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Hota - Mathematical Physical Chemistry: Practical and Intuitive Methodology

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Hota Mathematical Physical Chemistry: Practical and Intuitive Methodology
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    Mathematical Physical Chemistry: Practical and Intuitive Methodology
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Part I
Quantum Mechanics
Quantum mechanics is clearly distinguished from classical physics whose major pillars are Newtonian mechanics and electromagnetism established by Maxwell. Quantum mechanics was first established as a theory of atomic physics that handled microscopic world. Later on, quantum mechanics was applied to macroscopic world, i.e., cosmos. A question on how exactly quantum mechanics describes the natural world and on how far the theory can go remains yet problematic and is in dispute to this day.
Such an ultimate question is irrelevant to this monograph. Our major aim is to study a standard approach to applying Schrdinger equation to selected topics. The topics include a particle confined within a potential well, a harmonic oscillator, and a hydrogen-like atoms. Our major task rests on solving eigenvalue problems of these topics. To this end, we describe both an analytical method and algebraic (or operator) method. Focusing on these topics, we will be able to acquire various methods to tackle a wide range of quantum-mechanical problems. These problems are usually posed as an analytical equation (i.e., differential equation) or an algebraic equation. A Hamiltonian is constructed analytically or algebraically accordingly. Besides Hamiltonian, physical quantities are expressed as a differential operator or a matrix operator. In both analytical and algebraic approaches, Hermitian property (or Hermiticity) of an operator and matrix is of crucial importance. This feature will, therefore, be highlighted not only in this part but also throughout this book along with a unitary operator and matrix.
Optical transition and associated selection rules are dealt with in relation to the above topics. Those subjects are closely related to electromagnetic phenomena that are considered in Part II.
Springer Nature Singapore Pte Ltd. 2018
Shu Hotta Mathematical Physical Chemistry
1. Schrdinger Equation and Its Application
Shu Hotta 1
(1)
Faculty of Materials Science and Engineering, Kyoto Institute of Technology, Kyoto, Japan
Shu Hotta
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Quantum mechanics is an indispensable research tool of modern natural science that covers cosmology, atomic physics, molecular science , materials science, and so forth. The basic concept underlying quantum mechanics rests upon Schrdinger equation . The Schrdinger equation is described as a second-order linear differential equation ( SOLDE ). The equation is analytically solved accordingly. Alternatively, equations of the quantum mechanics are often described in terms of operators and matrices, and physical quantities are represented by those operators and matrices. Normally, they are non-commutative . In particular, the quantum-mechanical formalism requires the canonical commutation relation between position and momentum operators. One of the great characteristics of the quantum mechanics is that physical quantities must be Hermitian . This aspect is deeply related to the requirement that these quantities should be described by real numbers. We deal with the Hermiticity from both an analytical point of view ( or coordinate representation ) relevant to the differential equations and an algebraic viewpoint ( or matrix representation ) associated with the operators and matrices. Including these topics, we briefly survey the origin of Schrdinger equation and consider its implications. To get acquainted with the quantum-mechanical formalism, we deal with simple examples of the Schrdinger equation .
1.1 Early-Stage Quantum Theory
The Schrdinger equation is a direct consequence of discovery of quanta. It stemmed from the hypothesis of energy quanta propounded by Max Planck (1900). This hypothesis was further followed by photon ( light quantum ) hypothesis propounded by Albert Einstein (1905). He claimed that light is an aggregation of light quanta and that individual quanta carry an energy Picture 1 expressed as Planck constant Mathematical Physical Chemistry Practical and Intuitive Methodology - image 2 multiplied by frequency of light Mathematical Physical Chemistry Practical and Intuitive Methodology - image 3 , i.e.,
Mathematical Physical Chemistry Practical and Intuitive Methodology - image 4
(1.1)
where Picture 5 and Picture 6 . The quantity Picture 7 is called angular frequency with Picture 8 being frequency. The quantity Picture 9 is said to be a reduced Planck constant .
Also, Einstein (1917) concluded that momentum of light quantum p is identical to the energy of light quantum divided by light velocity in vacuum c . That is, we have
Mathematical Physical Chemistry Practical and Intuitive Methodology - image 10
(1.2)
where Picture 11 ( Picture 12 is wavelength of light in vacuum) and Picture 13 is called wavenumber . Using vector notation, we have
Picture 14
(1.3)
where Picture 15 ( Picture 16 : a unit vector in the direction of propagation of light) is said to be a wavenumber vector .
Meanwhile, Arthur Compton (1923) conducted various experiments where he investigated how an incident X-ray beam was scattered by matter (e.g., graphite, copper, etc.). As a result, Compton found out a systematical redshift in X-ray wavelengths as a function of scattering angles of the X-ray beam ( Compton effect ). Moreover, he found that the shift in wavelengths depended only on the scattering angle regardless of quality of material of a scatterer. The results can be summarized in a simple equation described as
14 where denotes a shift in wavelength of the scattered beam is a rest - photo 17
(1.4)
where Picture 18 denotes a shift in wavelength of the scattered beam; Picture 19 is a rest mass of an electron; Picture 20 is a scattering angle of the X-ray beam (see Fig. ). A quantity Mathematical Physical Chemistry Practical and Intuitive Methodology - image 21
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