Birge R R, Murray L P, Pierce B M, Akita H, Balogh-Nair V, Findsen L A, Nakanishi K
Proc Natl Acad Sci U S A. 1985 Jun;82(12):4117-21. doi: 10.1073/pnas.82.12.4117.
We studied the nature of the protein binding site of rhodopsin, using two-photon spectroscopy to assign the location of the low-lying "covalent" 1Ag*- -like pi pi * state in a model rhodopsin containing a locked-11-cis chromophore. The two-photon thermal lens maximum is observed at 22,800 cm-1, approximately equal to 2000 cm-1 above the one-photon absorption maximum, indicating that the protein environment has induced a level ordering reversal of the low-lying pi pi * states relative to that observed in retinyl Schiff bases in solution. The spectroscopic results clearly indicate that the chromophore is protonated and that the binding site is uncharged. Electrostatic energy contour maps of the binding site are calculated, showing possible locations for the external counterion(s). Two models of the binding site are proposed that accommodate the available spectroscopic data. One model involves a protonated Schiff base chromophore stabilized by a single negatively charged aspartic or glutamic acid residue. A more complicated model involving two residues (one charged, the other neutral) is also proposed. The latter model is interesting because it also accommodates the observed deuterium isotope effect in the form of a proton translocation between the two residues. The translocation is assumed to be a ground state process, initiated subsequent to the photoisomerization of the chromophore and energetically driven via destabilization of the counterion environment as a result of isomerization-induced charge separation.
我们利用双光子光谱法来确定视紫红质蛋白结合位点的性质,该方法用于在含有锁定11 - 顺式发色团的视紫红质模型中,确定低能“共价”1Ag * - 类ππ * 态的位置。双光子热透镜最大值出现在22,800 cm-1处,比单光子吸收最大值高约2000 cm-1,这表明蛋白质环境相对于溶液中视黄醛席夫碱中观察到的情况,诱导了低能ππ * 态的能级顺序反转。光谱结果清楚地表明发色团被质子化,且结合位点不带电荷。计算了结合位点的静电能等高线图,显示了外部抗衡离子的可能位置。提出了两种结合位点模型,以适应现有的光谱数据。一种模型涉及由单个带负电荷的天冬氨酸或谷氨酸残基稳定的质子化席夫碱发色团。还提出了一个更复杂的模型,涉及两个残基(一个带电荷,另一个不带电荷)。后一种模型很有趣,因为它还以两个残基之间的质子转移形式,解释了观察到的氘同位素效应。这种转移被认为是一种基态过程,在发色团光异构化之后启动,并由于异构化诱导的电荷分离导致抗衡离子环境不稳定而在能量上驱动。