10 research outputs found
<i>M</i>‑State and <i>N</i>‑Color (<i>M</i>–<i>N</i> = 1–1, 2–1, and 1–2) Turing Algorithms Demonstrated via DNA Self-Assembly
The fast and extensive
generation of patterns using specific algorithms
is a major challenge in the field of DNA algorithmic self-assembly.
Turing machines (TMs) are simple computable machines that execute
certain algorithms using carefully designed logic gates. We investigate
Turing algorithms for the generation of patterns on algorithmic lattices
using specific logic gates. Logic gates can be implemented into Turing
building blocks. We discuss comprehensive methods for designing Turing
building blocks to demonstrate an M-state and N-color Turing machine (M–N TM). The M-state and N-color (M–N = 1–1,
2–1, and 1–2) TMs generate Turing patterns that can
be fabricated via DNA algorithmic self-assembly. The M–N TMs require two-input and three-output
logic gates. We designed the head, tape, and transition rule tiles
to demonstrate TMs for the 1–1, 2–1, and 1–2
Turing algorithms. By analyzing the characteristics of the Turing
patterns, we classified them into two classes (DL and DR for states
grown diagonally to the left and right, respectively) for the 1–1
TM, three for the 2–1 TM, and nine for the 1–2 TM. Among
these, six representative Turing patterns generated using rules R11-0
and R11-1 for 1–1 TM, R21-01 and R21-09 for 2–1 TM,
and R12-02 and R12-08 for 1–2 TM were constructed with DNA
building blocks. Turing patterns on the DNA lattices were visualized
by atomic force microscopy. The Turing patterns on the DNA lattices
were similar to those simulated patterns. Implementing the Turing
algorithms into DNA building blocks, as demonstrated via DNA algorithmic
self-assembly, can be extended to a higher order of state and color
to generate more complicated patterns, compute arithmetic operations,
and solve mathematical functions
3‑Input/1-Output Logic Implementation Demonstrated by DNA Algorithmic Self-Assembly
Although
structural DNA nanotechnology is a well-established field,
computations performed using DNA algorithmic self-assembly is still
in the primitive stages in terms of its adaptability of rule implementation
and experimental complexity. Here, we discuss the feasibility of constructing
an <i>M</i>-input/<i>N</i>-output logic gate implemented
into simple DNA building blocks. To date, no experimental demonstrations
have been reported with <i>M</i> > 2 owing to the difficulty
of tile design. To overcome this problem, we introduce a special tile
referred to as an operator. We design appropriate binding domains
in DNA tiles, and we demonstrate the growth of DNA algorithmic lattices
generated by eight different rules from among 256 rules in a 3-input/1-output
logic. The DNA lattices show simple, linelike, random, and mixed patterns,
which we analyze to obtain errors and sorting factors. The errors
vary from 0.8% to 12.8% depending upon the pattern complexity, and
sorting factors obtained from the experiment are in good agreement
with simulation results within a range of 1–18%
Morphological and Optoelectronic Characteristics of Double and Triple Lanthanide Ion-Doped DNA Thin Films
Double and triple lanthanide ion
(Ln<sup>3+</sup>)-doped synthetic
double crossover (DX) DNA lattices and natural salmon DNA (SDNA) thin
films are fabricated by the substrate assisted growth and drop-casting
methods on given substrates. We employed three combinations of double
Ln<sup>3+</sup>-dopant pairs (Tb<sup>3+</sup>–Tm<sup>3+</sup>, Tb<sup>3+</sup>–Eu<sup>3+</sup>, and Tm<sup>3+</sup>–Eu<sup>3+</sup>) and a triple Ln<sup>3+</sup>-dopant pair (Tb<sup>3+</sup>–Tm<sup>3+</sup>–Eu<sup>3+</sup>) with different types
of Ln<sup>3+</sup>, (i.e., Tb<sup>3+</sup> chosen for green emission,
Tm<sup>3+</sup> for blue, and Eu<sup>3+</sup> for red), as well as
various concentrations of Ln<sup>3+</sup> for enhancement of specific
functionalities. We estimate the optimum concentration of Ln<sup>3+</sup> ([Ln<sup>3+</sup>]<sub>O</sub>) wherein the phase transition of
Ln<sup>3+</sup>-doped DX DNA lattices occurs from crystalline to amorphous.
