More bugs in basis set intro
- From: jkl' at
\`ccl.net
- Subject: More bugs in basis set intro
- Date: Fri, 15 Mar 91 15:10:10 EST
Mike Zerner (zerner' at \`qtp.ufl.edu Thu Mar 7 19:06:08 1991) found more
bad stuff in my basis set intro. I am really glad that the person of his
experience took the time to read it and write the comments to correct me.
Here are his comments and my "answers":
Jan Labanowski
jkl' at \`ccl.net
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MZ> One of the reasons that core orbitals make their appearance in valence
MZ> and other higher energy orbitals is due to the fact that all mo's must be
MZ> orthogonal. If one examines these coefficients they are very much like
MZ> those you would get from simple Schmidt orthogonalisation to the lower
MZ> lying core orbitals.
JL> Hi Mike,
JL>
JL> I aggree with you that some of my statements in the "Basis Sets
Trilogy"
JL> are at least misleading, if not plain wrong. Only after I heard people's
JL> comments I realised that what I wanted to say and what I actually said
are
JL> two different things. Of course, there are two major reasons for this:
JL> 1) I am truly ignorant is many of these issues, 2) I wanted to be brief,
JL>
JL> My statement that core orbitals are present in HOMO.
JL> What I wanted to imply was: if the basis functions were "true"
atomic
JL> orbitals (i.e. all atomic orbitals on a given center were orthogonal to
JL> each other and overlap between "core" orbitals on different
centers was
JL> negligible) we would not have large participation of core orbitals in
HOMO.
JL> But it seems that I am totally wrong on this. Please help me,since I
simply
JL> do not know. Of course, I probably should go and retake a course
"Quantum
JL> Chemistry for Psychologists 100" but I do not have time. This
perception
JL> comes from my early years when they showed me this diagram for
homonuclear
JL> molecule. If what I said above is not true than these molecular
JL> orbital diagrams are totally misleading and should be abolished.
JL> I would really appreciate your comment on this.
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MZ> I don't understand the discusion above the 66-31 basis set for Si Table.
MZ> If a primitive occurs contracted in a 3 combo , say, x+y+z, and appears
MZ> by itself, say z, why is this linearly dependent? I.e think of three
MZ> dimensional space. DId I read this wrong?
JL> Linear independence. Yes, I did say something else than I wanted to say.
JL> Basis functions:
JL> phi_1 = a_1*g_1 + a_2*g_2 + a_3*g_3 (set I)
JL> phi_2 = g_3
JL> are not linearly dependent.
JL> What I wanted to say is that basis functions
JL> phi_1' = a_1'*g_1 + a_2'*g_2 (set II)
JL> phi_2 = g_3
JL> would yield the basis set of exactly the same quality with the
following
JL> relationship between coefficients in resulting molecular orbitals:
JL>
JL> ... c_1*phi_1 + c_2*phi_2 ... (set I)
JL> and
JL> ... c_1*phi_1' + (c_1*a_3 + c_2)*g_3 (Set II)
JL>
JL> However, since set with "doubled" g_3 (set I) whould take
more time at
JL> integral calculation stage (assuming no support for general
JL> contractions), it would be wasteful not to use basis set II.
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MZ> under 66-31G means that there is :" should this not be S(6/6/3/1)
rather
MZ> than S(6/6/3/2) ?
JL> 66-31G -> is s(6/6/3/1) and not s(6/6/3/2) and it is a typo (another
one).
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MS> The difference between the 2p function on Li, and the 3d on S, is that
the
MS> former is needed for hybridization, and ignoring it ignores all of first
MS> year chemistry! (The first solid state calculations on Li and alkali
MS> halides were done by physists, and of course, did not contain the 2p!).
MS> The 3d function on sulfur is usually polarization, but even this is
MS> somewhat controversial.
JL> p's for Li and d's for S. What I wanted to say is, that designating
JL> a function as "polarization" or "basic" should not be
based on how
JL> obvious or not obvious it is. I would welcome some more precise
criterion,
JL> since "accuracy of the results" and "correctness of
physical picture" is
JL> very subjective (depends on the investigator) and depends on the
particular
JL> system studied.
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