5 research outputs found
Investigation on the Behavior of Noise in Asynchronous Spectra in Generalized Two-Dimensional (2D) Correlation Spectroscopy and Application of Butterworth Filter in the Improvement of Signal-to-Noise Ratio of 2D Asynchronous Spectra
The
behavior of noise in asynchronous spectrum in generalized two-dimensional
(2D) correlation spectroscopy is investigated. Mathematical analysis
on the noise of 2D spectra and computer simulation on a model system
show that the fluctuation of noise in a 2D asynchronous spectrum can
be characterized by the standard deviation of noise in 1D spectra.
Furthermore, a new approach to improve a signal-to-noise ratio of
2D asynchronous spectrum by a Butterworth filter is developed. A strategy
to determine the optimal conditions is proposed. Computer simulation
on a model system indicates that the noise of 2D asynchronous spectrum
can be significantly suppressed using the Butterworth filtering. In
addition, we have tested the approach to a real chemical system where
interaction between berberine and β-cyclodextrin is investigated
using 2D UV–vis asynchronous spectra. When artificial noise
is added, cross peaks that reflect intermolecular interaction between
berberine and β-cyclodextrin are completely masked by noise.
After the method described in this article is utilized, noise is effectively
suppressed, and cross peaks are faithfully recovered. The above result
demonstrates that the approach described in this article is applicable
in real chemical systems
Novel Method of Constructing Two-Dimensional Correlation Spectroscopy without Subtracting a Reference Spectrum
In
this study, we propose a new approach to generate two-dimension
spectra to enhance the intensity of cross peaks relevant to intermolecular
interaction. We investigate intermolecular interaction between two
solutes (denoted as P and Q, where P has a characteristic peak at <i>X</i><sub>P</sub>) dissolved in the same solvent via the near
diagonal cross peaks around the coordinate (<i>X</i><sub>P</sub>, <i>X</i><sub>P</sub>) in a two-dimensional (2D)
asynchronous spectrum of generalized spectroscopy. Because of physical
constrains in many cases, the variation ranges of the initial concentrations
of P or Q must be kept very narrow, leading to very weak cross peak
intensities. The weak cross peaks vulnerable to noise bring about
difficulty in the investigation of subtle intermolecular interaction.
Herein, we propose a new of way constructing a 2D asynchronous spectrum
without the subtraction of the average spectrum often used as a reference
spectrum. Mathematical analysis and computer simulation demonstrate
that the near diagonal cross peaks around the coordinate (<i>X</i><sub>P</sub>, <i>X</i><sub>P</sub>) in the 2D
asynchronous spectrum using the new approach possess two characteristics:
(1) they can still reflect an intermolecular interaction reliably;
2) the absolute intensities of the cross peaks are significantly stronger
than those generated by the conventional method. We incorporate the
novel method with the DAOSD (double asynchronous orthogonal sample
design scheme) approach and applied the modified DAOSD approach to
study hydrogen bonding behavior in diethyl either/methanol/THF system.
The new approach made the weak cross peaks, which are not observable
in 2D asynchronous spectrum generated using conventional approach,
become observable. The appearance of the cross peak demonstrate that
When a small amount of THF is introduced into diethyl solution containing
low amount of methanol, THF breaks the methanol–diethyl ether
complex and forms methanol-THF complex via new hydrogen bond. This
process takes place in spite of the fact that the content of diethyl
ether is overwhelmingly larger than that of THF. The above result
demonstrates that the new approach described in this article is applicable
to enhance intensity of cross peaks in real chemical systems
Double Asynchronous Orthogonal Sample Design Scheme for Probing Intermolecular Interactions
This paper introduces a new approach called double asynchronous
orthogonal sample design (DAOSD) to probe intermolecular interactions.
A specifically designed concentration series is selected according
to the mathematical analysis to generate useful 2D correlated spectra.
As a result, the interfering portions are completely removed and a
pair of complementary sub-2D asynchronous spectra can be obtained.