The phase change of DX DNA lattices at [Ln<sup>3+</sup>]<sub>O</sub> and a phase diagram controlled by combinations of [Ln<sup>3+</sup>] were verified by atomic force microscope measurement. We also developed
a theoretical method to obtain a phase diagram by identifying a simple
relationship between [Ln<sup>3+</sup>] and [Ln<sup>3+</sup>]<sub>O</sub> that in practice was found to be in agreement with experimental
results. Finally, we address significance of physical characteristicsî—¸current
for evaluating [Ln<sup>3+</sup>]<sub>O</sub>, absorption for understanding
the modes of Ln<sup>3+</sup> binding, and photoluminescence for studying
energy transfer mechanismsî—¸of double and triple Ln<sup>3+</sup>-doped SDNA thin films. Current and photoluminescence in the visible
region increased as the varying [Ln<sup>3+</sup>] increased up to
a certain [Ln<sup>3+</sup>]<sub>O</sub>, then decreased with further
increases in [Ln<sup>3+</sup>]. In contrast, the absorbance peak intensity
at 260 nm showed the opposite trend, as compared with current and
photoluminescence behaviors as a function of varying [Ln<sup>3+</sup>]. A DNA thin film with varying combinations of [Ln<sup>3+</sup>]
might provide immense potential for the development of efficient devices
or sensors with increasingly complex functionality
Multidimensional Honeycomb-like DNA Nanostructures Made of C‑Motifs
Thanks to its remarkable properties of self-assembly
and molecular
recognition, DNA can be used in the construction of various dimensional
nanostructures to serve as templates for decorating nanomaterials
with nanometer-scale precision. Accordingly, this study discusses
a design strategy for fabricating such multidimensional DNA nanostructures
made of simple C-motifs. One-dimensional (1D) honeycomb-like tubes
(1HTs) and two-dimensional (2D) honeycomb-like lattices (2HLs) were
constructed using a C-motif with an arm length of 14 nucleotides (nt)
at an angle of 240° along the counterclockwise direction. We
designed and fabricated four different types of 1HTs and three different
2HLs. The study used atomic force microscopy to characterize the distinct
topologies of the 1D and 2D DNA nanostructures (i.e., 1HTs and 2HLs,
respectively). The width deviation of the 1HTs and height suppression
percentage of the 2HLs were calculated and discussed. Our study can
be provided to construct various dimensional DNA nanostructures easily
with high efficiency
n- and p‑Type Doping Phenomenon by Artificial DNA and M‑DNA on Two-Dimensional Transition Metal Dichalcogenides
Deoxyribonucleic acid (DNA) and two-dimensional (2D) transition metal dichalcogenide (TMD) nanotechnology holds great potential for the development of extremely small devices with increasingly complex functionality. However, most current research related to DNA is limited to crystal growth and synthesis. In addition, since controllable doping methods like ion implantation can cause fatal crystal damage to 2D TMD materials, it is very hard to achieve a low-level doping concentration (nondegenerate regime) on TMD in the present state of technology. Here, we report a nondegenerate doping phenomenon for TMD materials (MoS<sub>2</sub> and WSe<sub>2</sub>, which represent n- and p-channel materials, respectively) using DNA and slightly modified DNA by metal ions (Zn<sup>2+</sup>, Ni<sup>2+</sup>, Co<sup>2+</sup>, and Cu<sup>2+</sup>), named as M-DNA. This study is an example of interdisciplinary convergence research between DNA nanotechnology and TMD-based 2D device technology. The phosphate backbone (PO<sub>4</sub><sup>–</sup>) in DNA attracts and holds hole carriers in the TMD region, n-doping the TMD films. Conversely, M-DNA nanostructures, which are functionalized by intercalating metal ions, have positive dipole moments and consequently reduce the electron carrier density of TMD materials, resulting in p-doping phenomenon. N-doping by DNA occurs at ∼6.4 × 10<sup>10</sup> cm<sup>–2</sup> on MoS<sub>2</sub> and ∼7.3 × 10<sup>9</sup> cm<sup>–2</sup> on WSe<sub>2</sub>, which is uniform across the TMD area. p-Doping which is uniformly achieved by M-DNA occurs between 2.3 × 10<sup>10</sup> and 5.5 × 10<sup>10</sup> cm<sup>–2</sup> on MoS<sub>2</sub> and between 2.4 × 10<sup>10</sup> and 5.0 × 10<sup>10</sup> cm<sup>–2</sup> on WSe<sub>2</sub>. These doping levels are in the nondegenerate regime, allowing for the proper design of performance parameters of TMD-based electronic and optoelectronic devices (<i>V</i><sub>TH</sub>, on-/off-currents, field-effect mobility, photoresponsivity, and detectivity). In addition, by controlling the metal ions used, the p-doping level of TMD materials, which also influences their performance parameters, can be controlled. This interdisciplinary convergence research will allow for the successful integration of future layered semiconductor devices requiring extremely small and very complicated structures
Energy Band Gap and Optical Transition of Metal Ion Modified Double Crossover DNA Lattices
We report on the energy band gap
and optical transition of a series of divalent metal ion (Cu<sup>2+</sup>, Ni<sup>2+</sup>, Zn<sup>2+</sup>, and Co<sup>2+</sup>) modified
DNA (M–DNA) double crossover (DX) lattices fabricated on fused
silica by the substrate-assisted growth (SAG) method. We demonstrate
how the degree of coverage of the DX lattices is influenced by the
DX monomer concentration and also analyze the band gaps of the M–DNA
lattices. The energy band gap of the M–DNA, between the lowest
unoccupied molecular orbital (LUMO) and the highest occupied molecular
orbital (HOMO), ranges from 4.67 to 4.98 eV as judged by optical transitions.
