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T Oligo-Primed Polymerase Chain Reaction (TOP-PCR): A Robust Method for the Amplification of Minute DNA Fragments in Body Fluids.
Body fluid DNA sequencing is a powerful noninvasive approach for the diagnosis of genetic defects, infectious agents and diseases. The success relies on the quantity and quality of the DNA samples. However, numerous clinical samples are either at low quantity or of poor quality due to various reasons. To overcome these problems, we have developed T oligo-primed polymerase chain reaction (TOP-PCR) for full-length nonselective amplification of minute quantity of DNA fragments. TOP-PCR adopts homogeneous "half adaptor" (HA), generated by annealing P oligo (carrying a phosphate group at the 5' end) and T oligo (carrying a T-tail at the 3' end), for efficient ligation to target DNA and subsequent PCR amplification primed by the T oligo alone. Using DNA samples from body fluids, we demonstrate that TOP-PCR recovers minute DNA fragments and maintains the DNA size profile, while enhancing the major molecular populations. Our results also showed that TOP-PCR is a superior method for detecting apoptosis and outperforms the method adopted by Illumina for DNA amplification
Determining layer number of two dimensional flakes of transition-metal dichalcogenides by the Raman intensity from substrate
Transition-metal dichalcogenide (TMD) semiconductors have been widely studied
due to their distinctive electronic and optical properties. The property of TMD
flakes is a function of its thickness, or layer number (N). How to determine N
of ultrathin TMDs materials is of primary importance for fundamental study and
practical applications. Raman mode intensity from substrates has been used to
identify N of intrinsic and defective multilayer graphenes up to N=100.
However, such analysis is not applicable for ultrathin TMD flakes due to the
lack of a unified complex refractive index () from monolayer to bulk
TMDs. Here, we discuss the N identification of TMD flakes on the SiO/Si
substrate by the intensity ratio between the Si peak from 100-nm (or 89-nm)
SiO/Si substrates underneath TMD flakes and that from bare SiO/Si
substrates. We assume the real part of of TMD flakes as that of
monolayer TMD and treat the imaginary part of as a fitting
parameter to fit the experimental intensity ratio. An empirical ,
namely, , of ultrathin MoS, WS and WSe
flakes from monolayer to multilayer is obtained for typical laser excitations
(2.54 eV, 2.34 eV, or 2.09 eV). The fitted of MoS has
been used to identify N of MoS flakes deposited on 302-nm SiO/Si
substrate, which agrees well with that determined from their shear and
layer-breathing modes. This technique by measuring Raman intensity from the
substrate can be extended to identify N of ultrathin 2D flakes with N-dependent
. For the application purpose, the intensity ratio excited by
specific laser excitations has been provided for MoS, WS and
WSe flakes and multilayer graphene flakes deposited on Si substrates
covered by 80-110 nm or 280-310 nm SiO layer.Comment: 10 pages, 4 figures. Accepted by Nanotechnolog
Antiferromagnetism and hole pair checkerboard in the vortex state of high Tc superconductors
We propose a microscopic state for the vortex phase of BSCO superconductors.
Around the vortex core or above H_{c2}, the d wave hole pairs form a
checkerboard localized in the commensurate antiferromagnetic background. We
discuss this theory in connection with recent STM experiments.Comment: Final versio
Probing the Electron States and Metal-Insulator Transition Mechanisms in Atomically Thin MoS2 Based on Vertical Heterostructures
The metal-insulator transition (MIT) is one of the remarkable electrical
transport properties of atomically thin molybdenum disulphide (MoS2). Although
the theory of electron-electron interactions has been used in modeling the MIT
phenomena in MoS2, the underlying mechanism and detailed MIT process still
remain largely unexplored. Here, we demonstrate that the vertical
metal-insulator-semiconductor (MIS) heterostructures built from atomically thin
MoS2 (monolayers and multilayers) are ideal capacitor structures for probing
the electron states in MoS2. The vertical configuration of MIS heterostructures
offers the added advantage of eliminating the influence of large impedance at
the band tails and allows the observation of fully excited electron states near
the surface of MoS2 over a wide excitation frequency (100 Hz-1 MHz) and
temperature range (2 K- 300 K). By combining capacitance and transport
measurements, we have observed a percolation-type MIT, driven by density
inhomogeneities of electron states, in the vertical heterostructures built from
monolayer and multilayer MoS2. In addition, the valence band of thin MoS2
layers and their intrinsic properties such as thickness-dependence screening
abilities and band gap widths can be easily accessed and precisely determined
through the vertical heterostructures
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