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Volumn 93, Issue 23, 2004, Pages

Reproducible sequence generation in random neural ensembles

Author keywords

[No Author keywords available]

Indexed keywords

GENETIC CODES; LEARNING PHASES; MOTOR CONTROL; NEURONS;

EID: 42749104029     PISSN: 00319007     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevLett.93.238104     Document Type: Article
Times cited : (65)

References (16)
  • 3
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    • A. Selverston, Prog. Brain Res. 123, 247 (1999); O. Melamed et al. Trends Neurosci. 27, 11 (2004); J. W. Aldridge and K. C. Berridge J. Neurosci. 18, 2777 (1998).
    • (1999) Prog. Brain Res. , vol.123 , pp. 247
    • Selverston, A.1
  • 4
    • 0348047612 scopus 로고    scopus 로고
    • A. Selverston, Prog. Brain Res. 123, 247 (1999); O. Melamed et al. Trends Neurosci. 27, 11 (2004); J. W. Aldridge and K. C. Berridge J. Neurosci. 18, 2777 (1998).
    • (2004) Trends Neurosci. , vol.27 , pp. 11
    • Melamed, O.1
  • 5
    • 0032053432 scopus 로고    scopus 로고
    • A. Selverston, Prog. Brain Res. 123, 247 (1999); O. Melamed et al. Trends Neurosci. 27, 11 (2004); J. W. Aldridge and K. C. Berridge J. Neurosci. 18, 2777 (1998).
    • (1998) J. Neurosci. , vol.18 , pp. 2777
    • Aldridge, J.W.1    Berridge, K.C.2
  • 6
    • 0036834701 scopus 로고    scopus 로고
    • W. Maass et al. Neural Comput. 14, 2531 (2002); H. Jaeger and H. Haas, Science 304, 78 (2004).
    • (2002) Neural Comput. , vol.14 , pp. 2531
    • Maass, W.1
  • 7
    • 1842421269 scopus 로고    scopus 로고
    • W. Maass et al. Neural Comput. 14, 2531 (2002); H. Jaeger and H. Haas, Science 304, 78 (2004).
    • (2004) Science , vol.304 , pp. 78
    • Jaeger, H.1    Haas, H.2
  • 8
    • 0015868589 scopus 로고
    • H. R. Wilson and J. D. Cowan, Kybernetik 13, 55 (1973).In the model we analyze here we set the refractory periods to 0. Therefore, the rising and decay time constants of the model are identical.
    • (1973) Kybernetik , vol.13 , pp. 55
    • Wilson, H.R.1    Cowan, J.D.2
  • 12
    • 11344260167 scopus 로고    scopus 로고
    • note
    • The activity distribution is actually bimodal because there is always a peak in the absorbing state. The results that we analyze in the simulations are obtained without counting the absorbing states.
  • 13
    • 33749553474 scopus 로고
    • L. Glass, J. Chem. Phys. 63, 1325 (1975); L. Glass and J. Pasternack, J. Math. Biol. 6, 207 (1978).
    • (1975) J. Chem. Phys. , vol.63 , pp. 1325
    • Glass, L.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.