers,” J. Opt. Soc. Am. B 21(10), 1772–1780 (2004).
[CrossRef]

Y. H. Hong, M. W. Lee, P. S. Spencer, and K. A. Shore, “Synchronization of chaos in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers,” Opt. Lett. 29(11), 1215–1217 (2004).
[CrossRef] [PubMed]

M. W. Lee, Y. Hong, and K. A. Shore, “Experimental demonstration of VCSEL-based chaotic optical communications,” IEEE Photon. Technol. Lett. 16(10), 2392–2394 (2004).
[CrossRef]

J. M. Buldú, J. García-Ojalvo, and M. C. Torrent, “Multimode synchronization and communication using unidirectionally coupled semiconductor lasers,” IEEE J. Quantum Electron. 40(6), 640–650 (2004).
[CrossRef]

2002 (2)

J. M. Liu, H. F. Chen, and S. Tang, “Synchronized chaotic optical communications at high bit-rates,” IEEE J. Quantum Electron. 38(9), 1184–1196 (2002).
[CrossRef]

C. Mirasso, J. Mulet, and C. Masoller, “Chaos shift keying encryption in chaotic external-cavity semiconductor lasers using a single-receiver scheme,” IEEE Photon. Technol. Lett. 14(4), 456–458 (2002).
[CrossRef]

2001 (2)

1999 (2)

A. Sanchez-Diaz, C. R. Mirasso, P. Colet, and P. Garcia-Fernandez, “Encoded Gbit/s digital communications with synchronized chaotic semiconductor lasers,” IEEE J. Quantum Electron. 35(3), 292–297 (1999).
[CrossRef]

S. Sivaprakasam and K. A. Shore, “Signal masking for chaotic optical communication using external-cavity diode lasers,” Opt. Lett. 24(17), 1200–1202 (1999).
[CrossRef]

1997 (1)

J. M. Regalado, F. Prati, M. S. Miguel, and N. B. Abraham, “Polarization properties of vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 33(5), 765–783 (1997).
[CrossRef]

1990 (1)

L. M. Pecora and T. L. Carroll, “Synchronization in chaotic systems,” Phys. Rev. Lett. 64(8), 821–824 (1990).
[CrossRef] [PubMed]

Abraham, N. B.

J. M. Regalado, F. Prati, M. S. Miguel, and N. B. Abraham, “Polarization properties of vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 33(5), 765–783 (1997).
[CrossRef]

Argyris, A.

D. Kanakidis, A. Argyris, A. Bogris, and D. Syvridis, ““Influence of the decoding process on the performance of chaos encrypted optical communication systems,” J. Lightwave Technol. 24, 335–341 (2006).

Blondel, M.

Bogris, A.

D. Kanakidis, A. Argyris, A. Bogris, and D. Syvridis, ““Influence of the decoding process on the performance of chaos encrypted optical communication systems,” J. Lightwave Technol. 24, 335–341 (2006).

Buldú, J. M.

J. M. Buldú, J. García-Ojalvo, and M. C. Torrent, “Multimode synchronization and communication using unidirectionally coupled semiconductor lasers,” IEEE J. Quantum Electron. 40(6), 640–650 (2004).
[CrossRef]

Cao, L. P.

T. Deng, G. Q. Xia, L. P. Cao, J. G. Chen, X. D. Lin, and Z. M. Wu, “Bidirectional chaos synchronization and communication in semiconductor lasers with optoelectronic feedback,” Opt. Commun. 282(11), 2243–2249 (2009).
[CrossRef]

Carroll, T. L.

L. M. Pecora and T. L. Carroll, “Synchronization in chaotic systems,” Phys. Rev. Lett. 64(8), 821–824 (1990).
[CrossRef] [PubMed]

Chen, H. F.

J. M. Liu, H. F. Chen, and S. Tang, “Synchronized chaotic optical communications at high bit-rates,” IEEE J. Quantum Electron. 38(9), 1184–1196 (2002).
[CrossRef]

Chen, J. G.

