37 research outputs found
Nose Structure Delineation of Bouguer Anomaly as the Interpretation Basis of Probable Hydrocarbon Traps: a Case Study on the Mainland Area of Northwest Java Basin
DOI: 10.17014/ijog.v7i3.144Two important aspects in the exploration of oil and gas are technology and exploration concepts, but the use of technology is not always suitable for areas with geological conditions covered by young volcanic sediments or limestone. The land of the Northwest Java Basin is mostly covered by young volcanic products, so exploration using seismic methods will produce less clear image resolution. To identify and interpret the subsurface structure and the possibility of hydrocarbon trap, gravity measurements have been carried out. Delineation of nose structures of a Bouguer anomaly map was used to interpret the probability of hydrocarbon traps. The result of the study shows that the gravity anomalies could be categorized into three groups : low anomaly (< 34 mgal), middle anomaly (34 - 50 mgal), and high anomaly (> 50 mgal). The analysis of Bouguer anomaly indicates that the low anomaly is concentrated in Cibarusa area as a southern part of Ciputat Subbasin, and in Cikampek area. The result of delineation of the Bouguer anomaly map shows the nose structures existing on Cibinong-Cileungsi and Pangkalan-Bekasi Highs, while delineation of residual anomaly map shows the nose structures occurs on Cilamaya-Karawang high. Locally, the gas fields of Jatirangon and Cicauh areas exist on the flank of the nose structure of Pangkalan-Bekasi High, while the oil/gas field of Northern Cilamaya is situated on the flank of the nose structure of Cilamaya-Karawang High. The concept of fluid/gas migration concentrated on nose structures which are delineated from gravity data can be applied in the studied area. This concept needs to be tested in other oil and gas field areas
Shedding Light on the Single-Molecule Magnet Behavior of Mononuclear Dy<sup>III</sup> Complexes
General requirements
for obtaining Dy<sup>III</sup> single-molecule magnets (SMM) were
studied by CASSCF+RASSI calculations on both real and model systems.
A set of 20 Dy<sup>III</sup> complexes was considered using their
X-ray crystal structure for our calculations. Theoretical results
were compared with their experimental slow relaxation data, and general
conclusions about the calculated key parameters related with SMM behavior
are presented. The effect of the coordination geometry and nature
of ligands is discussed based on calculations on real and model systems.
We found two different patterns to exhibit SMM behavior: the first
one leads to the largest axial anisotropy in complexes showing heterolepticity
of the ligand environment (more important than symmetric requirements),
while the second one corresponds to sandwich-shaped complexes with
a smaller anisotropy. Thus, most existing mononuclear zero-field SMMs
adopting a heteroleptic coordination mode mixing neutral and anionic
ligands present the same pattern in the electrostatic potential induced
by their ligands, with a lower potential island related to the presence
of neutral ligands inside a high potential background related with
anionic groups. The existence of different electrostatic regions caused
by the ligands induces a preferential orientation to reduce the electron
repulsion for the electron density of the Dy<sup>III</sup> cations,
resulting in the magnetic anisotropy
Coherent Transport through Spin-Crossover Single Molecules
Coherent quantum transport calculations were performed
for high-
and low-spin states of a mononuclear Fe<sup>II</sup> complex showing
spin-crossover behavior using density functional theory methods combined
with the non-equilibrium Green functions procedure. The high-spin
state has a larger conductivity than the low-spin state; furthermore,
it behaves as a spin filter, giving a Ī²-polarized current
Theoretical Modeling of the Ligand-Tuning Effect over the Transition Temperature in Four-Coordinated Fe<sup>II</sup> Molecules
Spin-crossover molecules are systems
of great interest due to their
behavior as molecular level switches, which makes them promising candidates
for nanoscale memory devices, among other applications. In this paper,
we report a computational study for the calculation of the transition
temperature (<i>T</i><sub>1/2</sub>), a key physical quantity
in the characterization of spin-crossover systems, for the family
of tetracoordinated Fe<sup>II</sup> transition-metal complexes of
