10 research outputs found
Polarization-Consistent versus Correlation-Consistent Basis Sets in Predicting Molecular and Spectroscopic Properties
Compared to the correlation-consistent basis sets, it is not known if polarization-consistent pc-n basis sets,
which were initially developed for HF and DFT calculations, can provide a monotonic and faster convergence
toward the basis-set limit for results at correlated levels as well as better accuracy for a similar number of
basis functions. It is also not known whether the pc-n basis sets can compute second derivatives of energy,
such as nuclear magnetic shielding tensors, efficiently. To address these questions, the pc-n (n = 1−4), cc-pVxZ, and/or aug-cc-pVxZ (x = D, T, Q, 5, and 6) basis sets were used to compute the molecular and/or
spectroscopic parameters of H2, H2O, and NH3 at the RHF, B3-LYP, MP2, and/or CCSD(T) levels of theory.
The results show that compared to the cc-pVxZ and/or aug-cc-pVxZ basis sets the pc-n basis sets yield faster
convergence toward the basis-set limit but equivalent molecular and/or spectroscopic parameters in the basis-set limit at the RHF, DFT, MP2, and CCSD(T) levels. Because the pc-n basis sets show faster convergence,
fewer basis-set functions are needed to reach the accuracy obtained with the aug-cc-pVxZ basis sets, enabling
faster calculations and less computer storage space. The results also show that the pc-n basis sets, in conjunction
with the “locally dense” basis-set approach, could be applied to predict accurate parameters; thus, they could
be used to estimate accurate molecular or spectroscopic properties (e.g., NMR parameters) for larger systems
such as the active site of enzymes
Toward Hartree−Fock- and Density Functional Complete Basis-Set-Predicted NMR Parameters
The molecular and spectroscopic parameters calculated using the hybrid density functional B3PW91 are reported
for a model set of compounds composed of H2, N2, NH3, CH4, C2H4, HCN, CH3CN, and H2O. An estimation
of the DFT and Hartree−Fock complete basis-set limit (CBS) energy and NMR parameters from the 2- (3-)
point exact fit versus least-squares fit (NLLSQ) was obtained with the cc-pVxZ and aug-cc-pVxZ basis sets
(x = D, T, Q, 5, 6). A marginally faster convergence of the fitted parameters obtained with core-valence
basis sets cc-pCVxZ and aug-cc-pCVxZ was noticed. The Hartree−Fock-predicted CBS heavy-atom isotropic
shieldings of the model molecules, as compared with those of DFT, were closer to experiment. It was also
shown that GIAO MP2-predicted NMR parameters yield the best agreement with those obtained from
experiment and benchmark calculations. As support for experimental studies, the CBS approach of calculating
accurate nuclear shieldings of larger molecules is proposed
On the convergence of zero-point vibrational corrections to nuclear shieldings and shielding anisotropies towards the complete basis set limit in water
<p>The method and basis set dependence of zero-point vibrational corrections (ZPVCs) to nuclear magnetic resonance shielding constants and anisotropies has been investigated using water as a test system. A systematic comparison has been made using the Hartree–Fock, second-order Møller–Plesset perturbation theory (MP2), coupled cluster singles and doubles (CCSD), coupled cluster singles and doubles with perturbative triples corrections (CCSD(T)) and Kohn–Sham density functional theory with the B3LYP exchange-correlation functional methods in combination with the second-order vibrational perturbation theory (VPT2) approach for the vibrational corrections. As basis sets, the correlation consistent basis sets cc-pVXZ, aug-cc-pVXZ, cc-pCVXZ and aug-cc-pCVXZ with <i>X</i> = D, T, Q, 5, 6 and the polarisation consistent basis sets aug-pc-n and aug-pcS-n with <i>n</i> = 1, 2, 3, 4 were employed. Our results show that basis set convergence of the vibrational corrections is not monotonic and that very large basis sets are needed before a reasonable extrapolation to the basis set limit can be performed. Furthermore, our results suggest that coupled cluster methods and a decent basis set are required before the error of the electronic structure approach is lower than the inherent error of the VPT2 approximation.</p> <p></p
Convergence of Nuclear Magnetic Shieldings in the Kohn−Sham Limit for Several Small Molecules
Convergence patterns and limiting values of isotropic nuclear magnetic shieldings were studied for several small molecules (N2, CO, CO2, NH3, CH4, C2H2, C2H4, C2H6, and C6H6) in the Kohn−Sham limit. Individual results of calculations using dedicated families of Jensen’s basis sets (pcS-n and pcJ-n) were fitted toward the complete basis set limit (CBS) using a simple two-parameter formula. Several density functionals were used; calculated vibrational corrections (ZPV) applied; and, for comparison purposes, similar calculations performed using RHF, MP2, SOPPA, SOPPA(CCSD), and CCSD(T) methods and additionally, the aug-cc-pVTZ-J basis set. Finally, the CBS estimated results were critically compared with earlier reported literature data and experimental results. Among 42 studied DFT methods, the KTn and “pure” functionals produced the most accurate heavy atom isotropic nuclear shieldings
Efficient Modeling of NMR Parameters in Carbon Nanosystems
Rapid growth of nanoscience
and nanotechnology requires new and more powerful modeling tools.