T. Deng, G. Q. Xia, L. P. Cao, J. G. Chen, X. D. Lin, and Z. M. Wu, “Bidirectional chaos synchronization and communication in semiconductor lasers with optoelectronic feedback,” Opt. Commun. 282(11), 2243–2249 (2009).
[CrossRef]

Colet, P.

A. Sanchez-Diaz, C. R. Mirasso, P. Colet, and P. Garcia-Fernandez, “Encoded Gbit/s digital communications with synchronized chaotic semiconductor lasers,” IEEE J. Quantum Electron. 35(3), 292–297 (1999).
[CrossRef]

Deng, T.

T. Deng, G. Q. Xia, L. P. Cao, J. G. Chen, X. D. Lin, and Z. M. Wu, “Bidirectional chaos synchronization and communication in semiconductor lasers with optoelectronic feedback,” Opt. Commun. 282(11), 2243–2249 (2009).
[CrossRef]

Deparis, O.

Garcia-Fernandez, P.

A. Sanchez-Diaz, C. R. Mirasso, P. Colet, and P. Garcia-Fernandez, “Encoded Gbit/s digital communications with synchronized chaotic semiconductor lasers,” IEEE J. Quantum Electron. 35(3), 292–297 (1999).
[CrossRef]

García-Ojalvo, J.

J. M. Buldú, J. García-Ojalvo, and M. C. Torrent, “Multimode synchronization and communication using unidirectionally coupled semiconductor lasers,” IEEE J. Quantum Electron. 40(6), 640–650 (2004).
[CrossRef]

Gatare, I.

Hong, Y.

M. W. Lee, Y. Hong, and K. A. Shore, “Experimental demonstration of VCSEL-based chaotic optical communications,” IEEE Photon. Technol. Lett. 16(10), 2392–2394 (2004).
[CrossRef]

Hong, Y. H.

Y. H. Hong, M. W. Lee, J. Paul, P. S. Spencer, and K. A. Shore, “Enhanced chaos synchronization in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers with polarization-preserved injection,” Opt. Lett. 33(6), 587–589 (2008).
[CrossRef] [PubMed]

Y. H. Hong, M. W. Lee, P. S. Spencer, and K. A. Shore, “Synchronization of chaos in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers,” Opt. Lett. 29(11), 1215–1217 (2004).
[CrossRef] [PubMed]

Jia, X. H.

D. Z. Zhong, G. Q. Xia, Z. M. Wu, and X. H. Jia, “Complete chaotic synchronization characteristics of the linear-polarization mode of vertical-cavity surface-emitting semiconductor lasers with isotropic optical feedback,” Opt. Commun. 281(6), 1698–1709 (2008).
[CrossRef]

Ju, R.

R. Ju, P. S. Spencer, and K. A. Shore, “Polarization-preserved and polarization-rotated synchronization of chaotic vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 41(12), 1461–1467 (2005).
[CrossRef]

Kanakidis, D.

D. Kanakidis, A. Argyris, A. Bogris, and D. Syvridis, ““Influence of the decoding process on the performance of chaos encrypted optical communication systems,” J. Lightwave Technol. 24, 335–341 (2006).

Lee, M. W.

Y. H. Hong, M. W. Lee, J. Paul, P. S. Spencer, and K. A. Shore, “Enhanced chaos synchronization in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers with polarization-preserved injection,” Opt. Lett. 33(6), 587–589 (2008).
[CrossRef] [PubMed]

M. W. Lee, J. Paul, C. Masoller, and K. A. Shore, “Observation of cascade complete chaos synchronisation with zero time lag in laser diodes,” J. Opt. Soc. Am. B 23(5), 846–851 (2006).
[CrossRef]

Y. H. Hong, M. W. Lee, P. S. Spencer, and K. A. Shore, “Synchronization of chaos in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers,” Opt. Lett. 29(11), 1215–1217 (2004).
[CrossRef] [PubMed]

M. W. Lee, Y. Hong, and K. A. Shore, “Experimental demonstration of VCSEL-based chaotic optical communications,” IEEE Photon. Technol. Lett. 16(10), 2392–2394 (2004).
[CrossRef]

Li, X. F.