generic formula [PhBĀ(MesIm)<sub>3</sub>ĀFeNPR<sub>1</sub>R<sub>2</sub>R<sub>3</sub>]. Our calculations correctly reproduce the experimentally
reported decrease in the <i>T</i><sub>1/2</sub> with an
increasing size of the phosphine and allow for the prediction of the <i>T</i><sub>1/2</sub> in new members of the family that are not
reported so far. More importantly, further insight into the factors
that control the fine-tuning of the <i>T</i><sub>1/2</sub> can be obtained by direct analysis of the underlying electronic
structure in terms of the relevant molecular orbitals
Electronic and Steric Control of the Spin-Crossover Behavior in [(Cp<sup>R</sup>)<sub>2</sub>Mn] Manganocenes
A computational
study of the spin-crossover behavior in the family [(Cp<sup>R</sup>)<sub>2</sub>Mn] (R = Me, <sup><i>i</i></sup>Pr, <sup><i>t</i></sup>Bu) is presented. Using the OPBE functional, the
different electronic and steric effects over the metalās ligand
field are studied, and trends in the spin-crossover-temperature (<i>T</i><sub>1/2</sub>) behavior are presented in terms of the
cyclopentadienyl (Cp) ligand functionalization. Our calculations outlined
a delicate balance between both electronic and steric effects. While
an increase in the number of electron-donating groups increases the
spin-crossover temperature (<i>T</i><sub>1/2</sub>) to the
point that the transition is suppressed and only the low-spin state
is observed, steric effects play an opposite role, increasing the
distance between the Cp rings, which in turns shifts <i>T</i><sub>1/2</sub> to lower values, eventually stabilizing the high-spin
state. Both effects can be rationalized by exploring the electronic
structure of such systems in terms of the relevant d-based molecular
orbitals
Structures, Magnetochemistry, Spectroscopy, Theoretical Study, and Catechol Oxidase Activity of Dinuclear and Dimer-of-Dinuclear Mixed-Valence Mn<sup>III</sup>Mn<sup>II</sup> Complexes Derived from a Macrocyclic Ligand
The
work in this paper presents syntheses, characterization, magnetic
properties (experimental and density functional theoretical), catecholase
activity, and electrospray ionization mass spectroscopic (ESI-MS positive)
studies of two mixed-valence dinuclear Mn<sup>III</sup>Mn<sup>II</sup> complexes, [Mn<sup>III</sup>Mn<sup>II</sup>LĀ(Ī¼-O<sub>2</sub>CMe)Ā(H<sub>2</sub>O)<sub>2</sub>]Ā(ClO<sub>4</sub>)<sub>2</sub>Ā·H<sub>2</sub>OĀ·MeCN (<b>1</b>) and [Mn<sup>III</sup>Mn<sup>II</sup>LĀ(Ī¼-O<sub>2</sub>CPh)Ā(MeOH)Ā(ClO<sub>4</sub>)]Ā(ClO<sub>4</sub>) (<b>2</b>), and a Mn<sup>III</sup>Mn<sup>II</sup>Mn<sup>II</sup>Mn<sup>III</sup> complex, [{Mn<sup>III</sup>Mn<sup>II</sup>LĀ(Ī¼-O<sub>2</sub>CEt)Ā(EtOH)}<sub>2</sub>(Ī¼-O<sub>2</sub>CEt)]Ā(ClO<sub>4</sub>)<sub>3</sub> (<b>3</b>), derived from the Robson-type
macrocycle H<sub>2</sub>L, which is the [2 + 2] condensation product
of 2,6-diformyl-4-methylphenol and 2,2-dimethyl-1,3-diaminopropane.
In <b>1</b> and <b>2</b> and in two Mn<sup>III</sup>Mn<sup>II</sup> units in <b>3</b>, the two metal centers are bridged
by a bisĀ(Ī¼-phenoxo)-Ī¼-carboxylate moiety. The two Mn<sup>II</sup> centers of the two Mn<sup>III</sup>Mn<sup>II</sup> units
in <b>3</b> are bridged by a propionate moiety, and therefore
this compound is a dimer of two dinuclear units. The coordination
geometry of the Mn<sup>III</sup> and Mn<sup>II</sup> centers are JahnāTeller
distorted octahedral and distorted trigonal prism, respectively. Magnetic
studies reveal weak ferro- or antiferromagnetic interactions between
the Mn<sup>III</sup> and Mn<sup>II</sup> centers in <b>1</b> (<i>J</i> = +0.08 cm<sup>ā1</sup>), <b>2</b> (<i>J</i> = ā0.095 cm<sup>ā1</sup>), and <b>3</b> (<i>J</i><sub>1</sub> = +0.015 cm<sup>ā1</sup>). A weak antiferromagnetic interaction (<i>J</i><sub>2</sub> = ā0.20 cm<sup>ā1</sup>) also exists between the Mn<sup>II</sup> centers in <b>3</b>. DFT methods properly reproduce
the nature of the exchange interactions present in such systems. A
magneto-structural correlation based on MnāO bridging distances
has been proposed to explain the different sign of the exchange coupling
constants. Utilizing 3,5-di-<i>tert</i>-butyl catechol (3,5-DTBCH<sub>2</sub>) as the substrate, catecholase activity of all the three
complexes has been checked in MeCN and MeOH, revealing that all three
are active catalysts with <i>K</i><sub>cat</sub> values
lying in the range 7.5ā64.7 h<sup>ā1</sup>. Electrospray
