29 research outputs found
Langmuir Analysis of the Binding Affinity and Kinetics for Surface Tethered Duplex DNA and a LigandāApoprotein Complex
In
this work, the hybridization and dehybridization of ssDNA with
20 bases at gold coated sensor surfaces modified with complementary
20 bases capture probe ssDNA was investigated at 18 Ā°C by quartz
crystal microbalance measurements with dissipation monitoring (QCM-D).
A sequence of 20 base pairs with a melting temperature of about 64
Ā°C was chosen, since in many biosensor studies the target molecules
are DNA or RNA oligomers of similar length. It turned out that at
the applied experimental conditions the DNA hybridization was irreversible,
and therefore the hybridization and dehybridization process could
not be described by the Langmuir model of adsorption. Nevertheless,
quantitative dehybridization could be achieved by rinsing the sensor
surface thoroughly with pure water. When in contrast the hybridization
of a target with only 10 bases complementary to the outermost 10 bases
of the 20 bases capture probe was studied, binding and unbinding were
reversible, and the hybridization/dehybridization process could be
satisfactorily described by the Langmuir model. For the 10 base pair
sequence, the melting temperature was about 36 Ā°C. Apparently,
for Langmuir behavior, it is important that the experiments are applied
at a temperature sufficiently close to the melting temperature of
the sequence under investigation to ensure that at least traces of
the target molecules are unhybridized (i.e., there needs to be an
equilibrium between hybridized and dehybridized target molecules).
To validate the reliability of our experimental approach we also studied
the reconstitution and disassembly of the flavoprotein dodecin at
flavin-terminated DNA monolayers, as according to previous studies
it is assumed that the apododecināflavin system can be well
described by the Langmuir model. As a result, this assumption could
be verified. Using three different approaches, <i>K</i><sub>D</sub> values were obtained that differ not more than by a factor
of 4
Phase Relationships in the BaOāGa<sub>2</sub>O<sub>3</sub>āTa<sub>2</sub>O<sub>5</sub> System and the Structure of Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub>
Phase relationships in the BaOāGa<sub>2</sub>O<sub>3</sub>āTa<sub>2</sub>O<sub>5</sub> ternary system at 1200
Ā°C
were determined. The A<sub>6</sub>B<sub>10</sub>O<sub>30</sub> tetragonal
tungsten bronze (TTB) related solution in the BaOāTa<sub>2</sub>O<sub>5</sub> subsystem dissolved up to ā¼11 mol % Ga<sub>2</sub>O<sub>3</sub>, forming a ternary trapezoid-shaped TTB-related solid
solution region defined by the BaTa<sub>2</sub>O<sub>6</sub>, Ba<sub>1.1</sub>Ta<sub>5</sub>O<sub>13.6</sub>, Ba<sub>1.58</sub>Ga<sub>0.92</sub>Ta<sub>4.08</sub>O<sub>13.16</sub>, and Ba<sub>6</sub>GaTa<sub>9</sub>O<sub>30</sub> compositions in the BaOāGa<sub>2</sub>O<sub>3</sub>āTa<sub>2</sub>O<sub>5</sub> system. Two ternary
phases Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub> and eight-layer
twinned hexagonal perovskite solid solution Ba<sub>8</sub>Ga<sub>4ā<i>x</i></sub>Ta<sub>4+0.6<i>x</i></sub>O<sub>24</sub> were confirmed in the BaOāGa<sub>2</sub>O<sub>3</sub>āTa<sub>2</sub>O<sub>5</sub> system. Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub> crystallized in a monoclinic cell of <i>a</i> =
15.9130(2) Ć
, <i>b</i> = 11.7309(1) Ć
, <i>c</i> = 5.13593(6) Ć
, Ī² = 107.7893(9)Ā°, and <i>Z</i> = 1 in space group <i>C</i>2/<i>m</i>. The structure of Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub> was
solved by the charge flipping method, and it represents a three-dimensional
(3D) mixed GaO<sub>4</sub> tetrahedral and GaO<sub>6</sub>/TaO<sub>6</sub> octahedral framework, forming mixed 1D 5/6-fold tunnels that
accommodate the Ba cations along the <i>c</i> axis. The
