33 research outputs found
Direct observation of the ground state of a 1/3 quantum magnetization plateau in SrMnPO using neutron diffraction measurements
We can directly investigate the ground state in magnetization-plateau fields
(plateau ground state) using neutron diffraction measurements. We performed
neutron diffraction measurements on the spin-5/2 trimer substance
SrMnPO in magnetization-plateau fields. The integrated
intensities of magnetic reflections calculated using an expectation value of
each spin in a plateau ground state of an isolated-trimer model agree well with
those obtained experimentally in the magnetization-plateau fields. We succeeded
in direct observation of a plateau ground state in SrMnPO
Spiral magnetic structure in spin-5/2 frustrated trimerized chains in SrMn3P4O14
We study a spin-5/2 antiferromagnetic trimerized chain substance SrMn3P4O14
using neutron powder diffraction experiments. The coplanar spiral magnetic
structure appears below T_N1 = 2.2(1) K. Values of several magnetic structure
parameters change rapidly at T_N2 = 1.75(5) K, indicating another phase
transition, although the magnetic structures above and below T_N2 are the
qualitatively same. The spiral magnetic structure can be explained by
frustration between nearest-neighbor and next-nearest-neighbor exchange
interactions in the trimerized chains.Comment: submitted to Phys. Rev.
Regulation of NDVI and ET negative responses to increased atmospheric vapor pressure deficit by water availability in global drylands
Atmospheric vapor pressure deficit (VPD, indicative of atmospheric water conditions) has been identified as a major driver of global vegetation dynamics. Drylands, including deserts, temperate grasslands, savannas, and dry forests, are more sensitive to water conditions and affect carbon, nitrogen, and water cycles. However, our knowledge is limited on the way increasing VPD affects vegetation growth and evapotranspiration (ET) in global drylands. In this study, we used long-term satellite datasets combined with multiple statistical analyses to examine the relationship between the satellite-derived normalized difference vegetation index (NDVI), a proxy for vegetation growth, and ET to VPD across global drylands. We found that significant decreases in NDVI and ET predominantly influenced the NDVI (RVPD − NDVI) and ET (RVPD − ET) responses to VPD in both the savannas and dry forests of South American, African, and Australian savannas and dry forests, as well as in temperate grasslands (e.g., Eurasian steppes and American prairies). Notably, more than 60% of global drylands exhibited significantly negative RVPD − NDVI and RVPD − ET values. In contrast, the percentage of significantly negative RVPD − NDVI and RVPD − ET decreased to <10% in cold drylands (>60° N). In predominantly warm drylands (60° N~60° S), negative VPD effects were significantly and positively regulated by soil water availability, as determined by multiple linear regression models. However, these significant regulatory effects were not observed in cold drylands. Moving-window analyses further revealed that temporal changes in RVPD − NDVI and RVPD − ET were positively correlated with changes in the Standardized Precipitation Evapotranspiration Index (SPEI). In warm drylands, areas with increasing RVPD − NDVI and RVPD − ET over time showed an increasing trend in the SPEI, whereas areas with a decreasing SPEI showed a negative trend in RVPD − NDVI and RVPD − ET values over time. Given the increasing atmospheric dryness due to climate change, this study highlighted the importance of re-evaluating the representation of the role of water availability in driving the response of the carbon-water cycle to increased VPD across global drylands
Modeling and Analysis of the Influence of an Edge Filter on the Combining Efficiency and Beam Quality of a 10-kW-Class Spectral Beam-Combining System
Filter-based spectral beam combining (FSBC) is a promising power-scaling concept for high-power, broad-linewidth fiber lasers, as it relaxes the requirements for linewidth control and also the sizes of the individual beams. As the combining element in the FSBC system, the steep-edge filter plays a major role in achievement of the combining efficiency and the beam quality. In this case, we combine the uncorrelated surface roughness model and the combining efficiency model, and we conduct a comprehensive analysis of the effects of surface roughness, thickness error, and incident angle on the filter’s optical properties and the combining efficiency, in order to determine the optimal configuration for the laser beam-combining system. The simulation results show a good agreement with the measured ones. Meanwhile, through the adoption of the angular spectrum theory, this paper has also conducted a preliminary analysis of the influence of the combining elements on the quality of the combined beam, and some theoretical instructions on the future design of the spectral beam-combining system are provided
Observation of the Sixth Polymorph of BiB<sub>3</sub>O<sub>6</sub>: In Situ High-Pressure Raman Spectroscopy and Synchrotron X‑ray Diffraction Studies on the β‑Polymorph
β-BiB<sub>3</sub>O<sub>6</sub> was compressed in a diamond anvil cell at room temperature and studied
using a combinstion of in situ high-pressure Raman scattering and
angle-dispersive synchrotron X-ray diffraction. The results reveal
that β-BiB<sub>3</sub>O<sub>6</sub> retains its structure below
9.0 GPa and undergoes a structural phase transition that starts at
∼11.5 GPa and finishes at ∼18.5 GPa. No other phase
transition occurred with increasing pressure up to ∼46 GPa.
It was also found that the high-pressure phase is different from the
already-reported five polymorphs of BiB<sub>3</sub>O<sub>6</sub>.
Therefore, the new phase is denoted as ζ-BiB<sub>3</sub>O<sub>6</sub>, which could be indexed by an orthorhombic unit cell (<i>a</i> ≈ 12.5 Å, <i>b</i> ≈ 6.7
Å, <i>c</i> ≈ 4.0 Å) from the powder XRD
pattern collected at 22.2 GPa. Moreover, ζ-BiB<sub>3</sub>O<sub>6</sub> can be quenched to ambient conditions. The investigation
of the pressure dependence of the lattice parameters reveals that
both β-BiB<sub>3</sub>O<sub>6</sub> and ζ-BiB<sub>3</sub>O<sub>6</sub> exhibit a large amount of crystallographic anisotropy.
