Quantum Chemical Benchmark Studies of the Electronic Properties of the Green Fluorescent Protein Chromophore. 1. Electronically Excited and Ionized States of the Anionic Chromophore in the Gas Phase

被引:101
作者
Epifanovsky, Evgeny [1 ]
Polyakov, Igor [2 ]
Grigorenko, Bella [2 ]
Nemukhin, Alexander [2 ,3 ]
Krylov, Anna I. [1 ]
机构
[1] Univ So Calif, Dept Chem, Los Angeles, CA 90089 USA
[2] Moscow MV Lomonosov State Univ, Dept Chem, Moscow 119991, Russia
[3] Russian Acad Sci, Inst Biochem Phys, Moscow 119334, Russia
关键词
PLESSET PERTURBATION-THEORY; DENSITY-FUNCTIONAL THEORY; COUPLED-CLUSTER METHODS; SELF-INTERACTION ERROR; CHARGE-TRANSFER; EXCITATION-ENERGIES; CONFIGURATION-INTERACTION; CONICAL INTERSECTIONS; CYANINE DYES; AB-INITIO;
D O I
10.1021/ct900143j
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
We present the results of quantum chemical calculations of the electronic properties of the anionic form of the green fluorescent protein chromophore in the gas phase. The vertical detachment energy of the chromophore is found to be 2.4-2.5 eV, which is below the strongly absorbing pi pi* state at 2.6 eV. The vertical excitation of the lowest triplet state is around 1.9 eV, which is below the photodetachment continuum. Thus, the lowest bright singlet state is a resonance state embedded in the photodetachment continuum, whereas the lowest triplet state is a regular bound state. Based on our estimation of the vertical detachment energy, we attribute a minor feature in the action spectrum as due to the photodetachment transition. The benchmark results for the bright pi pi* state demonstrated that the scaled opposite-spin method yields vertical excitation within 0.1 eV (20 nm) from the experimental maximum at 2.59 eV (479 nm). We also report estimations of the vertical excitation energy obtained with the equation-of-motion coupled cluster with the singles and doubles method, a multireference perturbation theory corrected approach MRMP2 as well as the time-dependent density functional theory with range-separated functionals. Expanding the basis set with diffuse functions lowers the pi pi* vertical excitation energy by 0.1 eV at the same time revealing a continuum of "ionized" states, which embeds the bright pi pi* transition.
引用
收藏
页码:1895 / 1906
页数:12
相关论文
共 99 条
[1]   Toward reliable density functional methods without adjustable parameters: The PBE0 model [J].
Adamo, C ;
Barone, V .
JOURNAL OF CHEMICAL PHYSICS, 1999, 110 (13) :6158-6170
[2]   Chromophores of the green fluorescent protein studied in the gas phase [J].
Andersen, LH ;
Lapierre, A ;
Nielsen, SB ;
Nielsen, IB ;
Pedersen, SU ;
Pedersen, UV ;
Tomita, S .
EUROPEAN PHYSICAL JOURNAL D, 2002, 20 (03) :597-600
[3]   Experimental studies of the photophysics of gas-phase fluorescent protein chromophores [J].
Andersen, LH ;
Bluhme, H ;
Boyé, S ;
Jorgensen, TJD ;
Krogh, H ;
Nielsen, IB ;
Nielsen, SB ;
Svendsen, A .
PHYSICAL CHEMISTRY CHEMICAL PHYSICS, 2004, 6 (10) :2617-2627
[4]   2ND-ORDER PERTURBATION-THEORY WITH A CASSCF REFERENCE FUNCTION [J].
ANDERSSON, K ;
MALMQVIST, PA ;
ROOS, BO ;
SADLEJ, AJ ;
WOLINSKI, K .
JOURNAL OF PHYSICAL CHEMISTRY, 1990, 94 (14) :5483-5488
[5]   Structure, initial excited-state relaxation, and energy storage of rhodopsin resolved at the multiconfigurational perturbation theory level [J].
Andruniów, T ;
Ferré, N ;
Olivucci, M .
PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 2004, 101 (52) :17908-17913
[6]   Aptamers switch on fluorescence of triphenylmethane dyes [J].
Babendure, JR ;
Adams, SR ;
Tsien, RY .
JOURNAL OF THE AMERICAN CHEMICAL SOCIETY, 2003, 125 (48) :14716-14717
[7]   Density functional theory with correct long-range asymptotic behavior [J].
Baer, R ;
Neuhauser, D .
PHYSICAL REVIEW LETTERS, 2005, 94 (04)
[8]  
BAER RL, UNPUB
[9]   DENSITY-FUNCTIONAL THERMOCHEMISTRY .3. THE ROLE OF EXACT EXCHANGE [J].
BECKE, AD .
JOURNAL OF CHEMICAL PHYSICS, 1993, 98 (07) :5648-5652
[10]   DENSITY-FUNCTIONAL EXCHANGE-ENERGY APPROXIMATION WITH CORRECT ASYMPTOTIC-BEHAVIOR [J].
BECKE, AD .
PHYSICAL REVIEW A, 1988, 38 (06) :3098-3100