electrical property of Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub> was characterized by using ac impedance spectroscopy
Molecular Beacon Modified Sensor Chips for Oligonucleotide Detection with Optical Readout
Three different surface bound molecular
beacons (MBs) were investigated
using surface plasmon fluorescence spectroscopy (SPFS) as an optical
readout technique. While MB1 and MB2, both consisting of 36 bases,
differed only in the length of the linker for surface attachment,
the significantly longer MB3, consisting of 56 bases, comprised an
entirely different sequence. For sensor chip preparation, the MBs
were chemisorbed on gold via thiol anchors together with different
thiol spacers. The influence of important parameters, such as the
length of the MBs, the length of the linker between the MBs and the
gold surface, the length and nature of the thiol spacers, and the
ratio between the MBs and the thiol spacers was studied. After hybridization
with the target, the fluorophore of the longer MB3 was oriented close
to the surface, and the shorter MBs were standing more or less upright,
leading to a larger increase in fluorescence intensity. Fluorescence
microscopy revealed a homogeneous distribution of the MBs on the surface.
The sensor chips could be used for simple and fast detection of target
molecules with a limit of detection in the larger picomolar range.
The response time was between 5 and 20 min. Furthermore, it was possible
to distinguish between fully complementary and singly mismatched targets.
While rinsing with buffer solution after hybridization with target
did not result in any signal decrease, complete dehybridization could
be carried out by intense rinsing with pure water. The MB modified
sensor chips could be prepared in a repeatable manner and reused many
times without significant decrease in performance
Studies of Terbium Bridge: Saturation Phenomenon, Significance of Sensitizer and Mechanisms of Energy Transfer, and Luminescence Quenching
Terbium chain in the form of S ā
(Tb<sup>3+</sup>)<sub><i>n</i></sub> ā A (S = Ce<sup>3+</sup> or Eu<sup>2+</sup>, A = Eu<sup>3+</sup>), as a promising
energy transfer (ET) approach,
has been proposed to enhance Eu<sup>3+</sup> emission for solid-state
lighting. However, the viewpoint of ET from S to A via the terbium
chain (Tb<sup>3+</sup>āTb<sup>3+</sup>āTb<sup>3+</sup>ā...) is very doubtful. Here, hosts of Ba<sub>3</sub>LnĀ(PO<sub>4</sub>)<sub>3</sub>, LnPO<sub>4</sub>, LnBO<sub>3</sub>, and Na<sub>2</sub>Ln<sub>2</sub>B<sub>2</sub>O<sub>7</sub> doped with Ce<sup>3+</sup> ā (Tb<sup>3+</sup>)<sub><i>n</i></sub> ā
Eu<sup>3+</sup> or (Tb<sup>3+</sup>)<sub><i>n</i></sub> ā
Eu<sup>3+</sup> are synthesized to prove the universality of S ā
(Tb<sup>3+</sup>)<sub><i>n</i></sub> ā A in inorganic
hosts and to study the unsolved issues. Saturation distance of Tb<sup>3+</sup>āEu<sup>3+</sup>, estimated with the empirical data
of different hosts, is proposed to be a criterion for determining
whether a spectral chromaticity coordinate keeps constant. A branch
model is put forward to replace the chain model to explain the role
of (Tb<sup>3+</sup>)<sub><i>n</i></sub> in ET from Ce<sup>3+</sup> to Eu<sup>3+</sup> and the necessity of high content of
Tb<sup>3+</sup>; the term āterbium bridgeā is used to
replace āterbium chainā, and the value of <i>n</i> is determined to be two or three. The intensity quenching of Eu<sup>3+</sup> emission is attributed to the surface defects ascribed to
the smaller particles and larger specific surface area rather than
the concentration quenching of Tb<sup>3+</sup>. Based on the saturation
distance and the mechanism of luminescence quenching, the necessary
concentration of Tb<sup>3+</sup> for (Tb<sup>3+</sup>)<sub><i>n</i></sub> can be estimated as long as the cell parameters
