15 research outputs found
Two-Dimensional Transceiver Beamforming for Mainlobe Jamming Suppression with FDA-MIMO Radar
With the rapid development of electronic warfare technology, the airborne electronic counter measures (ECM) system can generate mainlobe jamming using range gate pull-off (RGPO) strategy, which brings serious performance degradation of target tracking for the tracking and guidance radar. In this study, a two-dimensional transceiver beamforming approach is proposed to suppress the mainlobe jamming with frequency diverse array using multiple-input multiple-output (FDA-MIMO) radar. The mainlobe jamming signal differs from the real target echo in the joint transmit and receive domain due to the range dependence of FDA beampattern. The amplitude of RGPO signal is greater than the amplitude of real target echo. Thus, the transceiver beampattern can be designed to null out the jamming while maintaining the real target. The jamming suppression performance is studied in consideration of practical range constraint of RGPO. Simulation results are provided to verify the effectiveness of the proposed approach
The Spatially Separated Polarization Sensitive FDA-MIMO Radar: A New Antenna Structure for Unambiguous Parameter Estimation
Joint DOA-range-polarization estimation with a novel radar system, i.e., spatially separated polarization sensitive random frequency diverse array based on multiple-input multiple-output (SS-PSRFDA-MIMO) radar, is discussed. The proposed array can obtain not only unambiguous range estimation but also polarization parameter estimation. Firstly, the signal model of SS-PSRFDA-MIMO radar is constructed. Secondly, dimension reduction multiple signal classification (DR-MUSIC) algorithm is extended to parameter estimation with the proposed array. Last, simulations demonstrate the proposed algorithm is effective to estimate parameter, and the performance of proposed array is better than that of polarization sensitive frequency diverse array based on MIMO radar. It is worth mentioning that the Cramér–Rao lower bound (CRLB) of range estimation with the proposed array is much lower than that of PSFDA-MIMO radar
Raman Spectral and Density Functional Theory Analyses of the CsB<sub>3</sub>O<sub>5</sub> Melt Structure
Melt
structures are essential to understand a variety of crystal growth
phenomena of alkali-metal triborates, but have not been fully explored.
In this work, Raman spectroscopy, coupled with the density functional
theory (DFT) method, has been used to solve the CsB<sub>3</sub>O<sub>5</sub> (CBO) melt structure. When the CBO crystal melts, the extra-ring
B<sub>4</sub>–Ø bonds (the B–Ø bonds of BØ<sub>4</sub> groups, Ø = bridging oxygen atom) that connect two B<sub>3</sub>O<sub>3</sub>Ø<sub>4</sub> rings (the basic boron–oxygen
unit in the CBO crystal structure) break. As a result, the three-dimensional
boron–oxygen network collapses to unique polymer-like [B<sub>3</sub>O<sub>4</sub>Ø<sub>2</sub>]<sub><i>n</i></sub> chains. On the basis of the optimized [B<sub>3</sub>O<sub>4</sub>Ø<sub>2</sub>]<sub><i>n</i></sub> chain model, the
CBO melt Raman spectrum was calculated by the DFT method for the first
time and the calculated results confirm that the [B<sub>3</sub>O<sub>4</sub>Ø<sub>2</sub>]<sub><i>n</i></sub> chain is
the primary species in the CBO melt. These results also demonstrate
the capability of the combined Raman spectral and DFT method for analyzing
borate melt structures
Raman and Density Functional Theory Studies of Li<sub>2</sub>Mo<sub>4</sub>O<sub>13</sub> Structures in Crystalline and Molten States
The Li<sub>2</sub>Mo<sub>4</sub>O<sub>13</sub> melt structure and its Raman spectral
characteristics are the key for establishing the composition–structure
relationship of lithium molybdate melts. In this work, Raman spectroscopy,
factor group analysis, and density functional theory (DFT) were applied
to investigate the structural and spectral details of the <i>H</i>-Li<sub>2</sub>Mo<sub>4</sub>O<sub>13</sub> crystal and
a Li<sub>2</sub>Mo<sub>4</sub>O<sub>13</sub> melt. Factor group analysis
shows that the crystal has 171 vibrational modes (84A<sub>g</sub> +
87A<sub>u</sub>), including three acoustic modes (3A<sub>u</sub>),
six librational modes (2A<sub>g</sub> + 4A<sub>u</sub>), 21 translational
modes (7A<sub>g</sub> + 14A<sub>u</sub>), and 141 internal modes (75A<sub>g</sub> + 66A<sub>u</sub>). All of the A<sub>g</sub> modes are Raman-active
and were assigned by the DFT method. The Li<sub>2</sub>Mo<sub>4</sub>O<sub>13</sub> melt structure was deduced from the <i>H</i>-Li<sub>2</sub>Mo<sub>4</sub>O<sub>13</sub> crystal structure and
demonstrated by the DFT method. The results show that the Li<sub>2</sub>Mo<sub>4</sub>O<sub>13</sub> melt is made up of Li<sup>+</sup> ions
and Mo<sub>4</sub>O<sub>13</sub><sup>2–</sup> groups, each
of which is formed by four corner-sharing MoO<sub>3</sub>Ø/MoO<sub>2</sub>Ø<sub>2</sub> tetrahedra (Ø = bridging oxygen).