Relative to the band gap of a pristine DNA molecule (4.69 eV), the
band gap of the M–DNA lattices increases with metal ion doping
up to a critical concentration and then decreases with further doping.
Interestingly, except for the case of Ni<sup>2+</sup>, the onset of
the second absorption band shifts to a lower energy until a critical
concentration and then shifts to a higher energy with further increasing
the metal ion concentration, which is consistent with the evolution
of electrical transport characteristics. Our results show that controllable
metal ion doping is an effective method to tune the band gap energy
of DNA-based nanostructures
A 2D DNA Lattice as an Ultrasensitive Detector for Beta Radiations
There is growing demand for the development of efficient ultrasensitive radiation detectors to monitor the doses administered to individuals during therapeutic nuclear medicine which is often based on radiopharmaceuticals, especially those involving beta emitters. Recently biological materials are used in sensors in the nanobio disciplines due to their abilities to detect specific target materials or sites. Artificially designed two-dimensional (2D) DNA lattices grown on a substrate were analyzed after exposure to pure beta emitters, <sup>90</sup>Sr-<sup>90</sup>Y. We studied the Raman spectra and reflected intensities of DNA lattices at various distances from the source with different exposure times. Although beta particles have very low linear energy transfer values, the significant physical and chemical changes observed throughout the extremely thin, ∼0.6 nm, DNA lattices suggested the feasibility of using them to develop ultrasensitive detectors of beta radiations
Combining Protein-Shelled Platinum Nanoparticles with Graphene to Build a Bionanohybrid Capacitor
The electronic properties of biomolecules and their hybrids with inorganic materials can be utilized for the fabrication of nanoelectronic devices. Here, we report the charge transport behavior of protein-shelled inorganic nanoparticles combined with graphene and demonstrate their possible application as a bionanohybrid capacitor. The conductivity of PepA, a bacterial aminopeptidase used as a protein shell (PS), and the platinum nanoparticles (PtNPs) encapsulated by PepA was measured using a field effect transistor (FET) and a graphene-based FET (GFET). Furthermore, we confirmed that the electronic properties of PepA-PtNPs were controlled by varying the size of the PtNPs. The use of two poly(methyl methacrylate) (PMMA)-coated graphene layers separated by PepA-PtNPs enabled us to build a bionanohybrid capacitor with tunable properties. The combination of bioinorganic nanohybrids with graphene is regarded as the cornerstone for developing flexible and biocompatible bionanoelectronic devices that can be integrated into bioelectric circuits for biomedical purposes
Long dsRNA-Mediated RNA Interference and Immunostimulation: A Targeted Delivery Approach Using Polyethyleneimine Based Nano-Carriers
RNA
oligonucleotides capable of inducing controlled immunostimulation
combined with specific oncogene silencing via an RNA interference
(RNAi) mechanism provide synergistic inhibition of cancer cell growth.
With this concept, we previously designed a potent immunostimulatory
long double stranded RNA, referred to as liRNA, capable of executing
RNAi mediated specific target gene silencing. In this study, we developed
a highly effective liRNA based targeted delivery system to apply in
the treatment of glioblastoma multiforme. A stable nanocomplex was
fabricated by complexing multimerized liRNA structures with cross-linked
branched polyÂ(ethylene imine) (bPEI) via electrostatic interactions.
We show clear evidence that the cross-linked bPEI was quite effective
in enhancing the cellular uptake of liRNA on U87MG cells. Moreover,
the liRNA-PEI nanocomplex provided strong RNAi mediated target gene
silencing compared to that of the conventional siRNA-PEI complex.
Further, the bPEI modification strategy with specific ligand attachment
assisted the uptake of the liRNA-PEI complex on the mouse brain endothelial
cell line (b.End3). Such delivery systems combining the beneficial
elements of targeted delivery, controlled immunostimulation, and RNAi
mediated target silencing have immense potential in anticancer therapy
Nature-Inspired Construction of Two-Dimensionally Self-Assembled Peptide on Pristine Graphene
Peptide assemblies
have received significant attention because
of their important role in biology and applications in bionanotechnology.
Despite recent efforts to elucidate the principles of peptide self-assembly
for developing novel functional devices, peptide self-assembly on
two-dimensional nanomaterials has remained challenging. Here, we report
nature-inspired two-dimensional peptide self-assembly on pristine
graphene via optimization of peptide–peptide and peptide–graphene
interactions. Two-dimensional peptide self-assembly was designed based
on statistical analyses of >10<sup>4</sup> protein structures existing
in nature and atomistic simulation-based structure predictions. We
characterized the structures and surface properties of the self-assembled
peptide formed on pristine graphene. Our study provides insights into
the formation of peptide assemblies coupled with two-dimensional nanomaterials
for further development of nanobiocomposite devices