are already known and the luminescent efficiency of Eu<sup>3+</sup> can be further improved by optimizing the synthesis method to decrease
the quantity of surface defects
Phase Relationships in the BaOāGa<sub>2</sub>O<sub>3</sub>āTa<sub>2</sub>O<sub>5</sub> System and the Structure of Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub>
Phase relationships in the BaOāGa<sub>2</sub>O<sub>3</sub>āTa<sub>2</sub>O<sub>5</sub> ternary system at 1200
Ā°C
were determined. The A<sub>6</sub>B<sub>10</sub>O<sub>30</sub> tetragonal
tungsten bronze (TTB) related solution in the BaOāTa<sub>2</sub>O<sub>5</sub> subsystem dissolved up to ā¼11 mol % Ga<sub>2</sub>O<sub>3</sub>, forming a ternary trapezoid-shaped TTB-related solid
solution region defined by the BaTa<sub>2</sub>O<sub>6</sub>, Ba<sub>1.1</sub>Ta<sub>5</sub>O<sub>13.6</sub>, Ba<sub>1.58</sub>Ga<sub>0.92</sub>Ta<sub>4.08</sub>O<sub>13.16</sub>, and Ba<sub>6</sub>GaTa<sub>9</sub>O<sub>30</sub> compositions in the BaOāGa<sub>2</sub>O<sub>3</sub>āTa<sub>2</sub>O<sub>5</sub> system. Two ternary
phases Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub> and eight-layer
twinned hexagonal perovskite solid solution Ba<sub>8</sub>Ga<sub>4ā<i>x</i></sub>Ta<sub>4+0.6<i>x</i></sub>O<sub>24</sub> were confirmed in the BaOāGa<sub>2</sub>O<sub>3</sub>āTa<sub>2</sub>O<sub>5</sub> system. Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub> crystallized in a monoclinic cell of <i>a</i> =
15.9130(2) Ć
, <i>b</i> = 11.7309(1) Ć
, <i>c</i> = 5.13593(6) Ć
, Ī² = 107.7893(9)Ā°, and <i>Z</i> = 1 in space group <i>C</i>2/<i>m</i>. The structure of Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub> was
solved by the charge flipping method, and it represents a three-dimensional
(3D) mixed GaO<sub>4</sub> tetrahedral and GaO<sub>6</sub>/TaO<sub>6</sub> octahedral framework, forming mixed 1D 5/6-fold tunnels that
accommodate the Ba cations along the <i>c</i> axis. The
electrical property of Ba<sub>6</sub>Ga<sub>21</sub>TaO<sub>40</sub> was characterized by using ac impedance spectroscopy
Critical View on Electrochemical Impedance Spectroscopy Using the Ferri/Ferrocyanide Redox Couple at Gold Electrodes
Electrochemical or faradaic impedance
spectroscopy (EIS) using
the ferri/ferrocyanide couple as a redox probe at gold working electrodes
was evaluated with respect to its ability to monitor consecutive surface
modification steps. As a model reaction, the reversible hybridization
and dehybridization of DNA was studied. Thiol-modified single stranded
DNA (ssDNA, 20 bases, capture probe) was chemisorbed to a gold electrode
and treated with a solution of short thiols to release nonspecifically
adsorbed DNA before hybridization with complementary ssDNA (20 bases,
target) was carried out. Reversible dehybridization was achieved by
intense rinsing with pure water. The experimental procedures were
optimized by kinetic surface plasmon resonance (SPR) and quartz crystal
microbalance with dissipation (QCM-D) measurements to maximize the
increase in reflectivity or decrease in frequency upon hybridization
before hybridization/dehybridization was also monitored by EIS. In
contrast to SPR and QCM-D, repeatable EIS measurements were not possible
at first. Combined SPR/EIS and QCM-D/EIS measurements revealed that
during EIS the gold surface is seriously damaged due to the presence
of CN<sup>ā</sup> ions, which are released from the ferri/ferrocyanide
redox probe. Even at optimized experimental conditions, etching the
gold electrodes could not be completely suppressed and the repeatability
of the EIS measurements was limited. In three out of four experimental
runs, only two hybridization/dehybridization steps could be monitored
reversibly by EIS. Thereafter etching the gold electrode significantly
contributed to the EIS spectra whereas the QCM-D response was still
