Charge Models#
Minimal Basis Iterative Stockholder (MBIS)#
The Minimal Basis Iterative Stockholder (MBIS) [Ayers2016] method is a variant of the Hirshfeld method. The idea behind this approach is to expand the pro-atomic density in a minimal set of atom-centered s-type Slater functions. MBIS is used in various applications like Force-Field parameterization or rescaling atomic polarizabilities.
MBIS charges can easily be requested by the simple input keyword MBIS
:
!wB97X-V DEF2-TZVP MBIS
Within ORCA its also possible to compute atomic dipole-, quadrupole-, and octupolemoments within the MBIS scheme. These can be printed via the extended output option:
%method
MBIS_LARGEPRINT TRUE # default = FALSE
end
There are various further options to use with MBIS that can be found in the ORCA manual.
Example: 5,6-diaminobenzene-2,3-dicarbonitrile#
In this example, we will compute MBIS properties for 5,6-diaminobenzene-2,3-dicarbonitrile. This molecules has, for a neutral compound, a high experimental dipole moment of 10.5±0.2 Debye [Müllen2016].
To obtain the MBIS charges and atomic multipoles we can employ the following input:
!wB97X-V DEF2-TZVP MBIS
%method
MBIS_LARGEPRINT TRUE # default = FALSE
end
We can now find the MBIS charges in the output file basename.out
:
------------------
MBIS ANALYSIS
------------------
Convergence threshold (charges) ... 1.000e-06
Number of iterations ... 74
Total integrated alpha density ... 52.999978264
Total integrated beta density ... 52.999978264
ATOM CHARGE POPULATION SPIN
0 N -0.843178 7.843178 0.000000
1 C 0.263789 5.736211 0.000000
2 C 0.263801 5.736199 0.000000
3 N -0.843087 7.843087 0.000000
4 C -0.257154 6.257154 0.000000
5 H 0.386423 0.613577 0.000000
6 C -0.027760 6.027760 0.000000
7 C 0.356352 5.643648 0.000000
8 C -0.027763 6.027763 0.000000
9 C 0.356292 5.643708 0.000000
10 C -0.257237 6.257237 0.000000
11 H 0.386406 0.613594 0.000000
12 H 0.384292 0.615708 0.000000
13 N -0.433365 7.433365 0.000000
14 N -0.433376 7.433376 0.000000
15 H 0.384314 0.615686 0.000000
16 H 0.170620 0.829380 0.000000
17 H 0.170678 0.829322 0.000000
TOTAL 0.000048 81.999952 0.000000
The charges mapped to to respective atoms are:
As we requested the large printout we also find the atomic dipole-
MBIS ATOMIC DIPOLE MOMENT (A.U.):
ATOM X Y Z
0 N -0.038066 -0.015118 -0.103029
[...]
quadrupole-, and
MBIS ATOMIC QUADRUPOLE MOMENT (A.U.):
ATOM XX YY ZZ XY XZ YZ
0 N -5.193059 -5.361218 -5.246343 -0.051584 0.008768 0.095351
[...]
octupole moments
MBIS ATOMIC OCTUPOLE MOMENT (A.U.):
ATOM XXX YYY ZZZ XXY XXZ XYY XYZ XZZ YYZ YZZ
0 N -0.327912 0.056948 -0.069312 -0.055253 -0.039152 -0.006909 0.012998 0.314205 -0.394240 -0.035321
[...]
Note
Note that there are various other charge models available within ORCA including Mulliken, Hirshfeld, and more.
Starting structure#
5,6-diaminobenzene-2,3-dicarbonitrile
18
N 1.34721241437119 -0.19875204578868 2.39728170838216
C 0.70867203692614 -0.08409568583235 1.17165794089898
C -0.69557523765992 -0.03503410755084 1.15547373801566
N -1.36695245837416 -0.05357620226644 2.36862799274125
C -1.35463448913564 0.08033827321651 -0.05146262039998
H 2.34810629260485 -0.10903909384438 2.36022439042418
C -0.65492341506459 0.11650354440257 -1.24923904175946
C -1.38024608777480 0.22912849642218 -2.47568708881038
C 0.73267914111713 0.02684352514116 -1.23535246715296
C 1.49072510922012 0.04700848828691 -2.44697511349353
C 1.40013842906872 -0.06847776855218 -0.02246437719730
H -2.36630779122682 -0.13781135092574 2.29511415417341
H 0.95194597461754 0.38337577789381 3.11975943676764
N -1.98904585311221 0.31503849289177 -3.44573900381660
N 2.12487320894712 0.06661771348260 -3.40431289691542
H -0.98996937874613 -0.71100834890760 3.03401439822709
H -2.43381979990049 0.12883159310508 -0.07188432898727
H 2.47966190412196 -0.11602130117439 -0.01964682109748