7 research outputs found
Highly Sensitive and Automated Surface Enhanced Raman Scattering-based Immunoassay for H5N1 Detection with Digital Microfluidics
Digital
microfluidics (DMF) is a powerful platform for a broad
range of applications, especially immunoassays having multiple steps,
due to the advantages of low reagent consumption and high automatization.
Surface enhanced Raman scattering (SERS) has been proven as an attractive
method for highly sensitive and multiplex detection, because of its
remarkable signal amplification and excellent spatial resolution.
Here we propose a SERS-based immunoassay with DMF for rapid, automated,
and sensitive detection of disease biomarkers. SERS tags labeled with
Raman reporter 4-mercaptobenzoic acid (4-MBA) were synthesized with
a core@shell nanostructure and showed strong signals, good uniformity,
and high stability. A sandwich immunoassay was designed, in which
magnetic beads coated with antibodies were used as solid support to
capture antigens from samples to form a beads–antibody–antigen
immunocomplex. By labeling the immunocomplex with a detection antibody-functionalized
SERS tag, antigen can be sensitively detected through the strong SERS
signal. The automation capability of DMF can greatly simplify the
assay procedure while reducing the risk of exposure to hazardous samples.
Quantitative detection of avian influenza virus H5N1 in buffer and
human serum was implemented to demonstrate the utility of the DMF-SERS
method. The DMF-SERS method shows excellent sensitivity (LOD of 74
pg/mL) and selectivity for H5N1 detection with less assay time (<1
h) and lower reagent consumption (∼30 μL) compared to
the standard ELISA method. Therefore, this DMF-SERS method holds great
potentials for automated and sensitive detection of a variety of infectious
diseases
Probing Hydrogen Bond Energies by Mass Spectrometry
Mass spectrometry with desorption
electrospray ionization (DESI)
is demonstrated to be useful for probing the strength of hydrogen
bonding, exemplified by various complexes of benzothiazoles and carboxylic
acids in the solid state. Efficiencies for fragmentation of the complexes,
quantified by collision-induced dissociation (CID) technology, correspond
well with energies of the hydrogen bonds of O–H···N
and N–H···O bridging each pair of benzothiazole
and carboxylic acid. Linear correlations (with correlation factors
of 0.8953 and 0.9928) have been established for the calibration curves
of normalized collision energy at 100% fragmentation rate vs the length
between donor and acceptor (in the hydrogen bond of O–H···N)
as well as the slope of the fragmentation efficiency curve vs the
average length difference between O–H···N and
N–H···O in the complex. The mechanism responsible
for determination of the hydrogen bonds is proposed on the basis of
the experiments starting from the mixtures of the complexes as well
as labeling with deuterium. As a complement of previously available
methods (e.g., X-ray diffraction analysis), expectably, the proposed
mass spectrometric method seems to be versatile for probing hydrogen
bond energies
Probing Hydrogen Bond Energies by Mass Spectrometry
Mass spectrometry with desorption
electrospray ionization (DESI)
is demonstrated to be useful for probing the strength of hydrogen
bonding, exemplified by various complexes of benzothiazoles and carboxylic
acids in the solid state. Efficiencies for fragmentation of the complexes,
quantified by collision-induced dissociation (CID) technology, correspond
well with energies of the hydrogen bonds of O–H···N
and N–H···O bridging each pair of benzothiazole
and carboxylic acid. Linear correlations (with correlation factors
of 0.8953 and 0.9928) have been established for the calibration curves
of normalized collision energy at 100% fragmentation rate vs the length
between donor and acceptor (in the hydrogen bond of O–H···N)
as well as the slope of the fragmentation efficiency curve vs the
average length difference between O–H···N and
N–H···O in the complex. The mechanism responsible
for determination of the hydrogen bonds is proposed on the basis of
the experiments starting from the mixtures of the complexes as well
as labeling with deuterium. As a complement of previously available
methods (e.g., X-ray diffraction analysis), expectably, the proposed
mass spectrometric method seems to be versatile for probing hydrogen
bond energies
Pentagon-Fused Hollow Fullerene in C<sub>78</sub> Family Retrieved by Chlorination
C78 is one of the most widely investigated higher fullerenes. Among its huge isomer family, only one non-IPR (IPR = isolated pentagon ring) cage, the C2-symmetric #22010C78, was previously stabilized by endohedral derivatization. Here we report a new C1-symmetric non-IPR hollow isomer, #23863C78, which was captured as #23863C78Cl8 and then subjected to a regioselective substitution reaction with benzyl hydroperoxide to form #23863C78(OOCH2C6H5)Cl7. The structural connectivity of #23863C78, which contains a pair of fused pentagons, was confirmed by single-crystal X-ray diffraction analysis of the #23863C78(OOCH2C6H5)Cl7 molecule, which shares the same fullerene core with #23863C78Cl8; support for the structure is provided by comparable IR measurements and computation. Theoretical studies suggest that the differences in C−Cl bond length, intermediate stability, and steric effects of the involved molecules account for the chemical regioselectivity of the substitution reaction
Hierarchical Assembly of a {Mn<sup>II</sup><sub>15</sub>Mn<sup>III</sup><sub>4</sub>} Brucite Disc: Step-by-Step Formation and Ferrimagnetism
In
search of functional molecular materials and the study of their
formation mechanism, we report the elucidation of a hierarchical step-by-step
formation from monomer (Mn) to heptamer (Mn<sub>7</sub>) to nonadecamer
(Mn<sub>19</sub>) satisfying the relation 1 + Σ<sub><i>n</i></sub>6<i>n</i>, where <i>n</i> is
the ring number of the Brucite structure using high-resolution electrospray
ionization mass spectrometry (HRESI-MS). Three intermediate clusters,
Mn<sub>10</sub>, Mn<sub>12</sub>, and Mn<sub>14</sub>, were identified.