W. L. Zhang, W. Pan, B. Luo, X. F. Li, X. H. Zou, and M. Y. Wang, “Separate polarization modes synchronization and synchronization switches between vertical-cavity surface-emitting lasers,” Opt. Rev. 13(6), 443–448 (2006).
[CrossRef]

Liao, J. F.

G. Q. Xia, Z. M. Wu, and J. F. Liao, “Theoretical investigations of cascaded chaotic synchronization and communication based on optoelectronic negative feedback semiconductor lasers,” Opt. Commun. 282(5), 1009–1015 (2009).
[CrossRef]

Lin, X. D.

T. Deng, G. Q. Xia, L. P. Cao, J. G. Chen, X. D. Lin, and Z. M. Wu, “Bidirectional chaos synchronization and communication in semiconductor lasers with optoelectronic feedback,” Opt. Commun. 282(11), 2243–2249 (2009).
[CrossRef]

Liu, J. M.

J. M. Liu, H. F. Chen, and S. Tang, “Synchronized chaotic optical communications at high bit-rates,” IEEE J. Quantum Electron. 38(9), 1184–1196 (2002).
[CrossRef]

Locquet, A.

Luo, B.

W. L. Zhang, W. Pan, B. Luo, X. F. Li, X. H. Zou, and M. Y. Wang, “Separate polarization modes synchronization and synchronization switches between vertical-cavity surface-emitting lasers,” Opt. Rev. 13(6), 443–448 (2006).
[CrossRef]

Masoller, C.

M. W. Lee, J. Paul, C. Masoller, and K. A. Shore, “Observation of cascade complete chaos synchronisation with zero time lag in laser diodes,” J. Opt. Soc. Am. B 23(5), 846–851 (2006).
[CrossRef]

M. S. Torre, C. Masoller, and K. A. Shore, “Synchronization of unidirectionally coupled multi-transverse-mode vertical-cavity surface-emitting lasers,” J. Opt. Soc. Am. B 21(10), 1772–1780 (2004).
[CrossRef]

C. Mirasso, J. Mulet, and C. Masoller, “Chaos shift keying encryption in chaotic external-cavity semiconductor lasers using a single-receiver scheme,” IEEE Photon. Technol. Lett. 14(4), 456–458 (2002).
[CrossRef]

C. Masoller, “Anticipation in the synchronization of chaotic semiconductor lasers with optical feedback,” Phys. Rev. Lett. 86(13), 2782–2785 (2001).
[CrossRef] [PubMed]

Mégret, P.

Miguel, M. S.

J. M. Regalado, F. Prati, M. S. Miguel, and N. B. Abraham, “Polarization properties of vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 33(5), 765–783 (1997).
[CrossRef]

Mirasso, C.

C. Mirasso, J. Mulet, and C. Masoller, “Chaos shift keying encryption in chaotic external-cavity semiconductor lasers using a single-receiver scheme,” IEEE Photon. Technol. Lett. 14(4), 456–458 (2002).
[CrossRef]

Mirasso, C. R.

A. Sanchez-Diaz, C. R. Mirasso, P. Colet, and P. Garcia-Fernandez, “Encoded Gbit/s digital communications with synchronized chaotic semiconductor lasers,” IEEE J. Quantum Electron. 35(3), 292–297 (1999).
[CrossRef]

Mulet, J.

C. Mirasso, J. Mulet, and C. Masoller, “Chaos shift keying encryption in chaotic external-cavity semiconductor lasers using a single-receiver scheme,” IEEE Photon. Technol. Lett. 14(4), 456–458 (2002).
[CrossRef]

Pan, W.

W. L. Zhang, W. Pan, B. Luo, X. F. Li, X. H. Zou, and M. Y. Wang, “Separate polarization modes synchronization and synchronization switches between vertical-cavity surface-emitting lasers,” Opt. Rev. 13(6), 443–448 (2006).
[CrossRef]

Panajotov, K.