An unusual expansion of the <i>c</i>-axis of ζ-BiB<sub>3</sub>O<sub>6</sub> was observed. Assignments for the Raman spectra
of β-BiB<sub>3</sub>O<sub>6</sub>, γ-BiB<sub>3</sub>O<sub>6</sub>, and δ-BiB<sub>3</sub>O<sub>6</sub> under ambient conditions
were also performed. Currently, we cannot solve the crystal structure
of ζ-BiB<sub>3</sub>O<sub>6</sub> but give some speculations
based on its relationship with β-BiB<sub>3</sub>O<sub>6</sub>
Chemical Substitution-Induced and Competitive Formation of 6H and 3C Perovskite Structures in Ba<sub>3–<i>x</i></sub>Sr<sub><i>x</i></sub>ZnSb<sub>2</sub>O<sub>9</sub>: The Coexistence of Two Perovskites in 0.3 ≤ <i>x</i> ≤ 1.0
6H and 3C perovskites
are important prototype structures in materials science. We systemically
studied the structural evolution induced by the Sr<sup>2+</sup>-to-Ba<sup>2+</sup> substitution to the parent 6H perovskite Ba<sub>3</sub>ZnSb<sub>2</sub>O<sub>9</sub>. The 6H perovskite is only stable in the narrow
range of <i>x</i> ≤ 0.2, which attributes to the
impressibility of [Sb<sub>2</sub>O<sub>9</sub>]. The preference of
90° Sb–O–Sb connection and the strong Sb<sup>5+</sup>-Sb<sup>5+</sup> electrostatic repulsion in [Sb<sub>2</sub>O<sub>9</sub>] are competitive factors to stabilize or destabilize the
6H structure when chemical pressure was introduced by Sr<sup>2+</sup> incorporation. Therefore, in the following, a wide two-phase region
containing 1:2 ordered 6H–Ba<sub>2.8</sub>Sr<sub>0.2</sub>ZnSb<sub>2</sub>O<sub>9</sub> and rock-salt ordered 3C–Ba<sub>2</sub>SrZnSb<sub>2</sub>O<sub>9</sub> was observed (0.3 ≤ <i>x</i> ≤ 1.0). In the final, the successive symmetry descending
was established from cubic (<i>Fm</i>3̅<i>m</i>, 1.3 ≤ <i>x</i> ≤ 1.8) to tetragonal (<i>I</i>4/<i>m</i>, 2.0 ≤ <i>x</i> ≤
2.4), and finally to monoclinic (<i>I</i>2/<i>m</i>, 2.6 ≤ <i>x</i> ≤ 3.0). Here we proved that
the electronic configurations of B-site cations, with either empty,
partially, or fully filled d-shell, would also affect the structure
stabilization, through the orientation preference of the B–O
covalent bonding. Our investigation gives a deeper understanding of
the factors to the competitive formation of perovskite structures,
facilitating the fine manipulation on their physical properties
ZnGa<sub>2–<i>x</i></sub>In<sub><i>x</i></sub>S<sub>4</sub> (0 ≤ <i>x</i> ≤ 0.4) and Zn<sub>1–2<i>y</i></sub>(CuGa)<sub><i>y</i></sub>Ga<sub>1.7</sub>In<sub>0.3</sub>S<sub>4</sub> (0.1 ≤ <i>y</i> ≤ 0.2): Optimize Visible Light Photocatalytic H<sub>2</sub> Evolution by Fine Modulation of Band Structures
Band structure engineering
is an efficient technique to develop desired semiconductor photocatalysts,
which was usually carried out through isovalent or aliovalent ionic
substitutions. Starting from a UV-activated catalyst ZnGa<sub>2</sub>S<sub>4</sub>, we successfully exploited good visible light photocatalysts
for H<sub>2</sub> evolution by In<sup>3+</sup>-to-Ga<sup>3+</sup> and
(Cu<sup>+</sup>/Ga<sup>3+</sup>)-to-Zn<sup>2+</sup> substitutions.
First, the bandgap of ZnGa<sub>2–<i>x</i></sub>ÂIn<sub><i>x</i></sub>S<sub>4</sub> (0 ≤ <i>x</i> ≤ 0.4) decreased from 3.36 to 3.04 eV by lowering the conduction
band position. Second, Zn<sub>1–2<i>y</i></sub>(CuGa)<sub><i>y</i></sub>ÂGa<sub>1.7</sub>In<sub>0.3</sub>S<sub>4</sub> (<i>y</i> = 0.1, 0.15, 0.2) provided a further
and significant red-shift of the photon absorption to ∼500
nm by raising the valence band maximum and barely losing the overpotential
to water reduction. Zn<sub>0.7</sub>Cu<sub>0.15</sub>ÂGa<sub>1.85</sub>In<sub>0.3</sub>S<sub>4</sub> possessed the highest H<sub>2</sub> evolution rate under pure visible light irradiation using
S<sup>2–</sup> and SO<sub>3</sub><sup>2–</sup> as sacrificial
reagents (386 μmol/h/g for the noble-metal-free sample and 629
μmol/h/g for the one loaded with 0.5 wt % Ru), while the binary
hosts ZnGa<sub>2</sub>S<sub>4</sub> and ZnIn<sub>2</sub>S<sub>4</sub> (synthesized using the same procedure) show 0 and 27.9 μmol/h/g,
respectively. The optimal apparent quantum yield reached to 7.9% at
500 nm by tuning the composition to Zn<sub>0.6</sub>Cu<sub>0.2</sub>ÂGa<sub>1.9</sub>In<sub>0.3</sub>S<sub>4</sub> (loaded with
0.5 wt % Ru)