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锰肌红蛋白及其叠氮配合物的共振拉曼光谱。将一个新的电荷转移带归属为叠氮(π)到卟啉(π)的跃迁。

Resonance Raman spectra of manganese myoglobin and its azide complex. Assignment of a new charge-transfer band to azide (pi) to porphyrin (pi) transition.

作者信息

Yu N T, Tsubaki M

出版信息

Biochemistry. 1980 Sep 30;19(20):4647-53. doi: 10.1021/bi00561a017.

Abstract

The enhancement of bound azide vibrations at 650 [depolarized (dp), bending] and 2039 cm-1 (dp, antisymmetric stretch) upon excitation at approximately 400-460 nm indicates the existence of a new charge-transfer transition in manganese(III) myoglobin-azide complex. The assignments of these two vibrational modes are based on the agreement of their 15N3 isotope shifts (22 and 70 cm-1) with the calculated values (22 and 69 cm-1), the depolarized nature, and their close proximity to the corresponding vibrations in ionized azide. The Mn-(III)-N3 stretch has not been observed in the present study although the Fe(III)-N3 stretch at 413 cm-1 (polarized) was reported [Asher, S. A., Vickery, L. E., Schuster, T. M., & Sauer, K. (1977) Biochemistry 16, 5849]. The RR spectra of MnIIIMb-azide between 150 and 300 cm-1 differ dramatically from those of FeIIIMb-azide exicted in the 640-nm charge-transfer band or near the Soret band. There are lines at 170 and 282 cm-1 (both polarized) in the MnIIIMb-azide spectra which exhibit extremely large resonance enhancements and are unshifted by 15N3 isotope substitution. These two lines, having no analogue in other heme protein spectra, may be tentatively assigned to the out-of-plane porphyrin ring vibrations, with the latter involving significant Mn(III)-N(pyrrole) stretch. The enhancement of non totally symmetric azide modes suggests that the charge-transfer state may be mixed with other excited electronic states (possibly band Va or band VI) via Herzberg-Teller vibronic couplings. The lack of enhancement of the Mn(III)-N3 stretch leads to our present assignment of azide (pi) to porphyrin (pi) charge-transfer transition rather than azide (pi) to metal (dz2) or azide (n) to metal (dz2).

摘要

在约400 - 460 nm激发下,650 cm⁻¹(非偏振,弯曲)和2039 cm⁻¹(非偏振,反对称拉伸)处结合叠氮化物振动的增强表明锰(III)肌红蛋白 - 叠氮化物复合物中存在新的电荷转移跃迁。这两种振动模式的归属基于它们的¹⁵N₃同位素位移(22和70 cm⁻¹)与计算值(22和69 cm⁻¹)的一致性、非偏振性质以及它们与离子化叠氮化物中相应振动的紧密接近程度。尽管报道了413 cm⁻¹(偏振)处的Fe(III)-N₃拉伸[阿舍,S. A.,维克里,L. E.,舒斯特,T. M.,& 索尔,K.(1977年)《生物化学》16,5849],但本研究中未观察到Mn -(III)-N₃拉伸。150至300 cm⁻¹之间的MnIIIMb - 叠氮化物的拉曼光谱与在640 nm电荷转移带或接近Soret带激发的FeIIIMb - 叠氮化物的拉曼光谱有显著差异。MnIIIMb - 叠氮化物光谱中在170和282 cm⁻¹(均为偏振)处有谱线,它们表现出极大的共振增强,并且¹⁵N₃同位素取代时不发生位移。这两条谱线在其他血红素蛋白质光谱中没有类似物,可能暂时归属于卟啉环的面外振动,后者涉及显著的Mn(III)-N(吡咯)拉伸。非完全对称叠氮化物模式的增强表明电荷转移态可能通过赫兹伯格 - 泰勒电子振动耦合与其他激发电子态(可能是能带Va或能带VI)混合。Mn(III)-N₃拉伸缺乏增强导致我们目前将叠氮化物(π)到卟啉(π)的电荷转移跃迁而非叠氮化物(π)到金属(dz²)或叠氮化物(n)到金属(dz²)进行归属。

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