5.5A: \(BH_3\)
 Page ID
 2550
Symmetry Labels
D_{3H}  E  2C_{3}  3C_{2}  σh  2S_{3}  σv 


A1'  1  1  1  1  1  1 
 x^{2}+y^{2}, z^{2} 
A2'  1  1  1  1  1  1  R_{z} 

E'  2  1  0  2  1  0  (x,y)  (x^{2}y^{2},xy) 
A1''  1  1  1  1  1  1 


A2''  1  1  1  1  1  1  z 

E''  2  1  0  2  1  0  (R_{x},R_{y})  (xz,yz) 
FIGURE2: Character table for the the point group D3h
B atom in BH3:
+sorbital: with the shape of the sphere, its function is x^{2}+y^{2}+z^{2}. Therefore, 2s orbital hasa_{1}' symmetry
+porbital: has 3 orbitals , p_{x}, p_{y}, p_{z}. Therefore, 2p_{z} orbital has a_{2}" symmetry
2p_{x} and 2p_{y} orbital are degenerate and have e' symmetry
3 Hydrogen atoms in BH3: (Ligand group orbitals)
a. Symmetry labels of LGOs:
With the symmetry operations of BH3 above, we can determine how many LGO unmoved by creating the following table:
D_{3h}  E  2C_{3}  3C_{2}  σ_{h}  2S_{3}  3σ_{v} 
LGO  3  0  1  3  0  1 
Next, with these values we can apply the following formula to identify the symmetry labels of the Ligan group orbitals
a= 1/h ∑[(N).Xr(R).Xi(R)]
h: the total number of coeficients of symmetry operation
N: the coeficient of the each symmetry operation
Xr(R): the character of the reducible representation corresponding to the R (values that just found in the LGO row
Xi(R): the character of the irreducible representation corresponding to the R (from the character table)
Calculation:
A1'= 1/12 [(1)(3)(1)+(2)(0)(1)+(3)(1)(1)+(1)(3)(1)+(2)(0)(1)+(3)(1)(1)] = 1 A1'
A2'= 1/12 [(1)(3)(1)+(2)(0)(1)+(3)(1)(1)+(1)(3)(1)+(2)(0)(1)+(3)(1)(1)]= 0 A2'
E'= 1/12 [(1)(3)(2)+(2)(0)(1)+(3)(1)(0)+(1)(3)(2)+(2)(0)(1)+(3)(1)(0)]= 1E'
A1''= 1/12 [(1)(3)(1)+(2)(0)(1)+(3)(1)(1)+(1)(3)(1)+(2)(0)(1)+(3)(1)(1)]= 0 A1''
A2''= 1/12 [(1)(3)(1)+(2)(0)(1)+(3)(1)(1)+(1)(3)(1)+(2)(0)(1)+(3)(1)(1)] = 0 A2''
E''= 1/12 [(1)(3)(2)+(2)(0)(1)+(3)(1)(0)+(1)(3)(2)+(2)(0)(1)+(3)(1)(0)] = 0 E ''
Thus, LGO's symmetry labels are a1' + e'
b. How to determine the shapes of the LGOS?
LGO's symmetry labels are a1' + e'. There are 3 LGOs that can be made out of these symmetry labels,one LGO is from a1' and two LGOs are from e' due to doubly degenerate. In order to determine the shape of each LGO, we would use the wavefunctions.
Three hydrogens in BH3 are assigned with Ψ1, Ψ2, Ψ3. Now lets look at how each Ψ is affected by the symmetry operations of the D3h and their results are completed in the following table:
D_{3h}  E  C_{3}  C^{2}_{3}  C_{2}  C_{2}’  C_{2}’’  σ_{h}  S_{3}  S^{2}_{3}  σ_{v}  σ_{v}’  σ_{v}’’ 
Ψ1  Ψ1  Ψ2  Ψ3  Ψ1  Ψ3  Ψ2  Ψ1  Ψ2  Ψ3  Ψ1  Ψ3  Ψ2 
a1’  1  1  1  1  1  1  1  1  1  1  1  1 
LGO1  Ψ1  Ψ2  Ψ3  Ψ1  Ψ3  Ψ2  Ψ1  Ψ2  Ψ3  Ψ1  Ψ3  Ψ2 
Ψ (a1') = 4Ψ1+4Ψ2+4Ψ3
= 4(Ψ1+Ψ2+Ψ3)
Ψ(a1')= 1/√3 (Ψ1+Ψ2+Ψ3)
The shape of the LGO1 is