Furthermore, the Mn<sub>19</sub> disc remains intact when dissolved
in acetonitrile with a well-resolved general formula of [Mn<sub>19</sub>(<i>L</i>)<sub><i>x</i></sub>(OH)<sub><i>y</i></sub>(N<sub>3</sub>)<sub>36–<i>x</i>−<i>y</i></sub>]<sup>2+</sup> (<i>x</i> = 18, 17, 16; <i>y</i> = 8, 7, 6; H<i>L</i> = 1-(hydroxymethyl)-3,5-dimethylpyrazole) indicating progressive
exchange of N<sub>3</sub><sup>–</sup> for OH<sup>–</sup>. The high symmetry (<i>R</i>-3) Mn<sub>19</sub> crystal
structure consists of a well-ordered discotic motif where the peripheral
organic ligands form a double calix housing the anions and solvent
molecules. From the formula and valence bond sums, the charge state
is mixed-valent, [Mn<sup>II</sup><sub>15</sub>Mn<sup>III</sup><sub>4</sub>]. Its magnetic properties and electrochemistry have been
studied. It behaves as a ferrimagnet below 40 K and has a coercive
field of 2.7 kOe at 1.8 K, which can be possible by either weak exchange
between clusters through the anions and solvents or through dipolar
interaction through space as confirmed by the lack of ordering in
frozen CH<sub>3</sub>CN. The moment of nearly 50 Nμ<sub>B</sub> suggests Mn<sup>II</sup>–Mn<sup>II</sup> and Mn<sup>III</sup>–Mn<sup>III</sup> are ferromagnetically coupled while Mn<sup>II</sup>–Mn<sup>III</sup> is antiferromagnetic which is likely
if the Mn<sup>III</sup> are centrally placed in the cluster. This
compound displays the rare occurrence of magnetic ordering from nonconnected
high-spin molecules
Pentagon-Fused Hollow Fullerene in C<sub>78</sub> Family Retrieved by Chlorination
C78 is one of the most widely investigated higher fullerenes. Among its huge isomer family, only one non-IPR (IPR = isolated pentagon ring) cage, the C2-symmetric #22010C78, was previously stabilized by endohedral derivatization. Here we report a new C1-symmetric non-IPR hollow isomer, #23863C78, which was captured as #23863C78Cl8 and then subjected to a regioselective substitution reaction with benzyl hydroperoxide to form #23863C78(OOCH2C6H5)Cl7. The structural connectivity of #23863C78, which contains a pair of fused pentagons, was confirmed by single-crystal X-ray diffraction analysis of the #23863C78(OOCH2C6H5)Cl7 molecule, which shares the same fullerene core with #23863C78Cl8; support for the structure is provided by comparable IR measurements and computation. Theoretical studies suggest that the differences in C−Cl bond length, intermediate stability, and steric effects of the involved molecules account for the chemical regioselectivity of the substitution reaction
Hierarchical Assembly of a {Mn<sup>II</sup><sub>15</sub>Mn<sup>III</sup><sub>4</sub>} Brucite Disc: Step-by-Step Formation and Ferrimagnetism
In
search of functional molecular materials and the study of their
formation mechanism, we report the elucidation of a hierarchical step-by-step
formation from monomer (Mn) to heptamer (Mn<sub>7</sub>) to nonadecamer
(Mn<sub>19</sub>) satisfying the relation 1 + Σ<sub><i>n</i></sub>6<i>n</i>, where <i>n</i> is
the ring number of the Brucite structure using high-resolution electrospray
ionization mass spectrometry (HRESI-MS). Three intermediate clusters,
Mn<sub>10</sub>, Mn<sub>12</sub>, and Mn<sub>14</sub>, were identified.
Furthermore, the Mn<sub>19</sub> disc remains intact when dissolved
in acetonitrile with a well-resolved general formula of [Mn<sub>19</sub>(<i>L</i>)<sub><i>x</i></sub>(OH)<sub><i>y</i></sub>(N<sub>3</sub>)<sub>36–<i>x</i>−<i>y</i></sub>]<sup>2+</sup> (<i>x</i> = 18, 17, 16; <i>y</i> = 8, 7, 6; H<i>L</i> = 1-(hydroxymethyl)-3,5-dimethylpyrazole) indicating progressive
exchange of N<sub>3</sub><sup>–</sup> for OH<sup>–</sup>. The high symmetry (<i>R</i>-3) Mn<sub>19</sub> crystal
structure consists of a well-ordered discotic motif where the peripheral
organic ligands form a double calix housing the anions and solvent
molecules. From the formula and valence bond sums, the charge state
is mixed-valent, [Mn<sup>II</sup><sub>15</sub>Mn<sup>III</sup><sub>4</sub>]. Its magnetic properties and electrochemistry have been
studied. It behaves as a ferrimagnet below 40 K and has a coercive
field of 2.7 kOe at 1.8 K, which can be possible by either weak exchange
between clusters through the anions and solvents or through dipolar
interaction through space as confirmed by the lack of ordering in
frozen CH<sub>3</sub>CN. The moment of nearly 50 Nμ<sub>B</sub> suggests Mn<sup>II</sup>–Mn<sup>II</sup> and Mn<sup>III</sup>–Mn<sup>III</sup> are ferromagnetically coupled while Mn<sup>II</sup>–Mn<sup>III</sup> is antiferromagnetic which is likely
if the Mn<sup>III</sup> are centrally placed in the cluster. This
compound displays the rare occurrence of magnetic ordering from nonconnected
high-spin molecules