A computer simulation is applied on a model system with two solutes
to study the spectral behavior of cross peaks in 2D asynchronous spectra
generated by using the DAOSD approach. Variations on different spectral
parameters, such as peak position, bandwidth, and absorptivity, caused
by intermolecular interactions can be estimated by the characteristic
spectral patterns of cross peaks in the pair of complementary sub-2D
asynchronous spectra. Intermolecular interactions between benzene
and iodine in CCl<sub>4</sub> solutions were investigated using the
DAOSD approach to prove the applicability of the DAOSD method in real
chemical system
Sugar–Metal Ion Interactions: The Complicated Coordination Structures of Cesium Ion with d‑Ribose and <i>myo</i>-Inositol
The novel cesium chloride–d-ribose complex (CsCl·C<sub>5</sub>H<sub>10</sub>O<sub>5</sub>; Cs-R) and cesium chloride–<i>myo</i>-inositol
complex (CsCl·C<sub>6</sub>H<sub>12</sub>O<sub>6</sub>; Cs-I)
have been synthesized and characterized using X-ray diffraction and
FTIR, FIR, THz, and Raman spectroscopy. Cs<sup>+</sup> is eight-coordinated
to three chloride ions, O1 and O2 from one d-ribose molecule,
O1 from another d-ribose molecule, and O4 and O5 from the
third d-ribose molecule in Cs-R. For one d-ribose
molecule, the oxygen atom O1 in the ring is coordinated to two cesium
ions as an oxygen bridge, O2 is cocoordinated with O1 to one of the
two cesium ions, and O4 and O5 are coordinated to the third cesium
ion, respectively. O3 does not coordinate to metal ions and only takes
part in forming hydrogen bonds. One chloride ion is connected to three
cesium ions. Thus, a complicated structure of Cs–d-ribose forms. For Cs-I, Cs<sup>+</sup> is 10-coordinated to three
chloride ions, O1 and O2 from one <i>myo</i>-inositol molecule,
O3 and O4 from another <i>myo</i>-inositol molecule, O5
and O6 from the third <i>myo</i>-inositol molecule, and
O6 from the fourth <i>myo</i>-inositol molecule. One metal
ion is connected to four ligands, and one <i>myo</i>-inositol
is coordinated to four Cs<sup>+</sup> ions, which is also a complicated
coordination structure. Crystal structure results, FTIR, FIR, THz,
and Raman spectra provide detailed information on the structure and
coordination of hydroxyl groups to metal ions in the cesium chloride–d-ribose and cesium chloride–<i>myo</i>-inositol
complexes
Sugar–Metal Ion Interactions: The Complicated Coordination Structures of Cesium Ion with d‑Ribose and <i>myo</i>-Inositol
The novel cesium chloride–d-ribose complex (CsCl·C<sub>5</sub>H<sub>10</sub>O<sub>5</sub>; Cs-R) and cesium chloride–<i>myo</i>-inositol
complex (CsCl·C<sub>6</sub>H<sub>12</sub>O<sub>6</sub>; Cs-I)
have been synthesized and characterized using X-ray diffraction and
FTIR, FIR, THz, and Raman spectroscopy. Cs<sup>+</sup> is eight-coordinated
to three chloride ions, O1 and O2 from one d-ribose molecule,
O1 from another d-ribose molecule, and O4 and O5 from the
third d-ribose molecule in Cs-R. For one d-ribose
molecule, the oxygen atom O1 in the ring is coordinated to two cesium
ions as an oxygen bridge, O2 is cocoordinated with O1 to one of the
two cesium ions, and O4 and O5 are coordinated to the third cesium
ion, respectively. O3 does not coordinate to metal ions and only takes
part in forming hydrogen bonds. One chloride ion is connected to three
cesium ions. Thus, a complicated structure of Cs–d-ribose forms. For Cs-I, Cs<sup>+</sup> is 10-coordinated to three
chloride ions, O1 and O2 from one <i>myo</i>-inositol molecule,
O3 and O4 from another <i>myo</i>-inositol molecule, O5
and O6 from the third <i>myo</i>-inositol molecule, and
O6 from the fourth <i>myo</i>-inositol molecule. One metal
ion is connected to four ligands, and one <i>myo</i>-inositol
is coordinated to four Cs<sup>+</sup> ions, which is also a complicated
coordination structure. Crystal structure results, FTIR, FIR, THz,
and Raman spectra provide detailed information on the structure and
coordination of hydroxyl groups to metal ions in the cesium chloride–d-ribose and cesium chloride–<i>myo</i>-inositol
complexes