repeatable. Hence great care has to be taken when this technique is
used to monitor surface modification at gold electrodes
Multi-Ligand-Binding Flavoprotein Dodecin as a Key Element for Reversible Surface Modification in Nano-biotechnology
In this paper the multiple (re)programming of proteināDNA nanostructures comprising generation, deletion, and reprogramming on the same flavin-DNA-modified surface is introduced. This work is based on a systematic study of the binding affinity of the multi-ligand-binding flavoprotein dodecin on flavin-terminated DNA monolayers by surface plasmon resonance and quartz crystal microbalance with dissipation (QCM-D) measurements, surface plasmon fluorescence spectroscopy (SPFS), and dynamic AFM force spectroscopy. Depending on the flavin surface coverage, a single apododecin is captured by one or more surface-immobilized flavins. The corresponding complex binding and unbinding rate constants <i>k</i><sub>on(QCM)</sub> = 7.7 Ć 10<sup>3</sup> M<sup>ā1</sup>Ā·s<sup>ā1</sup> and <i>k</i><sub>off(QCM)</sub> = 4.5 Ć 10<sup>ā3</sup> s<sup>ā1</sup> (<i>K</i><sub>d(QCM)</sub> = 580 nM) were determined by QCM and were found to be in agreement with values for <i>k</i><sub>off</sub> determined by SPFS and force spectroscopy. Even though a single apododecināflavin bond is relatively weak, stable dodecin monolayers were formed on flavin-DNA-modified surfaces at high flavin surface coverage due to multivalent interactions between apododecin bearing six binding pockets and the surface-bound flavin-DNA ligands. If bi- or multivalent flavin ligands are adsorbed on dodecin monolayers, stable sandwich-type surface-DNA-flavin-apododecin-flavin ligand arrays are obtained. Nevertheless, the apododecin flavin complex is easily and quantitatively disassembled by flavin reduction. Binding and release of apododecin are reversible processes, which can be carried out alternatingly several times to release one type of ligand by an external redox trigger and subsequently replace it with a different ligand. Hence the versatile concept of reprogrammable functional biointerfaces with the multi-ligand-binding flavoprotein dodecin is demonstrated
Enhancing the Performance of Quantum-Dot Light-Emitting Diodes by Postmetallization Annealing
The
effect of postannealing on the device characteristics is systematically
investigated. The external quantum efficiency (EQE) of blue quantum-dot
light-emitting diodes (QLEDs) is significantly improved from 5.22
to 9.81% after postannealing. Similar results are obtained in green
and red QLEDs, whose EQEs are enhanced from 11.47 and 13.60 to 15.57
and 16.59%, respectively. The annealed devices also exhibit a larger
current density. The origin of efficiency improvement is thoroughly
investigated. Our finding indicates that postannealing promotes the
interfacial reaction of Al and ZnMgO and consequently leads to the
metallization of the AlZnMgO contact and the formation of the AlO<sub><i>x</i></sub> interlayer. Because of the metallization
of AlZnMgO, the contact resistance is effectively reduced, and thus
the electron injection is enhanced. On the other hand, the formation
of the AlO<sub><i>x</i></sub> interlayer can effectively
suppress the quenching of excitons by the metal electrode. Because
of the enhancement of electron injection and suppression of exciton
quenching, the annealed blue, green, and red QLEDs exhibit a 1.9-,
a 1.3-, and a 1.2-fold efficiency improvement, respectively. We envision
the results offer a simple yet effective method to enhance the charge
injection and the efficiency of QLED devices, which would promote
the practical application of QLEDs
Multifunctional Silicon Optoelectronics Integrated with Plasmonic Scattering Color
Plasmonic
scattering from metallic nanoparticles has been used
for centuries to create the colorful appearance of stained glass.
