2019
DOI: 10.1007/s10876-019-01574-z
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2-Chlorobenzoate Complex of Cu(II): Unexpected Appearance of Halogen···Halogen Contacts in Solid State

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Cited by 12 publications
(4 citation statements)
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“…), and very close to zero positive energy density (0.001 a.u.) in these bond critical points (3, −1) and estimated strength of appropriate contacts (0.9–1.8 kcal/mol) are typical for weak noncovalent interactions involving halogen atoms in similar chemical systems [22,64–72] . The balance between the Lagrangian kinetic energy G( r ) and potential energy density V( r ) at the bond critical points (3, −1) (the ratio −G( r )/V( r ) >1) reveals that a covalent contribution in all intermolecular interactions S⋅⋅⋅X (X=Cl and Br) in the X‐ray structures 1 and 2 is absent [73] .…”
Section: Resultsmentioning
confidence: 94%
See 1 more Smart Citation
“…), and very close to zero positive energy density (0.001 a.u.) in these bond critical points (3, −1) and estimated strength of appropriate contacts (0.9–1.8 kcal/mol) are typical for weak noncovalent interactions involving halogen atoms in similar chemical systems [22,64–72] . The balance between the Lagrangian kinetic energy G( r ) and potential energy density V( r ) at the bond critical points (3, −1) (the ratio −G( r )/V( r ) >1) reveals that a covalent contribution in all intermolecular interactions S⋅⋅⋅X (X=Cl and Br) in the X‐ray structures 1 and 2 is absent [73] .…”
Section: Resultsmentioning
confidence: 94%
“…in these bond critical points (3, À 1) and estimated strength of appropriate contacts (0.9-1.8 kcal/mol) are typical for weak noncovalent interactions involving halogen atoms in similar chemical systems. [22,[64][65][66][67][68][69][70][71][72] The balance between the Lagrangian kinetic energy G(r) and potential energy density V(r) at the bond critical points (3, À 1) (the ratio À G(r)/V(r) > 1) reveals that a covalent contribution in all intermolecular interactions S•••X (X = Cl and Br) in the X-ray structures 1 and 2 is absent. [73] The Laplacian of electron density is typically decomposed into the sum of contributions along the three principal axes of maximal variation, giving the three eigenvalues of the Hessian matrix (λ 1 , λ 2 and λ 3 ), and the sign of λ 2 can be utilized to distinguish bonding (attractive, λ 2 < 0) weak interactions from non-bonding ones (repulsive, λ 2 > 0).…”
Section: Dft Calculationsmentioning
confidence: 99%
“…This type I CÀ Cl•••ClÀ C geometry is found in a significant number of chlorinated crystal structures. [65] Although they are relatively weak, these contacts have been shown to play a role in the packing and properties of several molecular crystals , [31,66] The network of unconventional non-covalent interactions described above forms a complex molecular packing that extends in three dimensions (Figure 3).…”
Section: Resultsmentioning
confidence: 99%
“…In recent years, several studies have articulated the predilection of halogens to participate in s-hole interactions, foregrounding the premier role of halogenÁ Á Áhalogen contacts in materials science and crystal engineering. [34][35][36] To be precise, halogens exhibited an elegant propensity to participate in donor-acceptor interactions within two different types of halogenÁ Á Áhalogen contacts; [36][37][38][39] type I: in which the A-halogenÁ Á Áhalogen angle (y 1 ) is nearly equal to the halogenÁ Á Áhalogen-A angle (y 2 ); and type II: in which the y 1 angle is about 1801 and y 2 is about 901 (see Fig. 1).…”
Section: Introductionmentioning
confidence: 99%