Efficient theoretical modeling of large molecular systems at the <i>ab initio</i> and Density Functional Theory (DFT) levels of
theory depends critically on the size and completeness of the basis
set used. The recently designed variants of STO-3G basis set (STO-3G<sub>el</sub>, STO-3G<sub>mag</sub>), modified to correctly predict electronic
and magnetic properties were tested on simple models of pristine and
functionalized carbon nanotube (CNT) systems and fullerenes using
the B3LYP and VSXC density functionals. Predicted geometries, vibrational
properties, and HOMO/LUMO gaps of the model systems, calculated with
typical 6-31G* and modified STO-3G basis sets, were comparable. The <sup>13</sup>C nuclear isotropic shieldings, calculated with STO-3G<sub>mag</sub> and Jensen’s polarization consistent pcS-2 basis
sets, were also identical. The STO-3G<sub>mag</sub> basis sets, being
half the size of the latter one, are promising alternative for studying <sup>13</sup>C nuclear magnetic shieldings in larger size CNTs and fullerenes
Basis Set Convergence of Indirect Spin–Spin Coupling Constants in the Kohn–Sham Limit for Several Small Molecules
The performance of more than 40 density functionals in
predicting
indirect spin–spin coupling constants (SSCCs) in the Kohn–Sham
basis set limit was tested. For comparison, similar calculations were performed
using the RHF, SOPPA, SOPPA(CC2), and SOPPA(CCSD) methods, and the
results were estimated toward the complete basis set (CBS) limit.
The SSCCs of nine small molecules (N<sub>2</sub>, CO, CO<sub>2</sub>, NH<sub>3</sub>, CH<sub>4</sub>, C<sub>2</sub>H<sub>2</sub>, C<sub>2</sub>H<sub>4</sub>, C<sub>2</sub>H<sub>6</sub>, and C<sub>6</sub>H<sub>6</sub>) were calculated using the dedicated Jensen pcJ-<i>n</i> polarization-consistent basis sets and used for the CBS limit
estimations within the Kohn–Sham limit. These CBS results were
compared with calculations using the aug-cc-pVTZ-J basis set. Among
the 41 studied DFT methods, the tHCTHhyb, HSEh1PBE, HSE2PBE, wB97XD,
wB97, and wB97X functionals reproduced accurately the experimental <sup>1</sup><i>J</i>(XH) SSCCs and <sup>3</sup><i>J</i>(HH60) and <sup>2</sup><i>J</i>(HH<sub><i>gem</i></sub>) in ethane. Similarly, the functionals HSEh1PBE, HSE2PBE,
wB97XD, wB97, and wB97X predicted accurately <sup>1</sup><i>J</i>(CC), and B98, B97-1, B97-2, PBE1PBE, B1LYP, and O3LYP provided accurate <sup>1</sup><i>J</i>(CO) results in the CO molecule. A very
good performance for the calculation of the SSCCs based on the use
of the relatively small basis set aug-cc-pVTZ-J was observed
Host−Guest Complex Dependent Regioselectivity in Substitution Reactions of Chlorocyclotriphosphazene-Containing PNP-Crowns with Alkylenediamines
Host−Guest Complex Dependent Regioselectivity in
Substitution Reactions of
Chlorocyclotriphosphazene-Containing PNP-Crowns
with Alkylenediamine
Thermodynamic <i>vs</i> Supramolecular Effects in the Regiocontrol of the Formation of New Cyclotriphosphazene-Containing Chiral Ligands with 1,1‘-Binaphthyl Units: Spiro <i>vs</i> Ansa Substitution at the N<sub>3</sub>P<sub>3</sub> Ring
Synthesis of new cyclophosphazene-containing chiral
ligands (6−9) with 1,1‘-binaphthyl units has
been
