Orientation of the Infrared Transition Moments for an α-Helix

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Orientation of the Infrared Transition Moments for an α-Helix Derek Marsh, Martin Müller, Franz-Josef Schmitt  Biophysical Journal  Volume 78, Issue 5, Pages 2499-2510 (May 2000) DOI: 10.1016/S0006-3495(00)76795-6 Copyright © 2000 The Biophysical Society Terms and Conditions

Figure 1 Orientation of an individual amide transition moment, m, relative to the molecular axis of an α-helix. The resultant amide transition moments of the entire helix, M‖ and M⊥ are oriented either parallel or perpendicular, respectively, to the c-axis. Biophysical Journal 2000 78, 2499-2510DOI: (10.1016/S0006-3495(00)76795-6) Copyright © 2000 The Biophysical Society Terms and Conditions

Figure 2 Geometric relations of the incident radiation to the orienting plane in an ATR experiment (lower) and in a transmission experiment (upper). The z-axis lies along the normal to the supporting plate, the x-axis is orthogonal to the z-axis and lies in the plane of incidence, and the y-axis is perpendicular to the plane of incidence. The radiation electric field vectors polarised parallel and perpendicular to the plane of incidence are Ep and Es, respectively. In the present experiments, the polypeptide (indicated schematically by the cylinder) is preferentially oriented with the y-axis as director, which is the direction of polishing of the silicon plate in the ATR experiment. Biophysical Journal 2000 78, 2499-2510DOI: (10.1016/S0006-3495(00)76795-6) Copyright © 2000 The Biophysical Society Terms and Conditions

Figure 3 Band fitting in the amide I, amide II, and carbonyl regions of the mid-IR spectrum from a film of the modified polyglutamate PG30 that was oriented: (A) on a silicon ATR plate that was polished in the y-direction (perpendicular to the plane of incidence), and (B) on the window of a silicon transmission cell oriented normal to the plane of incidence. ATR spectra (A) and transmission spectra (B) are shown for upper: radiation polarized perpendicular to the plane of incidence (s-polarization) and lower: radiation polarized parallel to the plane of incidence (p-polarization). Solid lines represent the original spectra, long dashes are the spectral fit, and short dashes are the individual fitted components. For transmission spectra, the fitted baseline is also shown. Biophysical Journal 2000 78, 2499-2510DOI: (10.1016/S0006-3495(00)76795-6) Copyright © 2000 The Biophysical Society Terms and Conditions

Figure 4 Orientations of the carbonyl bond (CO) and an individual amide transition moment (m) in the peptide plane, and of the peptide plane relative to the axis of the α-helix. The carbonyl bond makes an angle β with respect to the projection of the helix axis on the peptide plane; the transition moment makes an angle δM with the carbonyl bond; and the peptide plane is tilted at an angle α to the helix axis. Biophysical Journal 2000 78, 2499-2510DOI: (10.1016/S0006-3495(00)76795-6) Copyright © 2000 The Biophysical Society Terms and Conditions