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ChemWiki: The Dynamic Chemistry E-textbook > Theoretical Chemistry > Symmetry > Group Theory: Theory

Group Theory: Theory

- 1. Introduction
- 2. Symmetry Elements
- 2.1.1. Identity E
- 2.1.2. Proper Rotations and Cn axis
- 2.1.3. Reflection and mirror plane σ
- 2.1.4. Inversion and inversion center i
- 2.1.5. Improper Rotations and Sn axis

- 3. Symmetry Point Groups
- 3.1.1. Closure
- 3.1.2. Associativity
- 3.1.3. Identity
- 3.1.4. Inverses

- 4. Group Multiplication Tables
- 5. Subgroups
- 6. Classes
- 7. Symmetry Point Groups
- 8. Determination of symmetry Point Groups
- 9. Character Tables
- 10. Representations of a Group
- 11. Five rules of Characters
- 12. Outside links
- 13. References
- 14. Contributors

Symmetry can help resolve many chemistry problems and usually the first step is to determine the symmetry. If we know how to determine the symmetry of small molecules, we can determine symmetry of other targets which we are interested in. Therefore, this module will introduce basic concepts of group theory and after reading this module, you will know how to determine the symmetries of small molecules.

Symmetry is very important in chemistry researches and group theory is the tool that is used to determine symmetry. Usually, it is not only the symmetry of molecule but also the symmetries of some local atoms, molecular orbitals, rotations and vibrations of bonds, etc. that are important. For example, if the symmetries of molecular orbital wave functions are known, we can find out information about the binding. Also, by the selection rules that are associated with symmetries, we can explain whether the transition is forbidden or not and also we can predict and interpret the bands we can observe in Infrared or Raman spectrum.

Symmetry operations and symmetry elements are two basic and important concepts in group theory. When we perform an operation to a molecule, if we cannot tell any difference before and after we do the operation, we call this operation a *symmetry operation.* This means that the molecule seems unchanged before and after a symmetry operation. As Cotton defines it in his book, when we do a symmetry operation to a molecule, every points of the molecule will be in an equivalent position.

For different molecules, there are different kinds of symmetry operations we can perform. To finish a symmetry operation, we may rotate a molecule on a line as an axis, reflect it on a mirror plane, or invert it through a point located in the center. These lines, planes, or points are called symmetry elements. There may be more then one symmetry operations associated with a particular symmetry

The molecule does not move and all atoms of the molecule stay at the same place when we apply an identity operation, E, on it. All molecules have the identity operation. Identity operation can also be a combination of different operations when the molecule returns to its original position after these operations are performed.^{1} This will be demonstrated later.

C_{n} generates n operations, whose symbols are C_{n}, C_{n}^{2}, C_{n}^{3}, C_{n}^{4},…, E (=C_{n}^{n}). However, we usually write them in another way. Table 1.2 shows the way we write the 6 operations generated by proper rotation C_{6}. From this table, we can see that the symbols of the 6 rotations generated by C_{6} are C_{6}, C_{3}, C_{2}, C_{3}^{2}, C_{6}^{5}, E.One molecule can have many proper axes and the one with the largest n is called ** principle axis**.

Table 1.2 C_{6} axis and operations it generates

Take NH_{3} for an example. There are 3 mirror planes in molecule NH_{3}. When we do a reflection through a mirror plane, molecule NH_{3 }dose not change (Figure 1.2).

Figure 1.2 A mirror plane of NH_{3}.

There are three different kinds of mirror plane, \(\sigma_v\), \(\sigma_h\), and \(\sigma_d\). The mirror plane that contains the principle axis is called \(\sigma_v\).The mirror plane that perpendicular to the principle axis is called σh.2 Figure 1.3 shows \(\sigma_v\), \(\sigma_h\), and \(\sigma_d\) in \(PtCl_4^{2-}\).

Figure 1.3 \(\sigma_v\), \(\sigma_h\), and \(\sigma_d\) of PtCl_{4}^{2-}.This picture is drawn by ACD Labs 11.0.