The melt has three acoustic modes (3A) and 54 optical modes (54A).
All of the optical modes are Raman-active and were accurately assigned
by the DFT method
Investigation on the Structure of a LiB<sub>3</sub>O<sub>5</sub>–Li<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub> High-Temperature Solution for Understanding the Li<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub> Flux Behavior
LiB<sub>3</sub>O<sub>5</sub> is the most widely used nonlinear optical crystal. Li<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub> (a nominal composition) is a
typical flux used to produce large-sized and high-quality LiB<sub>3</sub>O<sub>5</sub> crystals. The structure of the LiB<sub>3</sub>O<sub>5</sub>–Li<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub> high-temperature
solution is essential to understanding the flux behavior of Li<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub> but still remains unclear. In
this work, high-temperature Raman spectroscopy combined with density
functional theory (DFT) was applied to study the LiB<sub>3</sub>O<sub>5</sub>–Li<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub> solution
structure. Raman spectra of a LiB<sub>3</sub>O<sub>5</sub>–Li<sub>4</sub>Mo<sub>5</sub>O<sub>17</sub>–Li<sub>2</sub>Mo<sub>4</sub>O<sub>13</sub> polycrystalline mixture were recorded at different
temperatures until the mixture melted completely. The solution structure
was deduced from the spectral changes and verified by DFT calculations.
When the mixture began to melt, its molybdate component first changed
into the Li<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub> melt; meanwhile,
the complicated molybdate groups existing in the crystalline state
transformed into Mo<sub>3</sub>O<sub>10</sub><sup>2–</sup> groups,
which are formed by three corner-sharing MoO<sub>3</sub>Ø<sup>–</sup>/MoO<sub>2</sub>Ø<sub>2</sub> (Ø = bridging
oxygen atom) tetrahedra. When LiB<sub>3</sub>O<sub>5</sub> dissolved
in the Li<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub> melt, the crystal
structure collapsed into polymeric chains of [B<sub>3</sub>O<sub>4</sub>Ø<sub>2</sub><sup>–</sup>]<sub><i>n</i></sub>. Its basic structural unit, the B<sub>3</sub>O<sub>4</sub>Ø<sub>2</sub><sup>–</sup> ring, coordinated with the Mo<sub>3</sub>O<sub>10</sub><sup>2–</sup> group to form a MoO<sub>3</sub>·B<sub>3</sub>O<sub>4</sub>Ø<sub>2</sub><sup>–</sup> complex and a Mo<sub>2</sub>O<sub>7</sub><sup>2–</sup> group.
On the basis of the LiB<sub>3</sub>O<sub>5</sub>–Li<sub>2</sub>Mo<sub>3</sub>O<sub>10</sub> solution structure, we discuss the LiB<sub>3</sub>O<sub>5</sub> crystal growth mechanism and the compositional
dependence of the solution viscosity
Discovery of SHR9352: A Highly Potent G Protein-Biased μ‑Opioid Receptor Agonist
Recently, targeting
the G protein-biased signaling has emerged
as an attractive therapeutic strategy for treating severe acute pain
with the potential to reduce the side effect of the traditional opioid
drug. Herein, we describe the discovery of a highly potent G protein-biased
μ-opioid receptor (MOR) agonist, SHR9352. This novel molecule
exhibited excellent MOR activity and limited β-arrestin recruitment,
as well as a high selectivity over κ-opioid receptor and δ-opioid
receptor demonstrated robust in vivo efficacy and displayed favorable
pharmacokinetic properties across species