111
Dr. Sumanta Kumar Padhi Assistant Professor  Department of Applied Chemistry Indian School of Mines Dhanbad, 826 004, INDIA ACC 32138 Winter Semester 2013 2314

Introduction to Group Theory.pdf

Embed Size (px)

Citation preview

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 1/111

Dr. Sumanta Kumar Padhi

Assistant Professor Department of Applied Chemistry

Indian School of Mines Dhanbad, 826 004, INDIA

ACC 32138

Winter Semester 2013 2314

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 2/111

• Symmetry

Relationship between parts of an object with respect to size,shape and position.

e.g In nature:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 3/111

• Symmetry Element:

A symmetry element is a geometric entity e.g. a point, a line or aplane.

Symmetry element is a point, line or plane about which asymmetry operation is performed

• Symmetry Operator:A symmetry operator performs and action on a three

dimensional object.

A symmetry operation moves an object into an indistinguishableorientation .

Symmetry operators are like other mathematical operators (x, ÷,+, log, cos, sin, etc..) 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 4/111

• There are five types of symmetry operators:

Operator Symbol

Identity E

Rotation CMirror Plane σ 

Inversion i

Improper rotation S

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 5/111

• There are five symmetry elements, which will be defined relative

to point with coordinate (x1,y1,z1):

• Identity, E

E(x1 ,y1 ,z1) = (x1 ,y1 ,z1)This operator does nothing and is required for a completeness. Itis equivalent to multiplying “1” or adding “0” in algebra.

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 6/111

• Proper rotation axis, Cn (where θ= 2π/n)

Convention is a clockwise rotation of the point.The symmetry element is called axis of symmetry and denotedby Cn.C2(z) (x1 ,y1 ,z1) = (-x1 ,-y1 ,z1) ; in this case θ = 180°Many molecules have more than one symmetry axis. The axis

with higher “n” values is called principal axis.

n = (2π/θ)θ→0; n = ∞; Cn = C∞ 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 7/111

 Ammonia has a C3 axis. Note that there are two

operations associated with the C3 axis. Rotation by 120o 

in a clockwise or a counterclockwise direction provide

two different orientations of the molecule. 

Water has a 2-fold axis of rotation. When rotated by

180o, the hydrogen atoms trade places, but the

molecule will look exactly the same.

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 8/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 9/111

three-fold axis three-fold axis two-fold axis two-fold axis

viewed from viewed from viewed from viewed from

above the side the side above

Note: there are 3 C2 axes

C3  C3  C2  C2

principal axis

(highest value of Cn)

.

Rotational axes of BF3 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 10/111

Rotational axes of BF3

 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 11/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 12/111

 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 13/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 14/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 15/111

• Plane of Reflection (σ)σ

xz (x1 ,y1 ,z1) = (x1 ,-y1 ,z1)

σxz

σyz

H1 

H2 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 16/111

• Plane of Symmetry is of three types

1. Vertical plane (σ

v)2. Horizontal plane (σh)

3. Dihedral plane (σd)

• Horizontal plane (σh)

If a plane is ⊥ to the principal axis then it is called σh 

• Vertical plane (σv)If the plane is along the principal axis then it is called vertical plane (σv)

• Dihedral plane (σd)

If the plane bisects the angle subtended between two similar consecutive

C2-axis

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 17/111

 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 18/111

 

Mirror planes can contain the principal axis (σ v) or be atright angles to it (σ h). BF3 has one σ h and three σ v planes:

(v = vertical, h = horizontal)

σ vmirror plane C

3

principal axis

σ hmirror plane

C3

principal axis

σ v mirror plane

contains the C3 axis

σ h mirror plane

is at right angles to theC3 axis

Mirror planes (σ) of BF3:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 19/111

 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 20/111

  C6

principal axis

C2

C2

C2C6C2

σ v σ v

σ h

C6

principal axis

C6

principal axis

Rotational axes and mirror planes of benzene

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 21/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 22/111

• Inversion (i)

All the points in the molecule are reflected through a single point.The point is the symmetry element for inversion. The position of the (x,y,z)

coordinate changes to thecorresponding –ve coordinate (-x,-y,-z).

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 23/111

 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 24/111

 

center of symmetry center of symmetry

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 25/111

• Improper rotation (Sn)

Rotation by 2π

/n followed by reflectionσ

,⊥

 to the rotation axis.Since performing σ  two times is the same as doing nothing (E), therefore S

can only be performed odd number of times.