When mirror plane is operated n times, we have^{1}

In a molecule, if we can find a point, on the straight line through which we can find a pair of same atoms on both side of this point, we call this molecule has an inversion center. The inversion center, *i*, is not necessarily on an atom of the molecule.^{1}Figure 1.4 shows the inversion center of \(C_2H_4Cl_2\).When inversion is operated n times, we have^{1}

^{}

Figure 1.4 Inversion center of C_{2}H_{4}Cl_{2}.

Improper rotation is a combination of two operations, proper rotation C_{n} and reflection ?. Figure 1.5 shows the improper rotation operation in CH_{4}.

Table 1.3 and table 1.4 show the operations generated by S_{6} and S_{5} axes separately. The 6 operations generated by S_{6} axis are S_{6}, C_{3}, i, C_{3}^{2}, S_{6}^{5} and E. And the 10 operations generated by S_{5}axis are S_{5}, C_{5}^{2}, S_{5}^{3}, C_{5}^{4}, ?, C_{5}, S_{5}^{7}, C_{5}^{3}, S_{5}^{9} and E.^{1}Since S_{1}= \(\sigma_h\) and S_{2}=σ_{h}C_{2}=i, the order of improper rotation, n, must always be larger than 2. And generally, when n is even, there are n operations {S_{n}^{1}, S_{n}^{2}, ..., S_{n}^{n}}, while when n is odd, there are 2n operations {S_{n}^{1}, S_{n}^{2}, ..., S_{n}^{2n}}. And we have^{1}

Table 1.3 S_{6} axis and operations it generates

Table 1.4 S_{5} axis and operations it generates

Figure 1.5 Improper rotation operation S_{4} in CH_{4}

_{}

For a molecule, all the symmetry operations that can be applied to the molecule have all the properties of a group. Therefore, before we introduce the symmetry point groups, the concept and properties of a group will be introduced first. When some elements have a certain kind of relationships and can be related to each other by these relationships, these elements can form a *group*.

If two elements A and B are in the group G, then the multiplicity of these two elements, C, is also in this group. It can be expressed as

All the elements in the group must satisfy the law of associativity, which can be expressed as

(AB)C=A(BC)

The group must contain such an element E that

ER=RE=R

In group theory, it refers to the operation identity E. Because any molecule or substance must at least have the symmetry element E.

If A is an element in group G, there must be another element A^{-1} in group G that satisfies AA^{-1}= A^{-1}A=E. Usually we can write A^{-1} as B. It can be expressed as

If A?G and AA^{-1}= A^{-1}A=E then A^{-1}=B=G

If there are n elements in a group G, and all of the possible n^{2} multiplications of these elements are known, then this group G is unique and we can write all these n^{2} multiplications in a table called group multiplication table. All the symmetry operations of a molecule can be written in the form of group multiplication table. There is a very important rule about group multiplication tables called *rearrangement theorem*, which is that every element will only appear once in each row or column.^{1}In group theory, when the column element is A and row element is B, then the corresponding multiplication is AB, which means B operation is performed first, and then operation A follows.^{1 }

Table 2.1 Group multiplication table^{1}

G_{6} | E | A | B | C | D | F |

E | E | A | B | C | D | F |

A | A | E | D | F | B | C |

B | B | F | E | D | C | A |

C | C | D | F | E | A | B |

D | D | C | A | B | F | E |

F | F | B | C | A | E | D |

From table 2.1 above, we can find several small groups in the group multiplication table. For example,

G_{2} | E | A |

E | E | A |

A | A | E |

In the same way, there are also many several small groups with orders 1, 2, 3 respectively. These small order groups that can be found in a higher order group are called *subgroups*. The number of elements in a group is called the order of a group, using a symbol *h*. The number of elements consist a subgroup is called the order of a subgroup, using a symbol *g*. From the previous two examples, we have^{1},

h/g=k (*k * is a whole number)

Since the symmetry point group have all the properties of a group, there are also several subgroups that we can find in a perticular symmetry point group. And sometimes we just use symmetry opertaions in one subgroup to apply to a system instead of using all the symmetry operations in the group, which can significantly simplify the calculations.

Class is another important concept in group theory which provides a way to simplify the expression of all the symmetry operations in a group. This means that we do not have to write down all the symmetry operatoins in a group but combine some related operations instead. The followin part will introduce the concept of classes and how to divide a group into classes.