achieved by stepwise dicyclosubstitution of
hexachlorocyclotriphosphazene (1), with two sodium cation
paired
dinucleophiles derived from bis-β-naphthol (2) and
tetraethylene glycol (3). The structures of the
disubstitution
products have been found to be addition order-dependent. In
particular, the substitution pattern of the 1,1‘-binaphthalene-2,2‘-dioxy substituent in the N3P3
ring [spiro (4 → 6, 7) or ansa
(8, 9)] was related to whether or
not
the crown substituent had been incorporated into 1
beforehand. Addition of the phase transfer catalyst
reagent,
tetrabutylammonium bromide, to the reaction mixture of 5 +
2-Na2 led to the parallel formation
of both the spiro
6 and ansa 8 isomers. Spiro vs
ansa regioisomerism of the binaphthalenedioxy derivatives formed is
discussed in
terms of the contributions of the respective thermodynamic and
supramolecular effects to the regiocontrol of substitution
in the N3P3 ring. It is found that there
are two main factors determining the orientation of the
binaphthalenedioxy
substitutent incoming to the N3P3 ring: the
thermodynamic stability of seven-membered spirocycles at the
P-atoms
and the crown-related cation assistance of the ansa substitution at the
macrocycle bearing P-atoms; the regiocontrol
resulting from the supramolecular effects predominates, whenever
possible. The structures of compounds 7−9
were
proven by X-ray crystallography. The metal cation complexing
properties of compounds 6−9 were compared by
a
simple TLC method. The results show that the complexing properties
of the chiral binaphthalenedioxy-containing
PNP-crown ligands 6−9 toward alkali metal and
silver cations are either similar (spiro-ansa derivative 6)
or enhanced
(bis-ansa derivatives 7−9) with respect to the
parent tetrachloro PNP-crown 5
A Regioselective Route to New Polytopic Receptors by Diaminolysis of Chlorocyclotriphosphazatriene-Containing Crown Ethers
A general strategy is reported for the facile preparation of diamino-derivatized PNP-crowns, giving
access to a large range of new host molecules of different sizes, shapes, and topology. Reactions of
the tetrachloro-PNP-crown precursor 1 with polymethylene-diamines 2a−h (n = 2−6, 8, 10, 12)
proceed rapidly and regioselectively via substitution reactions of Cl at the PNP-crown-forming
P-atoms; the reaction is assisted by the macrocyclic 1,3-oxy(tetraethylenoxy) substituent at the
N3P3 ring which provides a site for the hydrogen-bond-driven assembly of reagents 1 and 2. The
products belong to three different classes of polytopic receptors: lateral macrobicycles (ansa, 5a−h), bola-amphiphilic tritopic bis-crowns (bino, 6a−h), and tetratopic cylindrical macrotricycles (bis-bino, 8a−h). The structures of 5, 6, 8, and 10b were established by MS and 31P NMR spectroscopy,
and an X-ray crystal structure was obtained for the bis-bino 1,3-diaminopropane PNP-crown
derivative 8b. Preliminary screening by a simple TLC test of the metal−cation complexing properties
of the series of compounds 5, 6, and 8 revealed their capacity to bind both harder (alkali and alkaline
earth) and softer (transition) metal cations, with significant affinity being displayed toward
potassium and silver cations by many of the ligands studied