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 26/111

• Improper rotation (Sn)• Sn (Improper Rotation Operation) = rotation about 360/n axis followed by reflection

through a plane perpendicular to axis of rotation

a. Methane has 3 S4 operations (90 degree rotation, then reflection)

b. 2 Sn operations = Cn/2  (S24 = C2)

c. nSn = E, S2 = i, S1 = s

d. Snowflake has S2, S3, S6 axes

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 27/111

 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 28/111

 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 29/111

 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 30/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 31/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 32/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 33/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 34/111

Types of matrices:

  Rectangular Matrix

  Column Matrix

  Row matrix

  Zero null matrix

  Square matrix

  Diagonal Matrix

  Scalar Matrix

  Unit or Identity Matrix

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 35/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 36/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 37/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 38/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 39/111

Equal Matrices:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 40/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 41/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 42/111

Direct product of two matrices:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 43/111

Trace or Character of a matrix

Trace or character of matrix is the sum of the diagonal elements.It is represented by “

 

” .

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 44/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 45/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 46/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 47/111

E or Identity Matrix:

E(x1 ,y1 ,z1) = (x1 ,y1 ,z1)

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 48/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 49/111

σ

 Matrix: σxz (x1 ,y1 ,z1) = (x1 ,-y1 ,z1)

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 50/111

Plane of symmetry (σ

) Matrix:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 51/111

σ

 Matrix:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 52/111

Inversion (i) Matrix:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 53/111

Inversion (i) Matrix:

Therefore, the inversion (i) matrix is:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 54/111

Cn Matrix:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 55/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 56/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 57/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 58/111

x2 = r [cosθ

 cos + sinθ

 sin ]

x2 = r [sin θ cos - cos θ sin ] 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 59/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 60/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 61/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 62/111

Sn Matrix:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 63/111

Sn Matrix:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 64/111

E C2  σxy  i

The following matrices form a representation of the C2h point group

The following matrices form a representation of the C3v point group→

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 65/111

• The symmetry properties of an object (e.g. atoms of a molecule,set of orbitals, vibrations). The collection of objects is commonly

referred to as a basis set .

Classify objects of the basis set into symmetry operations . Symmetry operations form a group.

Group mathematically defined and manipulated by group theory.

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 66/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 67/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 68/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 69/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 70/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 71/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 72/111

Defini tion of a group 

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 73/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 74/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 75/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 76/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 77/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 78/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 79/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 80/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 81/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 82/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 83/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 84/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 85/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 86/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 87/111

Group Multiplication table for C2h:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 88/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 89/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 90/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 91/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 92/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 93/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 94/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 95/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 96/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 97/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 98/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 99/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 100/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 101/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 102/111

• E  is always in a class by itself. It can be transformed into itself by

all the elements in the group.

• Inversion element , i, is in class by itself.

• All Cnm axes are in a class.

• Similar C2s  are in a class.

• Like Cnm all Sn

m axes are in a class. If there are two or many such

types they are placed in as many classes.

• Similar vertical (σv) and similar dihedral planes (σd) are in a class.

• Horizontal plane (σh) is a special plane and is always placed in a

different class from other planes.

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 103/111

• In all Abelian point groups each element is in a class by itself i.e.,

the number of symmetry elements or order of the group is equal

to the number of classes.

Number of Classes = Order of the group (h) 

• In non Abelian groups the number of classes is always less than

the order of the group.

• No element in the group occurs in more than one class.

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 104/111

• In symmetry, a point group is the collection of symmetry operations that leaves amolecule unchanged.

• Groups with very high symmetry:

1. Icosahedral, Ih

2. Octahedral, Oh

3. Tetrahedral, Td

• Groups with low symmetry:

1. C1 – molecules with only the E element

2. Cs – molecules with E and a single plane of symmetry (σ). 

3. Ci – molecules with only E and a center of inversion, i.• Groups with an n-fold axis of rotation:

1. Cn – identity (E) and n-fold rotation (Cn)

2. Cnv – identity (E), n-fold rotation (Cn) and n vertical reflections (σv).

3. Cnh – identity (E), n-fold rotation (Cn) and horizontal reflection plane (σh).• Dihedral groups:

1. Dn – identity (E), n-fold rotation (Cn) and n two-fold rotations (C2) perpendicular to Cn axis (principal axis). (with no mirror planes)

2. Dnh  - identity (E), n-fold rotation (Cn), n two-fold rotations (C2) perpendicular to Cn 

axis and horizontal reflection plane (σh). (with a horizontal mirror plane)

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 105/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 106/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 107/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 108/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 109/111

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 110/111

B2Br 4 has the following staggered structure:

Ga2H6 has the following structure in the gas phase:

7/17/2019 Introduction to Group Theory.pdf

http://slidepdf.com/reader/full/introduction-to-group-theorypdf 111/111

SF5Cl: C4v H2O2: C2

 C3H4: D2d

  C60: Ih  CH2ClF:

CsOr C1h

S8: D4d  [Co(Ox)3]

3- : D3