Besides their use as passive spectral filtering components, multifunctional
optoelectronic applications can be achieved by integrating the nanoscatters
with semiconductors that generate electricity using the complementary
spectral components of plasmonic colors. To suppress the usual degradation
of both efficiency and the gamut of plasmonic scattering coloration
in highly asymmetric index configurations like a silicon host, aluminum
nanodisks on indium tin oxide (ITO) coated silicon were experimentally
studied and demonstrated color sorting in the full visible range along
with photocurrent generation. Interestingly, the photocurrents were
found to be comparable to the reference devices with only antireflection
coatings in spite of the power loss for coloration. Detailed investigation
shows that ITO serves as both the impedance matching layer for promoting
the backward scattering and schottky contact with silicon, and moreover,
plasmonic nanoscatters efficiently harvest the complement spectrum
components for charge generation. The present approach combines the
capacities of nanoscale color sorting and photoelectric converting
at a negligible cost of efficiency, thus providing a broad flexibility
of being utilized in various optoelectronic applications including
self-powered display, filter-free imaging, and colorful photovoltaics
Highly Thermally Stable Single-Component White-Emitting Silicate Glass for Organic-Resin-Free White-Light-Emitting Diodes
Thermal management is still a great challenge for high-power phosphor-converted white-light-emitting diodes (pc-WLEDs) intended for future general lighting. In this paper, a series of single-component white-emitting silicate SiO<sub>2</sub>āLi<sub>2</sub>OāSrOāAl<sub>2</sub>O<sub>3</sub>āK<sub>2</sub>OāP<sub>2</sub>O<sub>5</sub>: Ce<sup>3+</sup>, Tb<sup>3+</sup>, Mn<sup>2+</sup> (SLSAKP: Ce<sup>3+</sup>, Tb<sup>3+</sup>, Mn<sup>2+</sup>) glasses that simultaneously play key roles as a luminescent convertor and an encapsulating material for WLEDs were prepared via the conventional melt-quenching method, and systematically studied using their absorption spectra, transmittance spectra, photoluminescence excitation and emission spectra in the temperature range 296ā498 K, decay curves, and quantum efficiency. The glasses show strong and broad absorption in 250ā380 nm region and exhibit intense white emission, produced by in situ mixing of blue-violet, green, and orange-red light from Ce<sup>3+</sup>, Tb<sup>3+</sup>, and Mn<sup>2+</sup> ions, respectively, in a single glass component. The quantum efficiency of SLSAKP: 0.3%Ce<sup>3+</sup>, 2.0%Tb<sup>3+</sup>, 2.0%Mn<sup>2+</sup> glass is determined to be 19%. More importantly, this glass shows good thermal stability, exhibiting at 373 and 423 K about 84.56 and 71.02%, respectively, of the observed room temperature (298 K) emission intensity. The chromaticity shift of SLSAKP: 0.3%Ce<sup>3+</sup>, 2.0%Tb<sup>3+</sup>, 2.0%Mn<sup>2+</sup> is 2.94 Ć 10<sup>ā2</sup> at 498 K, only 57% of the commercial triple-color white-emitting phosphor mixture. Additionally, this glass shows no transmittance loss at the 370 nm emission of a UV-Chip-On-Board (UV-COB) after thermal aging for 240 h, compared with the 82% transmittance loss of epoxy resin. The thermal conductivity of the glass is about 1.07 W/mK, much larger than the 0.17 W/mK of epoxy resin. An organic-resin-free WLEDs device based on SLSAKP: 0.3%Ce<sup>3+</sup>, 2.0%Tb<sup>3+</sup>, 2.0%Mn<sup>2+</sup> glass and UV-COB is successfully demonstrated. All of our results demonstrate that the presented Ce<sup>3+</sup>/Tb<sup>3+</sup>/Mn<sup>2+</sup> tridoped lithiumāstrontiumāsilicate glass may serve as a promising candidate for high-power WLEDs