2017(平成29)年度 「反応物理化学セミナー」案内

過去のセミナー


 Reading Circle : (前期) 毎週月曜日 16:30〜18:30

  分子分光学のテキスト

   P. F. Bernath, Spectra of Atoms and Molecules, 2nd ed., Oxford University Press, Oxford, 2005.

  を輪読します。

月日
(2017年度)
担当者

タイトル
担当範囲 欠席
1 4/10 井上(1) Chap. 1 Introduction
1.1 Waves, Particles, and Units
(p. 3) Spectroscopy is the study of the interaction 〜
(p. 3) electricity and magnetism.
中田(1)
2 4/17 鬼塚(1) 1.2 The Electromagnetic Spectrum (p. 3) Wavelength and frequency are related by 〜
(p. 6) and wavelength (Å).
門脇(1), 吉木(1)
3 5/8 長森(1) 1.3 Interaction of Radiation with Matter
・Blackbody Radiation
(p. 6) It is worth noting that the different region 〜
(p. 7) Eq (1.13)

4 5/15 門脇(1) ・Blackbody Radiation (p. 7) Eq (1.13) 鬼塚(1), 谷本(1),中田(2),吉木(2)
5 5/22 深水(1) ・Einstein A and B Coefficients
・Absorption and Emission of Radiation
(p. 8) Consider a collection of N two levels 〜
(p. 13) Eq (1.33b)
6 5/29 吉木(1) ・Absorption and Emission of Radiation (p. 13) The integral M01 = M10 = <ψ1|μ|ψ0> is 〜
(p. 14) by substitution into equations (1.36).

7 6/5 山﨑(裕)(1) ・Absorption and Emission of Radiation (p. 14) The time-dependent probability that 〜
(p. 15) in the field of quantum optics.

8 6/12 天道(1) ・Absorption and Emission of Radiation (p. 16) The effect of collisions and other relaxation 〜
(p. 17) is given by equation (1.1).
門脇(2)
9 6/19 川端(1) ・Absorption and Emission of Radiation (p. 17) Since a typical electronic transition may 〜
(p. 19) MHz in frequency space.
鬼塚(2)
10 6/26 谷本(1) ・Absorption and Emission of Radiation (p. 18) Before equation (1.47) can be used, 〜
(p. 19) possibility of relaxation.
門脇(3), 中田(3)
11 7/3 中田(1) ・Absorption and Emission of Radiation
・Beer's Law
・Lineshape Functions
(p. 19) Collisions or the spontaneous radiation 〜
(p. 22) in an inhomogeneous lineshape.

12 7/10 井上(2) ・Natural Lifetime Broadening (p. 22) Consider a two level system with an 〜
(p. 23) in the laboratory frame (Figure 1.16).

13 7/24 長森(2) ・Natural Lifetime Broadening (p. 23) Now if the population in the excited state 〜
(p. 27) lifetime of the excited states.
鬼塚(3), 谷本(2), 吉木(3)
14 7/31 門脇(2) ・Pressure Broadening (p. 27) The derivation of the pressure-broadening 〜
(p. 28) measurements are to be made.

15, 16 10/02, 10/16 鬼塚(2) ・Doppler Broadening (p. 28) Doppler broadning results in an 〜
(p. 30) in terms of the Doppler FWHM.
門脇(4,5)
17 10/23
深水(2) ・Doppler Broadening (p. 30) The Gaussian function is the bell-shaped 〜
(p. 34) use these relationship constantly.
鬼塚(4),門脇(6)
18, 19 10/30, 11/6 吉木(2) Chap. 2 Molecular Symmetry (p. 41) The language of group theory has become 〜
(p. 41) operations is more useful.
門脇(7,8),山﨑(裕)(1,2)
20a 11/13 西村(1) 2.1 Symmetry Operations
・Operator Algebra
(p. 41) The idea of molecular symmetry can be 〜
(p. 46) Eq (2.15)
門脇(9),山﨑(裕)(3)
20b, 21 11/13, 11/20 天道(2) ・Symmetry Operator Algebra
2.2 Groups
・Point Groups
・Classes
・Subgroups
2.3 Notations of Point Groups
(p. 46) Symmetry operations can be applied 〜
(p. 55) Kh. Ar.
門脇(10)
22 11/27 山﨑(裕)(2) Chap. 3 Matrix Representation of Groups
3.1 Vectors and Matrices
(p. 58) A point in space can be described by 〜
(p. 59) Eq (3.9)
門脇(11),谷本(3),吉木(4)
23 12/4 川端(2) 3.1 Vectors and Matrices (p. 60) A row vector xt = (x1x2...xn) is the 〜
(p. 62) Eq (3.20)
門脇(12)
24 12/11 中田(2) 3.1 Vectors and Matrices (p. 62) If we allow the elements of the column 〜
(p. 63) Eq (3.27).
門脇(13),谷本(4)
25 12/18 井上(3) 3.1 Vectors and Matrices
・Matrix Eigenvalue Problem
(p. 63) Matrices are useful in transforming 〜
(p. 65) x1 and x2 gives x1, x2, and X.
門脇(14),谷本(5),吉木(5)
26 12/25 鬼塚(3) ・Matrix Eigenvalue Problem
・Similarity Transformations
(p. 65) If A is Hermitian, A = A, then the 〜
(p. 65) by a unitary (or orthogonal) transformation.
門脇(15),谷本(6)
27 1/15 長森(3) 3.2 Symmetry Operations and Position Vectors (p. 65) Perhaps the simplest way to generate 〜



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