Paul, J.

Pecora, L. M.

L. M. Pecora and T. L. Carroll, “Synchronization in chaotic systems,” Phys. Rev. Lett. 64(8), 821–824 (1990).
[CrossRef] [PubMed]

Pieroux, D.

Prati, F.

J. M. Regalado, F. Prati, M. S. Miguel, and N. B. Abraham, “Polarization properties of vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 33(5), 765–783 (1997).
[CrossRef]

Regalado, J. M.

J. M. Regalado, F. Prati, M. S. Miguel, and N. B. Abraham, “Polarization properties of vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 33(5), 765–783 (1997).
[CrossRef]

Rogister, F.

Sanchez-Diaz, A.

A. Sanchez-Diaz, C. R. Mirasso, P. Colet, and P. Garcia-Fernandez, “Encoded Gbit/s digital communications with synchronized chaotic semiconductor lasers,” IEEE J. Quantum Electron. 35(3), 292–297 (1999).
[CrossRef]

Sciamanna, M.

Shore, K. A.

Y. H. Hong, M. W. Lee, J. Paul, P. S. Spencer, and K. A. Shore, “Enhanced chaos synchronization in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers with polarization-preserved injection,” Opt. Lett. 33(6), 587–589 (2008).
[CrossRef] [PubMed]

M. W. Lee, J. Paul, C. Masoller, and K. A. Shore, “Observation of cascade complete chaos synchronisation with zero time lag in laser diodes,” J. Opt. Soc. Am. B 23(5), 846–851 (2006).
[CrossRef]

R. Ju, P. S. Spencer, and K. A. Shore, “Polarization-preserved and polarization-rotated synchronization of chaotic vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 41(12), 1461–1467 (2005).
[CrossRef]

Y. H. Hong, M. W. Lee, P. S. Spencer, and K. A. Shore, “Synchronization of chaos in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers,” Opt. Lett. 29(11), 1215–1217 (2004).
[CrossRef] [PubMed]

M. W. Lee, Y. Hong, and K. A. Shore, “Experimental demonstration of VCSEL-based chaotic optical communications,” IEEE Photon. Technol. Lett. 16(10), 2392–2394 (2004).
[CrossRef]

M. S. Torre, C. Masoller, and K. A. Shore, “Synchronization of unidirectionally coupled multi-transverse-mode vertical-cavity surface-emitting lasers,” J. Opt. Soc. Am. B 21(10), 1772–1780 (2004).
[CrossRef]

S. Sivaprakasam and K. A. Shore, “Signal masking for chaotic optical communication using external-cavity diode lasers,” Opt. Lett. 24(17), 1200–1202 (1999).
[CrossRef]

Sivaprakasam, S.

Spencer, P. S.

Y. H. Hong, M. W. Lee, J. Paul, P. S. Spencer, and K. A. Shore, “Enhanced chaos synchronization in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers with polarization-preserved injection,” Opt. Lett. 33(6), 587–589 (2008).
[CrossRef] [PubMed]

R. Ju, P. S. Spencer, and K. A. Shore, “Polarization-preserved and polarization-rotated synchronization of chaotic vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 41(12), 1461–1467 (2005).
[CrossRef]

Y. H. Hong, M. W. Lee, P. S. Spencer, and K. A. Shore, “Synchronization of chaos in unidirectionally coupled vertical-cavity surface-emitting semiconductor lasers,” Opt. Lett. 29(11), 1215–1217 (2004).
[CrossRef] [PubMed]

Syvridis, D.

D. Kanakidis, A. Argyris, A. Bogris, and D. Syvridis, ““Influence of the decoding process on the performance of chaos encrypted optical communication systems,” J. Lightwave Technol. 24, 335–341 (2006).

Tang, S.

J. M. Liu, H. F. Chen, and S. Tang, “Synchronized chaotic optical communications at high bit-rates,” IEEE J. Quantum Electron. 38(9), 1184–1196 (2002).
[CrossRef]

Torre, M. S.