A and B are two elements in a group, X is any elements in this group. If

\[X^{-1}AX=B\]

Then we can say the relationship of A and B is similarity transformation. A and B are conjugate.^{1 }Conjugate elements have three properties^{1}:

- Every element is conjugate with itself. \[A=X^{-1}AX\]
- If A is conjugate with B, then B is conjugate with A. \[\text{If} A=X^{-1}BX, \text{then} B=Y^{-1}AY\]
- If A is conjugate with B and C, then B is conjugate with C. \[\text{If} A=X^{-1}BX \text{ and } A=Y^{-1}CY, \text{then} B=Z^{-1}CZ\]

Now we can define a class. A class of a group is defined as all the elements in the group that are conjugated to each other.* ^{1}* To determine the classes of a group, we need to apply similarity transformation to the elements in the group until all the elements are grouped into smaller sets. For example, there are four elements in a group: {E, C

X= E, C_{2}, \(\sigma_v\), \(\sigma_v\)^{’ }X^{-1}= E, C_{2}, σ_{v}, σ_{v}^{’}

Because we always have XEX^{-1}=E, {E} is always a class for any point group. Then, apply similarity transformation to other elements in the group until all the elements are classified in smaller sets. Table 2.3 shows how the elements are classified in to classes.

**Table 2.4** Classes six order group

Therefore, there are three classes in group C_{3v}: {E}, {C_{3}, C_{3}^{2}} and { σ_{v}, σ_{v} ^{‘}, σ_{v} '‘ }.

__Significance of classes of a group__

In the same class of a group, the operations can be converted to each other by an operation. The operations in the same class are called *equivalent operations*. And a class of a symmetry group is a group of equivalent operations. This gives a simpler way to express the operations in a group.^{1}For example, for operations in the six order group above, table 2.5 shows the new way to express these operations.

**Table 2.5** Ways to express operations in six order group

As what mantioned above, all the symmetry operations of a molecule as a group can be written in the form of group multification table and they obey all the properties of a group. This group is called *symmetry point group*. It is called point group for two reasions. First reason is that this group have all the properties of a group in mathmeths. Second reason is that all the symmetry operations are related to a fixed point in the molecue, which is not necessearily to be an atom of the molecule. According to the symmetry of molecules, they can be classified as symmetry point groups.^{1}To determine the symmetry point group of a molecule is very important, because all symmetry related properties are dependent on the symmetry point group of the molecule. Symmetry point groups can be divided into 5 classes which are summaried below and the they are described in details here (symmetry point groups).^{1,6 }

Point groups | Symmetry Elements | Order | Example | |

Nonaxial | C_{1 } | E | 1 | HCFBrCl |

C_{i} | E, i | 2 | C_{2}H_{2}F_{2}Cl_{2} | |

C_{s} | E, ? | 2 | CH_{2}BrCl | |

Cyclic | C_{n} | E, C_{n} | n | C_{2}H_{4}Cl_{2} |

C_{nh} | E, C_{n}, n\(\sigma_v\) | 2n | NH_{3} | |

C_{nv} | E, C_{n}, σ_{h}, S_{n} | 2n | C_{2}H_{2}F_{2} | |

S_{n} | E, S_{n} | n | 1,3,5,7 -tetrafluoracyclooctatetrane | |

Dihedral | D_{n} | E, C_{n}, nC_{2} (?C_{n}) | 2n | [Co(en)_{3}]^{3+}. |

D_{nh} | E, C_{n}, σ_{h}, nC_{2} (?C_{n}) | 4n | | |

D_{nd} | E, C_{n}, σ_{d}, nC_{2} (?C_{n}) | 4n | C_{2}H_{6} | |

Polyhedral | T_{d} | E, 3C_{2}, 4C_{3}, 3S_{4, }6σ_{d} | 24 | CCl_{4} |

O_{h} | E, 3S_{4}, 3C_{4}, 6C_{2}, 4S_{6}, 4C_{3}, 3σ_{h}, 6σ_{d}, i | 48 | SF_{6} | |

I_{h} | E, 6S_{10}, 10S_{6}, 6C_{5}, 10C_{3}, 15C_{2}, 15? | 120 | C_{60} | |

Linear | C_{\(\sigma_v\)} | E, C_{?}, σ_{v} | ? | HCl |

D_{\(\sigma_h\)} | E, C_{?} σ_{v} , σ_{h}, i, ?C_{2} | ? | O_{2} |

Determination of symmetry point group of a molecule is the very first step when we are solving chemistry problems. The symmetry point group of a molecule can be determined by the following flow chart^{7}.

