Physical chemistry excited electronic state

The SAC-CI method was proposed in 1978 as an accurate electronic-structure theory for the ground, excited, ionized and electron-attached states of atoms and molecules. The method has been successfully applied to various photochemistry involving more than 150 molecules and established to be a useful method for studying chemistry and physics involving various electronic states. In this article, we gave a brief overview of our SAC-CI applications to the molecular spectroscopy. 

By convention in physical chemistry, vibrational levels and rotational levels of the ground electronic state are denoted with double primes, as in i/ and /", respectively. Vibratioiral levels and rotational levels of the excited electronic state are denoted with single primes, as in i/ and /. Often, however, organic photochemists omit the double prime notation for the ground electronic state. Also, the vibrational quantum levels may be denoted as v or V instead of v. 

The Born-Oppenheimer adiabatic approximation represents one of the cornerstones of molecular physics and chemistry. The concept of adiabatic potential-energy surfaces, defined by the Born-Oppenheimer approximation, is fundamental to our thinking about molecular spectroscopy and chemical reaction djmamics. Many chemical processes can be rationalized in terms of the dynamics of the atomic nuclei on a single Born Oppenheimer potential-energy smface. Nonadiabatic processes, that is, chemical processes which involve nuclear djmamics on at least two coupled potential-energy surfaces and thus cannot be rationalized within the Born-Oppenheimer approximation, are nevertheless ubiquitous in chemistry, most notably in photochemistry and photobiology. Typical phenomena associated with a violation of the Born-Oppenheimer approximation are the radiationless relaxation of excited electronic states, photoinduced uni-molecular decay and isomerization processes of polyatomic molecules. 

On a somewhat larger scale, there has been considerable activity in the area of nanocrystals, quantum dots, and systems in the tens of nanometers scale. Interesting questions have arisen regarding electronic properties such as the semiconductor energy band gap dependence on nanocrystal size and the nature of the electronic states in these small systems. Application [31] of the approaches described here, with the appropriate boundary conditions [32] to assure that electron confinement effects are properly addressed, have been successful. Questions regarding excitations, such as exdtons and vibrational properties, are among the many that will require considerable scrutiny. It is likely that there will be important input from quantum chemistry as well as condensed matter physics. 

Miscellaneous Physical Chemistry. A review of the year s literature (mid-1975— mid-1976) on excited states of biomplecules including carotenoids and related polyenes has been published. " Various aspects of the physical chemistry of carotenoids have been reported, including electron donor-acceptor properties, ... 

Wilkinson, F., Helman, W.P. and Ross, A.B. (1995) Rate constants for the decay and reactions of the lowest electronically excited singlet state of molecular oxygen in solution. An expanded and revised compilation. Journal of Physical Chemistry Reference Data, 24 (2), 663-1021. 

New assignment of the electronically excited states of anthracene-9,10-endoperoxide and its derivatives. Journal of Physical Chemistry A, 104, 164—165. 

The solvated electron is a transient chemical species which exists in many solvents. The domain of existence of the solvated electron starts with the solvation time of the precursor and ends with the time required to complete reactions with other molecules or ions present in the medium. Due to the importance of water in physics, chemistry and biochemistry, the solvated electron in water has attracted much interest in order to determine its structure and excited states. The solvated electrons in other solvents are less quantitatively known, and much remains to be done, particularly with the theory. Likewise, although ultrafast dynamics of the excess electron in liquid water and in a few alcohols have been extensively studied over the past two decades, many questions concerning the mechanisms of localization, thermalization, and solvation of the electron still remain. Indeed, most interpretations of those dynamics correspond to phenomenological and macroscopic approaches leading to many kinetic schemes but providing little insight into microscopic and structural aspects of the electron dynamics. Such information can only be obtained by comparisons between experiments and theoretical models. For that, developments of quantum and molecular dynamics simulations are necessary to get a more detailed picture of the electron solvation process and to unravel the structure of the solvated electron in many solvents. 

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