Torrent, M. C.

J. M. Buldú, J. García-Ojalvo, and M. C. Torrent, “Multimode synchronization and communication using unidirectionally coupled semiconductor lasers,” IEEE J. Quantum Electron. 40(6), 640–650 (2004).
[CrossRef]

Wang, M. Y.

W. L. Zhang, W. Pan, B. Luo, X. F. Li, X. H. Zou, and M. Y. Wang, “Separate polarization modes synchronization and synchronization switches between vertical-cavity surface-emitting lasers,” Opt. Rev. 13(6), 443–448 (2006).
[CrossRef]

Wu, J. G.

Wu, Z. M.

G. Q. Xia, Z. M. Wu, and J. F. Liao, “Theoretical investigations of cascaded chaotic synchronization and communication based on optoelectronic negative feedback semiconductor lasers,” Opt. Commun. 282(5), 1009–1015 (2009).
[CrossRef]

T. Deng, G. Q. Xia, L. P. Cao, J. G. Chen, X. D. Lin, and Z. M. Wu, “Bidirectional chaos synchronization and communication in semiconductor lasers with optoelectronic feedback,” Opt. Commun. 282(11), 2243–2249 (2009).
[CrossRef]

D. Z. Zhong and Z. M. Wu, “Complete chaotic synchronization mechanism of polarization mode of VCSEL with anisotropic optical feedback,” Opt. Commun. 282(8), 1631–1639 (2009).
[CrossRef]

D. Z. Zhong, G. Q. Xia, Z. M. Wu, and X. H. Jia, “Complete chaotic synchronization characteristics of the linear-polarization mode of vertical-cavity surface-emitting semiconductor lasers with isotropic optical feedback,” Opt. Commun. 281(6), 1698–1709 (2008).
[CrossRef]

G. Q. Xia, Z. M. Wu, and J. G. Wu, “Theory and simulation of dual-channel optical chaotic communication system,” Opt. Express 13(9), 3445–3453 (2005).
[CrossRef] [PubMed]

Xia, G. Q.

T. Deng, G. Q. Xia, L. P. Cao, J. G. Chen, X. D. Lin, and Z. M. Wu, “Bidirectional chaos synchronization and communication in semiconductor lasers with optoelectronic feedback,” Opt. Commun. 282(11), 2243–2249 (2009).
[CrossRef]

G. Q. Xia, Z. M. Wu, and J. F. Liao, “Theoretical investigations of cascaded chaotic synchronization and communication based on optoelectronic negative feedback semiconductor lasers,” Opt. Commun. 282(5), 1009–1015 (2009).
[CrossRef]

D. Z. Zhong, G. Q. Xia, Z. M. Wu, and X. H. Jia, “Complete chaotic synchronization characteristics of the linear-polarization mode of vertical-cavity surface-emitting semiconductor lasers with isotropic optical feedback,” Opt. Commun. 281(6), 1698–1709 (2008).
[CrossRef]

G. Q. Xia, Z. M. Wu, and J. G. Wu, “Theory and simulation of dual-channel optical chaotic communication system,” Opt. Express 13(9), 3445–3453 (2005).
[CrossRef] [PubMed]

Zhang, W. L.

W. L. Zhang, W. Pan, B. Luo, X. F. Li, X. H. Zou, and M. Y. Wang, “Separate polarization modes synchronization and synchronization switches between vertical-cavity surface-emitting lasers,” Opt. Rev. 13(6), 443–448 (2006).
[CrossRef]

Zhong, D. Z.

D. Z. Zhong and Z. M. Wu, “Complete chaotic synchronization mechanism of polarization mode of VCSEL with anisotropic optical feedback,” Opt. Commun. 282(8), 1631–1639 (2009).
[CrossRef]

D. Z. Zhong, G. Q. Xia, Z. M. Wu, and X. H. Jia, “Complete chaotic synchronization characteristics of the linear-polarization mode of vertical-cavity surface-emitting semiconductor lasers with isotropic optical feedback,” Opt. Commun. 281(6), 1698–1709 (2008).
[CrossRef]

Zou, X. H.