**Table 2.12** Flow chart to determine point group

Now, using this flow chart, we can determine the symmetry of molecules. However, to further determine the symmetry properties of something such as molecular orbitals, vibrational modes, etc. we need character tables which will be introduced next.

Through similarity of transformation, we can define the reducible and irreducible representations of a group. If a matrix representation A can be transferred to block-factored matrix A’, a matrix composed of blocks (A’, A’’, A’’’) at the diagonal and zero in any other position, by similarity transformation, this matrix A is called the reducible representation of this group. And if these blocks (A’, A’’, A’’’) cannot be further transferred to block-factored matrix through similarity transformation, A’, A’’, A’’’ are called irreducible representations of the group. And the sum of the trace of A’, A’’, A’’’ (the number on the diagonal of A’, A’’, A’’’) is called the characters of this representation. As is shown in the following equation, a_{11}’+ a_{22}’+…+ a_{nn}’ is one of the characters. Reducible representations can be reduced to irreducible representations and irreducible representations cannot be reduced further.^{1}

Take C_{3v} as an example.Take (x, y, z) as the basic, the matrix of all the operations in C_{3v} group {E, C_{3}, C_{3}^{2}, σ_{v}, σ_{v} ^{‘}, σ_{v} ^{'‘}} are shown in Table 2.6.

**Table 2.6** Reducible and irreducible representations of C_{3v}

As shown in the table 2.6, all the matrix are block-factored matrix and they are reducible representations. Every block in these reducible representations are irreducible representations and the sums of the trace are the characters which are also listed in the table. Notice that the operations in the same class have the same character. Therefore, they are always written together using the new notations {E, 2C_{3}, 3σ_{v}}:

**Table 2.7** Two irreducible representations of C_{3v}

This is not a completed table of irreducible representations, because the basis chosen are not completed. There are different kinds of basis, including one-dimensional basis like x, y, z, R_{x}, R_{y}, R_{z} and two-dimensional basis like x^{2}, y^{2}, z^{2}, xy, yz, xz. If we chose R_{z} which is the rotation around z-axis as another basis, we can get another irreducible representation, (1, 1, -1). “1” means nothing change when operation is applied to the basis. “-1” means it becomes opposite when operation is applied to the basis. “0” means the basis are moved when operation is applied. Therefore, in summary, for now the irreducible representations of C_{3v} group is

** ****Table 2.8** Summary of irreducible representations of C_{3v}

For irreducible representations and their characters, there are five very important rules^{1}:

The order of the irreducible representation matrix is called the dimension of the irreducible representation, using symbol l_{1}, l_{2}, ... And rule 1 states that the sum of the squares of all the dimensions of irreducible representations (l_{1}^{2}+ l_{2}^{2}+ …) is equal to the order of the group, h.

?l_{i}^{2}=l_{1}^{2}+ l_{2}^{2}+ …=h

Since the character of the irreducible representation of operation E, ?_{i}(E), is equal to the dimension of the corresponding irreducible representation, Rule 1 can also be written as

? Γ_{i}(E)^{2}= Γ_{1}(E)^{2}+ Γ_{2}(E)^{2}+ …=h

Rule 2 is that the sum of the square of the characters in any irreducible representation is equal to h. For example, for the first irreducible representation in C_{3v} group

Γ_{1}(E)^{2}+ Γ_{1}(C_{3})^{2}+ Γ_{1}(C_{3}^{2})^{2}+ Γ_{1}(σ_{v})^{2}+ Γ_{1}(σ_{v} ^{‘})^{2}+ Γ_{1}(σ_{v} ^{'‘})^{2}=1^{2}+1^{2}+1^{2}+1^{2}+1^{2}+1^{2}=6

Since for the same class, the characters are the same, it can also be written as

Γ_{1}(E)^{2}+ 2*Γ_{1}(C_{3})^{2}+ 3* Γ_{1}(σ_{v})^{2}=1^{2}+2*1^{2}+3*1^{2}=6

Also, for another irreducible representation in C_{3v} group

Γ_{1}(E)^{2}+ 2*Γ_{1}(C_{3})^{2}+ 3* Γ_{1}(σ_{v})^{2}=2^{2}+2*(-1)^{2}+3*0^{2}=6

Rule 3 is that the vectors which composed of the characters from different irreducible representations are orthogonal.

