Helder Marques

Prof. Dr. Helder Marques

Molecular Sciences Institute, School of Chemistry, University of the Witwatersrand, Johannesburg 2050, South Africa
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Research Focus & Metrics

Academic Career Length

46Years (1981-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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31 December 1999 in Journal of Medicinal Chemistry
Verified
Journal Article
Closed access
TETimothy J. Egan
Timothy J. Egan
RHRoger Hunter
Roger Hunter
CKCatherine H. Kaschula
Catherine H. Kaschula
Helder MarquesHelder Marques
Helder Marques
AMAshley Misplon
Ashley Misplon
JWJason Walden
Jason Walden

15 July 2002 in Biochemical Journal
Verified
Journal Article
Open access
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TETimothy J. Egan
Timothy J. Egan
JCJill M. Combrinck
Jill M. Combrinck
JEJoanne Egan
Joanne Egan
GHGiovanni R. Hearne
Giovanni R. Hearne
Helder MarquesHelder Marques
Helder Marques
JWJason C. Walden
Jason C. Walden
Chemical analysis has shown that Plasmodium falciparum trophozoites contain 61±2% of the iron within parasitized erythrocytes, of which 92±6% is located within the food vacuole. Of this, 88±9% is in the form of haemozoin. 57Fe-Mössbauer spectroscopy shows that haemozoin is the only detectable iron species in trophozoites. Electron spectroscopic imaging confirms this conclusion.

12 March 2019 in Inorganics
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Journal Article
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Pradeep R. VaradwajPradeep R. Varadwaj
Pradeep R. Varadwaj
Arpita VaradwajArpita Varadwaj
Arpita Varadwaj
Helder MarquesHelder Marques
Helder Marques
In addition to the underlying basic concepts and early recognition of halogen bonding, this paper reviews the conflicting views that consistently appear in the area of noncovalent interactions and the ability of covalently bonded halogen atoms in molecules to participate in noncovalent interactions that contribute to packing in the solid-state. It may be relatively straightforward to identify Type-II halogen bonding between atoms using the conceptual framework of σ-hole theory, especially when the interaction is linear and is formed between the axial positive region (σ-hole) on the halogen in one monomer and a negative site on a second interacting monomer. A σ-hole is an electron density deficient region on the halogen atom X opposite to the R–X covalent bond, where R is the remainder part of the molecule. However, it is not trivial to do so when secondary interactions are involved as the directionality of the interaction is significantly affected. We show, by providing some specific examples, that halogen bonds do not always follow the strict Type-II topology, and the occurrence of Type-I and -III halogen-centered contacts in crystals is very difficult to predict. In many instances, Type-I halogen-centered contacts appear simultaneously with Type-II halogen bonds. We employed the Independent Gradient Model, a recently proposed electron density approach for probing strong and weak interactions in molecular domains, to show that this is a very useful tool in unraveling the chemistry of halogen-assisted noncovalent interactions, especially in the weak bonding regime. Wherever possible, we have attempted to connect some of these results with those reported previously. Though useful for studying interactions of reasonable strength, IUPAC’s proposed “less than the sum of the van der Waals radii” criterion should not always be assumed as a necessary and sufficient feature to reveal weakly bound interactions, since in many crystals the attractive interaction happens to occur between the midpoint of a bond, or the junction region, and a positive or negative site.

10 January 2019 in Scientific Reports
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Journal Article
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Pradeep R. VaradwajPradeep R. Varadwaj
Pradeep R. Varadwaj
Arpita VaradwajArpita Varadwaj
Arpita Varadwaj
Helder MarquesHelder Marques
Helder Marques
KYKoichi Yamashita
Koichi Yamashita
The CH3NH3PbI3(methylammonium lead triiodide) perovskite semiconductor system has been viewed as a blockbuster research material during the last five years. Because of its complicated architecture, several of its technological, physical and geometrical issues have been examined many times. Yet this has not assisted in overcoming a number of problems in the field nor in enabling the material to be marketed. For instance, these studies have not clarified the nature and type of hydrogen bonding and other noncovalent interactions involved; the origin of hysteresis; the actual role of the methylammonium cation; the nature of polarity associated with the tetragonal geometry; the unusual origin of various frontier orbital contributions to the conduction band minimum; the underlying phenomena of spin-orbit coupling that causes significant bandgap reduction; and the nature of direct-to-indirect bandgap transition features. Arising from many recent reports, it is now a common belief that the I···H–N interaction formed between the inorganic framework and the ammonium group of CH3NH3+is the only hydrogen bonded interaction responsible for all temperature-dependent geometrical polymorphs of the system, including the most stable one that persists at low-temperatures, and the significance of all other noncovalent interactions has been overlooked. This study focussed only on the low temperature orthorhombic polymorph of CH3NH3PbI3and CD3ND3PbI3, where D refers deuterium. Together with QTAIM, DORI and RDG based charge density analyses, the results of density functional theory calculations with PBE with and without van der Waals corrections demonstrate that the prevailing view of hydrogen bonding in CH3NH3PbI3is misleading as it does not alone determine thea−b+a−tilting pattern of the PbI64−octahedra. This study suggests that it is not only the I···H/D–N, but also the I···H/D–C hydrogen/deuterium bonding and other noncovalent interactions (viz. tetrel-, pnictogen- and lump-hole bonding interactions) that are ubiquitous in the orthorhombic CH3NH3PbI3/CD3ND3PbI3perovskite geometry. Their interplay determines the overall geometry of the polymorph, and are therefore responsible in part for the emergence of the functional optical properties of this material. This study also suggests that these interactions should not be regarded as the sole determinants of octahedral tilting since lattice dynamics is known to play a critical role as well, a common feature in many inorganic perovskites both in the presence and the absence of the encaged cation, as in CsPbI3/WO3perovskites, for example.

1 November 1997 in Journal of the American Chemical Society
Verified
Journal Article
Closed access
BCBeisong Cheng
Beisong Cheng
OMOrde Q. Munro
Orde Q. Munro
Helder MarquesHelder Marques
Helder Marques
WSW. Robert Scheidt
W. Robert Scheidt

1 November 1997 in Journal of Inorganic Biochemistry
Verified
Journal Article
Closed access
TETimothy J. Egan
Timothy J. Egan
WMWinile W. Mavuso
Winile W. Mavuso
DRDavid C. Ross
David C. Ross
Helder MarquesHelder Marques
Helder Marques