W. L. Zhang, W. Pan, B. Luo, X. F. Li, X. H. Zou, and M. Y. Wang, “Separate polarization modes synchronization and synchronization switches between vertical-cavity surface-emitting lasers,” Opt. Rev. 13(6), 443–448 (2006).
[CrossRef]

IEEE J. Quantum Electron. (5)

A. Sanchez-Diaz, C. R. Mirasso, P. Colet, and P. Garcia-Fernandez, “Encoded Gbit/s digital communications with synchronized chaotic semiconductor lasers,” IEEE J. Quantum Electron. 35(3), 292–297 (1999).
[CrossRef]

J. M. Buldú, J. García-Ojalvo, and M. C. Torrent, “Multimode synchronization and communication using unidirectionally coupled semiconductor lasers,” IEEE J. Quantum Electron. 40(6), 640–650 (2004).
[CrossRef]

R. Ju, P. S. Spencer, and K. A. Shore, “Polarization-preserved and polarization-rotated synchronization of chaotic vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 41(12), 1461–1467 (2005).
[CrossRef]

J. M. Liu, H. F. Chen, and S. Tang, “Synchronized chaotic optical communications at high bit-rates,” IEEE J. Quantum Electron. 38(9), 1184–1196 (2002).
[CrossRef]

J. M. Regalado, F. Prati, M. S. Miguel, and N. B. Abraham, “Polarization properties of vertical-cavity surface-emitting lasers,” IEEE J. Quantum Electron. 33(5), 765–783 (1997).
[CrossRef]

IEEE Photon. Technol. Lett. (2)

C. Mirasso, J. Mulet, and C. Masoller, “Chaos shift keying encryption in chaotic external-cavity semiconductor lasers using a single-receiver scheme,” IEEE Photon. Technol. Lett. 14(4), 456–458 (2002).
[CrossRef]

M. W. Lee, Y. Hong, and K. A. Shore, “Experimental demonstration of VCSEL-based chaotic optical communications,” IEEE Photon. Technol. Lett. 16(10), 2392–2394 (2004).
[CrossRef]

J. (1)

D. Kanakidis, A. Argyris, A. Bogris, and D. Syvridis, ““Influence of the decoding process on the performance of chaos encrypted optical communication systems,” J. Lightwave Technol. 24, 335–341 (2006).

J. Opt. Soc. Am. B (2)

Opt. Commun. (4)

T. Deng, G. Q. Xia, L. P. Cao, J. G. Chen, X. D. Lin, and Z. M. Wu, “Bidirectional chaos synchronization and communication in semiconductor lasers with optoelectronic feedback,” Opt. Commun. 282(11), 2243–2249 (2009).
[CrossRef]

D. Z. Zhong and Z. M. Wu, “Complete chaotic synchronization mechanism of polarization mode of VCSEL with anisotropic optical feedback,” Opt. Commun. 282(8), 1631–1639 (2009).
[CrossRef]

G. Q. Xia, Z. M. Wu, and J. F. Liao, “Theoretical investigations of cascaded chaotic synchronization and communication based on optoelectronic negative feedback semiconductor lasers,” Opt. Commun. 282(5), 1009–1015 (2009).
[CrossRef]

D. Z. Zhong, G. Q. Xia, Z. M. Wu, and X. H. Jia, “Complete chaotic synchronization characteristics of the linear-polarization mode of vertical-cavity surface-emitting semiconductor lasers with isotropic optical feedback,” Opt. Commun. 281(6), 1698–1709 (2008).
[CrossRef]

Opt. Express (1)

Opt. Lett. (5)

Opt. Rev. (1)

W. L. Zhang, W. Pan, B. Luo, X. F. Li, X. H. Zou, and M. Y. Wang, “Separate polarization modes synchronization and synchronization switches between vertical-cavity surface-emitting lasers,” Opt. Rev. 13(6), 443–448 (2006).
[CrossRef]