? ?_{i}(R)^{2}Γ_{j}(R)^{2} =0 (i is not equal to j)

Again, take C_{3v} group for an example

? Γ_{1}(R)^{2}Γ_{2}(R)^{2} =1*2+2*1*(-1)+3*1*0=0

Rule 4 is that the characters of matrix representations, either reducible or irreducible, of the operations in the same class are the same, which is shown as the former table.

Rule 5 is that the number of irreducible representations **is equal** to the number of classes.

For C_{3v} group, there are three classes and therefore there are also three irreducible representations. Therefore, the three irreducible representations in Table 2.8 are the complete list of irreducible representations in C_{3v} group.

There is a very important relationship between reducible representations and irreducible representations, which is that any reducible representation can be written as the linear combination of irreducible representations. The similarity transformations do not change the character of a reducible representation, therefore

where ?(R) is the character of reducible representation of operation R. ?_{j}(R) is the character of jth irreducible representation. a_{j} is the times ?_{j}(R) will appear in blocks when reducible representation is reduced to irreducible representation by similarity transformation. To determine a_{j}, the former equation can be written as

According to rule 3, only when i=j, the sum over R is not equal to zero. Then according to rule 1, the equation can be written as

Then rearrange to

Using this equation, we can express reducible representations with irreducible representations, which is very important when we solve chemistry problems.

Again, take C_{3v} group for an example, the reducible representation shown in table 2.6 can be express as combination of irreducible representations using this relationship. Use irreducible representations in table 2.8

a_{1}= 1/6 [1(3)(1)+2(0)(1)+3(1)(1)] = 1

a_{1}= 1/6 [1(3)(2)+2(0)(-1)+3(1)(0)] = 1

a_{1}= 1/6 [1(3)(1)+2(0)(1)+3(1)(-1)] = 0

Therefore,

^{5}

Table 2.11 Meanings of different area of character tables

Using this flow chart, you can determine the symmetries of small molecules. And also, by using group theory and character tables, you can determine the symmetries of any thing you are interested in, such as molecular orbitals, vibrational modes, etc. In conclusion, group theory play a very important role in chemistry, which we can see from various applications of group theory in chemistry, like Infrared spectrum, Raman spectrum, electronic spectrum, etc.

- http://www.jce.divched.org/JCEDLib/WebWare/collection/reviewed/JCE2005p1742WW/jcesubscriber/symmetry/index.htm (This is a very interesting and helpful website which shows animated picture of molecular symmetry operations, etc.)
- http://www.jce.divched.org/JCEDLib/WebWare/collection/reviewed/JCE2005p1741_2WW/jcesubscriber/3DMolSym/Index.htm (Another online 3D animated view of molecule symmetry elements and operations)
- http://www.3dchem.com (Animated 3D mode structures of lots of molecules)
- http://en.wikipedia.org/wiki/List_of_character_tables_for_chemically_important_3D_point_groups[1] (List of character tables for chemically important 3D point groups)

- Cotton, F. A., Chemical Applications of Group Theory. Third ed.; John Wiley & Sons: Canada, 1990.
- Kelly, P., Symmetry. Handout of CHE201. Fall 2008
- Basic Group Theory, MIT Open Courses 18.904
- Cotton, F. A., Chemical Applications of Group Theory. Third ed.; John Wiley & Sons: Canada, 1990; Vol. 2, p 8.
- Kelly, P., Anatomy of a Character Table. Handout Fall 2008.
- Wiberg, E.; Wiberg, N.; Holleman, A. F., Inorganic Chemistry. Academic Press: 2001; pp. 163-164.
- Principle of Inorganic Chemistry II, Lecture 6: Molecular Point groups II, MIT Department of Chemistry

- Wei Wei

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01:15, 6 Feb 2015

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