N7-methylguanosine (m7G) is one of the most common post-transcriptional epigenetic modifications. Different m7G methyltransferases (writers) load the m7G-cap at the 5'-terminal or inside the RNAs. For example, writers such as methyltransferase-like 1 (METTL1)/WD repeat domain 4 (WDR4) and Williams-Beuren syndrome chromosome region 22 (WBSCR22) have been reported in mammals to promote cell proliferation, EMT, and chemoresistance in massive quantities of cancers. The underlying mechanism includes modulating the RNA secondary structure, preventing RNA degradation from exonucleases, and improving codon-dependent translation. However, some studies have shown that in colorectal and lung cancers, m7G inhibits tumor progression. m7G binding proteins (readers), such as eukaryotic translation initiation factor 4E (eIF4E), promote the efficiency of cap-dependent translation and accelerate the cell cycle to improve cancer progression. Due to the more profound understanding of m7G regulatory proteins in cancer, numerous studies aim to investigate the clinical efficiency of m7G-targeted therapy. eIF4E antisense oligonucleotide drug (4EASO) and Ribavirin are the most mature trials that competitively inhibit the binding of eIF4E to m7G-cap. These drugs have encouraging results in halting cancer progression and improving prognosis, including AML and non-small cell lung cancer, which provide a promising perspective for developing more m7G-targeted drugs. In the future, we look forward to an ongoing investigation into the role of m7G modification in tumors and drug resistance to m7G-related therapies to be solved. Therefore, the clinical application would be put into practice as soon as possible.
Dielectric materials with a very low dielectric constant, k, will be required to overcome problems such as cross-talk and propagation delay in future generations of microprocessors, whose features are becoming increasingly smaller. Here pure-silica zeolite is examined as an alternative low-k material. Thin films prepared by in-situ crystallization (see Figure) and a spin-on process are compared.
In this article, an introduction is presented about the energy harvesting technologies that have potential for powering nanosystems. Our discussion mainly focuses on the approaches other than the well-known solar cell and thermoelectrics. We mainly introduce the piezoelectric nanogenerators developed using aligned ZnO nanowire arrays. This is a potential technology for converting mechanical movement energy (such as body movement, muscle stretching, blood pressure), vibration energy (such as acoustic/ultrasonic wave), and hydraulic energy (such as fl ow of body fl uid, blood fl ow, contraction of blood vessel, dynamic fl uid in nature) into electric energy for self-powered nanosystems.
Abstract The differential form of the Maxwell’s equations was first derived based on an assumption that the media are stationary, which is the foundation for describing the electro-magnetic coupling behavior of a system. For a general case in which the medium has a time-dependent volume, shape and boundary and may move at an arbitrary velocity field <?CDATA ${\boldsymbol{v}}({\boldsymbol{r}},{t})$?> <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="bold-italic">v</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mi mathvariant="bold-italic">r</mml:mi> <mml:mo>,</mml:mo> <mml:mi mathvariant="italic"> t</mml:mi> <mml:mo stretchy="false">)</mml:mo> </mml:math> and along a general trajectory, we derived the Maxwell’s equations for a mechano-driven slow-moving media system directly starting from the integral forms of four physics laws, which should be accurate enough for describing the coupling among mechano-electro-magnetic interactions of a general system in practice although it may not be Lorentz covarance. Our key point is directly from the four physics laws by describing all of the fields, the space and the time in the frame where the observation is done. The equations should be applicable to not only moving charged solid and soft media that has acceleration, but also charged fluid/liquid media, e.g., fluid electrodynamics. This is a step toward the electrodynamics in non-inertia frame of references. General strategies for solving the Maxwell’s equations for mechano-driven slowing moving medium are presented using the perturbation theory both in time and frequency spaces. Finally, approaches for the electrodynamics of moving media are compared, and related discussions are given about a few interesting questions.