Notes for Chapter

Eyring, J. Walter, and G. E. Kimball, Quantum Chemistry (New York, Wiley, 1944), p. iii. 

The fundamental equivalence between Schrodinger s wave-mechanical and Heisenberg s matrix-mechanical representation of quantum theory implies that H (or Hm ) may be viewed as a differential operator or a matrix. The latter viewpoint is usually more convenient in the 

Schrodinger, Ann. Phys. 80 (1926), 437. The quantal formalism substantially follows the classical method developed by Lord Rayleigh (Theory of Sound [1894]) and is commonly referred to as Rayleigh-Schrodinger perturbation theory.  

Throughout this work, familiarity will be assumed with basic mathematical notation and terminology of quantum chemistry and matrix algebra at the level of a standard text, such as I. N. Levine, Quantum Chemistry, 5th edn. (Englewood Cliffs, NJ, Prentice Hall, 2000) or J. R. Barrante, Applied Mathematics for Physical Chemistry, 2nd edn. (Upper Saddle River, NJ, Prentice Hall, 1998). 

Hirschfelder, W. Byers Brown, and S. T. Epstein, Adv. Quantum Chem. 1 (1964), 255. Formally, Eqs. (1.5a) and (1.5b) originate from expansions of E and in powers of a perturbation parameter that is set to unity in the final formulas used here. 

---

Bibliography and Notes for Chapter 2 Synthetic methods for dendritic molecules ... 

Bibliography and Notes for Chapter 3 "Synthetic methods for dendritic molecules" I 77... 

Bibliography and Notes for Chapter 5 Photophysicai properties of dendritic molecules" 193... 

Bibliography and Notes for Chapter 6 (Special) chemical reactions of dendritic molecules I 247... 

Bibliography and Notes for Chapter 8 Special properties and potential applications" I 325... 

---