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All results from a given calculation for HBS (hydrogen boron sulfide)

using model chemistry: LSDA/aug-cc-pCVTZ

19 10 17 12 22

States and conformations

State Conformation minimum conformation conformer description state description
1 1 yes C*V 1Σ
Energy calculated at LSDA/aug-cc-pCVTZ
 hartrees
Energy at 0K-422.463197
Energy at 298.15K 
HF Energy-422.463197
Nuclear repulsion energy31.812314
The energy at 298.15K was derived from the energy at 0K and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at LSDA/aug-cc-pCVTZ
Rotational Constants (cm-1) from geometry optimized at LSDA/aug-cc-pCVTZ
B
0.63888

See section I.F.4 to change rotational constant units
Geometric Data calculated at LSDA/aug-cc-pCVTZ

Point Group is C∞v

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
B1 0.000 0.000 -1.107
H2 0.000 0.000 -2.289
S3 0.000 0.000 0.489

Atom - Atom Distances (Å)
  B1 H2 S3
B11.18201.5960
H21.18202.7779
S31.59602.7779

picture of hydrogen boron sulfide state 1 conformation 1
More geometry information
Calculated Bond Angles
atom1 atom2 atom3 angle atom1 atom2 atom3 angle
H2 B1 S3 180.000
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/aug-cc-pCVTZ Charges (e)
Number Element Mulliken CHELPG AIM ESP
1 B -0.023      
2 H 0.037      
3 S -0.014      


Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section VII.A.3)
  x y z Total
  0.000 0.000 -1.200 1.200
CHELPG        
AIM        
ESP        


Electric Quadrupole moment
Quadrupole components in D Å
Primitive
 xyz
x -19.782 0.000 0.000
y 0.000 -19.782 0.000
z 0.000 0.000 -16.390
Traceless
 xyz
x -1.696 0.000 0.000
y 0.000 -1.696 0.000
z 0.000 0.000 3.392
Polar
3z2-r26.784
x2-y20.000
xy0.000
xz0.000
yz0.000


Polarizabilities
Components of the polarizability tensor.
Units are Å3 (Angstrom cubed)
Change units.
  x y z
x 0.000 0.000 0.000
y 0.000 0.000 0.000
z 0.000 0.000 0.000


<r2> (average value of r2) Å2
<r2> 26.841
(<r2>)1/2 5.181