Phys. Rev. Lett. (2)

L. M. Pecora and T. L. Carroll, “Synchronization in chaotic systems,” Phys. Rev. Lett. 64(8), 821–824 (1990).
[CrossRef] [PubMed]

C. Masoller, “Anticipation in the synchronization of chaotic semiconductor lasers with optical feedback,” Phys. Rev. Lett. 86(13), 2782–2785 (2001).
[CrossRef] [PubMed]

Other (2)

M. Sciamanna, I. Gatare, A. Locquet, and K. Panajotov, “Polarization synchronization in unidirectionally coupled vertical-cavity surface-emitting lasers with orthogonal optical injection,” Phys. Rev. E 75, 056213–1-10 (2007).

A. Locquet, C. Masoller, and C. R. Mirasso, “Synchronization regimes of optical-feedback-induced chaos in unidirectionally coupled semiconductor lasers,” Phys. Rev. E. 65, 056205–1-12 (2002).

Cited By

OSA participates in CrossRef's Cited-By Linking service. Citing articles from OSA journals and other participating publishers are listed here.

Alert me when this article is cited.


Figures (5)

Fig. 1
Fig. 1

Schematic diagram for the dual-channel chaos communication system based on the unidirectionally VCSELs subject to polarization-rotated optical feedback and polarization-rotated optical injection. T-VCSEL: transmitter-VCSEL; R-VCSEL: receiver-VCSEL; PBS: polarization beam splitter; HWP: half-wave plate; BS: beam splitter; ISO: optical isolator; M: mirror; PD: photodetector.

Fig. 2
Fig. 2

P-I curves for (a) polarization-rotated optical feedback and (b) polarization-preserved optical feedback.

Fig. 3
Fig. 3

(a) Time series of x LP, y LP and total output, and (b) corresponding cross-correlation coefficients.

Fig. 4
Fig. 4

Maximum of cross correlation coefficient between x LP, y LP and total output of T-VCSEL and R-VCSEL versus different mismatched parameters, where (a) and (b) is for polarization-rotated coupled system and polarization-preserved coupled system, respectively, dotted, solid and dashed lines correspond to x LP, y LP and total output, respectively.

Fig. 5
Fig. 5

Original message mx,y (t) and recovered message mx,y (t), where (a) and (b) correspond to x LP mode and y LP mode, respectively.

Equations (8)

Equations on this page are rendered with MathJax. Learn more.

dEx,yTdt=k(1+iα)[(NT1)Ex,yT±inTEy,xT]±(γaiγp)Ex,yT+fEy,xT(tτ)eiωTτ+Fx,yT
dEx,yRdt=k(1+iα)[(NR1)Ex,yR±inREy,xR]±(γaiγp)Ex,yR+ηEy,xT(tτc)e-iωTτc+iΔωt+Fx,yR
dNT,Rdt=γ[NT,Rμ+NT,R(|ExT,R|2+|EyT,R|2)]iγnT,R(EyT,RExT,R*ExT,REyT,R*)
dnT,Rdt=γsnT,RγnT,R(|ExT,R|2+|EyT,R|2)iγNT,R(EyT,RExT,R*ExT,REyT,R*)
FxT,R=βsp/2(NT,R+nT,Rξ1T,R+NT,RnT,Rξ2T,R)
FyT,R=iβsp/2(NT,R+nT,Rξ1T,RNT,RnT,Rξ2T,R)
Cx,y(Δt)=[Ix,yT(tΔt)Ix,yT(tΔt)][Ix,yR(t)Ix,yR(t)][Ix,yT(tΔt)Ix,yT(tΔt)]21/2[Ix,yR(t)Ix,yR(t)]21/2
Δα=αRαTαT,Δk=kRkTkT,Δγ=γRγTγT,Δγp=γpRγpTγpT,Δγs=γsRγsTγsT,Δγa=γaRγaTγaT

Metrics