D_{3h}  E  C_{3}  C^{2}_{3}  C_{2}  C_{2}’  C_{2}’’  σ_{h}  S_{3}  S^{2}_{3}  σ_{v}  σ_{v}’  σ_{v}’’ 
Ψ1  Ψ1  Ψ2  Ψ3  Ψ1  Ψ3  Ψ2  Ψ1  Ψ2  Ψ3  Ψ1  Ψ3  Ψ2 
e’  2  1  1  0  0  0  2  1  1  0  0  0 
LGO1  2Ψ1  Ψ2  Ψ3  0  0  0  2Ψ1  Ψ2  Ψ3  0  0  0 
Ψ(e') = 4 (Ψ1)2 (Ψ2)2 (Ψ3)
= 2[ 2(Ψ1)Ψ2Ψ3]
Ψ(e') = 1/ √6 (2 Ψ1Ψ2Ψ3)
The shape of the LGO2 is
Noticed that in the LGO2, we have 1 nodal plane which is the horizonal line between the positive charge and negative charge. Therefore, the LGO3 (doubly degenerate with e') would also 1 nodal plane and its wavefunction would be Ψ(e') = 1/√2 (Ψ2Ψ3). The shape of the LGO3 is
MO diagram
As we can see in this diagram, the energy level of 3 LGOs are higher than the 2s orbital and below the 2 p orbital dued to the electronegativy of both Boron and Hydrogen. Hydrogen has higher electronegativity than boron, therefore hydrogen would have lower energy level in the MO diagram.
In addition, B has 3 electrons in the valence electrons and 3 hydrogens have total 3 electrons. Therefore, the total number of electrons filled in orbitals are 6. With all of the informations above about symmetry labels of B atom and the 3 LGOs, we now construct the MO diagram of BH3. Noticed that, the bonding formation only happens to atoms that have the same symmetry labels. 2s orbital and LGO(1) would contribute 1 electron to give 2 spin pairs electrons at the a_{1}' energy level. 2p_{x} and 2p_{y} orbitals would bond to the LGO(2) and LGO(3), which give 2 spin pairs electrons at the e' energy level.
FIGURE 3: MO diagram for the formation of BH3
there is a detailed explaination that performed in this video
References
 Pople, John A.. Approximate Molecular Orbital Theory (Advanced Chemistry). New York: McgrawHill (Tx), 1970. Print., Phy Sci Engr Library QD461. P66
 Noebe, Guillermo (EDT)/, Ronald D. (EDT)/ Abel, and Phillip B. (EDT) Bozzolo. Applied Computational Materials Modeling. Berlin and Heidelberg: Springer Verlag, 2007. Print. Phy Sci Engr Library TA 404.23.A66
 Housecroft, Catherine, and Alan G. Sharpe. Housecroft Inorganic Chemistry 3e (3rd Edition). 3 ed. Alexandria, VA: Prentice Hall, 2008. 128
Outside Links
Problems
 What are the nonbonding orbital in this BH_{3}? '
 In the above MO diagram, why does e' have 2 lines energy levels compared to a1' has only 1 line energy level?
 What is the bond order of BH3 in this MO diagram?
 Assume that we have d orbitals in this BH_{3}, what are symmetry labels that dorbitals have based on the character table?
 Explain why a1' has the lowest energy level in the MO diagram.
Answers
 a2''
 because e' is doubly degenerate molecule orbital.
 B.O = 3
 a1' + e' + e''
 a1' has no node, so it is stable and has lowest energy compare to e'.