ionization mass (ESI-MS positive) spectra of the complexes <b>1</b>ā<b>3</b> have been recorded in MeCN solutions, and
the positive ions have been well characterized. ESI-MS positive spectrum
of complex <b>1</b> in presence of 3,5-DTBCH<sub>2</sub> has
also been recorded, and a positive ion, [Mn<sup>III</sup>Mn<sup>II</sup>LĀ(Ī¼-3,5-DTBC<sup>2ā</sup>)]<sup>+</sup>, having most
probably a bridging catecholate moiety has been identified
Huge Magnetic Anisotropy in a Trigonal-Pyramidal Nickel(II) Complex
The
work presented herein shows the experimental and theoretical studies
of a mononuclear nickelĀ(II) complex with the largest magnetic anisotropy
ever reported. The zero-field-splitting <i>D</i> parameter,
extracted from the fits of the magnetization and susceptibility measurements,
shows a large value of ā200 cm<sup>ā1</sup>, in agreement
with the theoretical value of ā244 cm<sup>ā1</sup> obtained
with the CASPT2āRASSI method
Mononuclear Single-Molecule Magnets: Tailoring the Magnetic Anisotropy of First-Row Transition-Metal Complexes
Magnetic anisotropy is the property
that confers to the spin a
preferred direction that could be not aligned with an external magnetic
field. Molecules that exhibit a high degree of magnetic anisotropy
can behave as individual nanomagnets in the absence of a magnetic
field, due to their predisposition to maintain their inherent spin
direction. Until now, it has proved very hard to predict magnetic
anisotropy, and as a consequence, most synthetic work has been based
on serendipitous processes in the search for large magnetic anisotropy
systems. The present work shows how the property can be predicted
based on the coordination numbers and electronic structures of paramagnetic
centers. Using these indicators, two Co<sup>II</sup> complexes known
from literature have been magnetically characterized and confirm the
predicted single-molecule magnet behavior
Mononuclear Single-Molecule Magnets: Tailoring the Magnetic Anisotropy of First-Row Transition-Metal Complexes
Magnetic anisotropy is the property
that confers to the spin a
preferred direction that could be not aligned with an external magnetic
field. Molecules that exhibit a high degree of magnetic anisotropy
can behave as individual nanomagnets in the absence of a magnetic
field, due to their predisposition to maintain their inherent spin
direction. Until now, it has proved very hard to predict magnetic
anisotropy, and as a consequence, most synthetic work has been based
on serendipitous processes in the search for large magnetic anisotropy
systems. The present work shows how the property can be predicted
based on the coordination numbers and electronic structures of paramagnetic
centers. Using these indicators, two Co<sup>II</sup> complexes known
from literature have been magnetically characterized and confirm the
predicted single-molecule magnet behavior
Ferro- to Antiferromagnetic Crossover Angle in Diphenoxido- and Carboxylato-Bridged Trinuclear Ni<sup>II</sup><sub>2</sub>āMn<sup>II</sup> Complexes: Experimental Observations and Theoretical Rationalization
Three
new trinuclear heterometallic Ni<sup>II</sup>āMn<sup>II</sup> complexes have been synthesized using a [NiL] metalloligand, where
H<sub>2</sub>L = <i>N,N</i>ā²-bisĀ(salicylidene)-1,3-propanediamine.
The complexes [(NiL)<sub>2</sub>MnĀ(OCnn)<sub>2</sub>(CH<sub>3</sub>OH)<sub>2</sub>]Ā·CH<sub>3</sub>OH (<b>1</b>), [(NiL)<sub>2</sub>MnĀ(OPh)<sub>2</sub>(CH<sub>3</sub>OH)<sub>2</sub>]Ā[(NiL)<sub>2</sub>MnĀ(OPh)<sub>2</sub>]Ā·H<sub>2</sub>O (<b>2</b>),
and [(NiL)<sub>2</sub>MnĀ(OSal)<sub>2</sub>(CH<sub>3</sub>OH)<sub>2</sub>]Ā·2Ā[NiL] (<b>3</b>) (where OCnn = cinnamate, OPh = phenylacetate,
OSal = salicylate) have been structurally characterized. In all three
complexes, in addition to the double phenoxido bridge, the two terminal
Ni<sup>II</sup> atoms are linked to the central Mn<sup>II</sup> by
means of a <i>syn-syn</i> bridging carboxylate, giving rise
to a linear structure. Complexes <b>1</b> and <b>2</b> with NiāOāMn angles of 97.24 and 96.43Ā°, respectively,
exhibit ferromagnetic interactions (<i>J</i><sub>NiāMn</sub> = +1.38 and +0.50 cm<sup>ā1</sup>, respectively), whereas <b>3</b> is antiferromagnetic (<i>J</i><sub>NiāMn</sub> = ā0.24 cm<sup>ā1</sup>), having an NiāOāMn
angle of 98.51Ā°. DFT calculations indicate that there is a clear
magneto-structural correlation between the NiāOāMn angle
and <i>J</i><sub>NiāMn</sub> values, which is in
agreement with the experimental results