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Volumn 106, Issue 24, 1997, Pages 10099-10104

Finding transition states using contangency curves

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0000809763     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.474043     Document Type: Article
Times cited : (16)

References (34)
  • 10
    • 85033304988 scopus 로고    scopus 로고
    • note
    • Properly speaking, the "transition state" should be called the "transition microstate" since only a single conformation is specified. It is important because it usually lies near the center of the extended "transition region" which governs transition rates, particularly at low temperatures.
  • 14
    • 85033285281 scopus 로고    scopus 로고
    • note
    • Y.
  • 15
    • 85033303927 scopus 로고    scopus 로고
    • note
    • If necessary, the labeling of metastable states X and Y can be reversed so that Eq. (11) will hold.
  • 16
    • 85033301337 scopus 로고    scopus 로고
    • note
    • s.
  • 17
    • 85033320360 scopus 로고    scopus 로고
    • note
    • g in lowest order.
  • 18
    • 85033317731 scopus 로고    scopus 로고
    • note
    • s.
  • 20
    • 85033321521 scopus 로고    scopus 로고
    • note
    • i is large will be appropriate.
  • 27
    • 85033310531 scopus 로고    scopus 로고
    • note
    • Both these numbers are ∼15% higher than those calculated using MM2 (Ref. 24) and CHARMM (Ref. 2) potentials with explicit hydrogen atoms.
  • 28
    • 85033316934 scopus 로고    scopus 로고
    • note
    • The Monte Carlo sampling was modified to accommodate the degeneracies associated with the rigid-body translational and rotational invariance. The translational degeneracy was eliminated simply by translating the center-of-mass of each sampled conformation back to the origin. The rotational degeneracy was eliminated by rotating each sampled conformation to minimize its mean-square deviation from the reference isomer conformation using the procedure of Ref. 34. The formal justification for this procedure will be described in a subsequent publication.
  • 30
    • 85033292435 scopus 로고    scopus 로고
    • note
    • -5.
  • 31
    • 85033313169 scopus 로고    scopus 로고
    • note
    • i.
  • 32
    • 85033279885 scopus 로고    scopus 로고
    • note
    • BT=0, i.e., when script C sign was determined just using the Hessian. This is probably so only because this problem is relatively simple - we expect that script C sign derived from the Hessian will be much less useful in macromolecular problems. A stable bi-Gaussian approximation was not obtained at temperatures much above ≈2.5 kcal/mol. At higher temperatures the iterative self-consistent quasi-harmonic fitting method (Ref. 29) would not converge to model each metastable state separately - the separate solutions became unstable and only a single Gaussian modeling the combination of both states was stable.
  • 33
    • 85033321284 scopus 로고    scopus 로고
    • note
    • X).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.