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Journal Articles

Assessing and tackling the barocaloric fatigue for applicable solid-state refrigeration

Xue, J.*; Huang, D.*; Hattori, Takanori; Li, L.*; Feng, Y.*; Wang, H.*; Fan, X.*; Yao, J.*; Wang, Y.*; Liu, Z.*; et al.

Applied Physics Letters, 128(20), p.201903_1 - 201903_8, 2026/05

 Times Cited Count:0 Percentile:0.00(Physics, Applied)

The cycling fatigue and barocaloric response of NH$$_4$$I is directly assessed under loading-unloading cycles with stress up to 100,MPa, with the adiabatic temperature change ($$Delta T_{mathrm{ad}}$$) decaying from 15,K to approximately 0.8,K after 100 cycles. $emph{In situ}$ X-ray diffraction, Raman spectroscopy, and neutron diffraction concertedly reveal the existence of the residual high-pressure phase even after the first unloading, whose fraction is rapidly increased to 90% at the 100th cycle. A phenomenological model is developed to elucidate this fatigue behavior, and an excellent agreement with experimental data has been achieved. To relieve the intergranular stress and enhance the mobility of grains, we encapsulate the composite of NH$$_4$$I particles and silicone oil into a 3D-printed polymer shell. Such an architectural tailoring has markedly improved the cyclic stability of the barocaloric effect with $$Delta T_{mathrm{ad}}$$ rising to c.a. 4.6,K after 100 cycles. Our results establish a fundamental understanding of the barocaloric fatigue behavior and pave a feasible route to applicable barocaloric cooling technology.

Journal Articles

All-temperature barocaloric effects at pressure-induced phase transitions

Zhao, X.*; Zhang, Z.*; Hattori, Takanori; Wang, J.*; Li, L.*; Jia, Y.*; Li, W.*; Xue, J.*; Fan, X.*; Song, R.*; et al.

Nature Communications (Internet), 16, p.7713_1 - 7713_8, 2025/08

 Times Cited Count:10 Percentile:78.37(Multidisciplinary Sciences)

Caloric effects usually occur in the vicinity of solid-state phase transitions with a limited refrigeration temperature span. Here, we introduce and realize an unprecedented concept -all temperature barocaloric effect, i.e., a remarkable barocaloric effect in KPF$$_6$$ across an exceptionally wide temperature span, from 77.5 to 300 K and potentially down to 4 K, covering typical room temperature, liquid nitrogen, liquid hydrogen, and liquid helium refrigeration regions. The directly measured barocaloric adiabatic temperature change reaches 12 K at room temperature and 2.5 K at 77.5 K upon the release of a 250 MPa pressure. This effect is attributed to a persistent phase transition to a rhombohedral high pressure phases. We depict the thermodynamic energy landscape to account for the structural instability. This unique all-temperature barocaloric effect presents a novel approach to highly applicable solid-state refrigeration technology, transcending the conventional multi-stage scenario.

Journal Articles

Super-absorbent polymer valves and colorimetric chemistries for time-sequenced discrete sampling and chloride analysis of sweat via skin-mounted soft microfluidics

Kim, S. B.*; Zhang, Y.*; Won, S. M.*; Bandodkar, A. J.*; Sekine, Yurina; Xue, Y.*; Koo, J.*; Harshman, S. W.*; Martin, J. A.*; Park, J. M.*; et al.

Small, 14(12), p.1703334_1 - 1703334_11, 2018/03

 Times Cited Count:143 Percentile:96.16(Chemistry, Multidisciplinary)

Oral presentation

Water structure in a hydrogel

Sekine, Yurina; Fukazawa, Hiroshi; Songxue, C.*; Chakoumakos, B.*; Fernandez-Baca, J. A.*

no journal, , 

no abstracts in English

Oral presentation

Neutron scattering study on NdB$$_4$$

Metoki, Naoto; Yamauchi, Hiroki; Watanuki, Ryuta*; Suzuki, Kazuya*; Hagihara, Masato*; Masuda, Takatsugu*; Matsuda, Masaaki*; Songxue, C.*; Fernandez Baca, J.*

no journal, , 

Our neutron scattering study and using representational analysis revealed the magnetic structure in phase II of NdB$$_4$$ with Shastry-Sutherland lattice. We found that the magnetic structure is described by the mixture of the basis vector of $$Gamma_2$$ and $$Gamma_4$$ representation with the magnetic moment of about 2$$mu_B$$. We observed pseudo-quartet CEF state and the temperature dependence by means of neutron inelastic scattering below 5 meV.

Oral presentation

Structure of water and ice in poly-N,N,-dimethylacrylamide hydrogel

Sekine, Yurina; Fukazawa, Tomoko*; Yamauchi, Hiroki; Songxue, C.*; Chakoumakos, B.*; Fernandez-Baca, J. A.*; Fukazawa, Hiroshi

no journal, , 

Neutron diffraction data of deuterated poly-N,N,-dimethylacrylamide (PDMAA) hydrogel were measured at temperatures of 10 - 290 K in order to investigate the structure and properties of water in the hydrogel. Diffraction peaks observed below 270 K indicate the existence of a solid ice in the hydrogel. The positions of some peaks from the ice are lower than those in ordinary hexagonal ice (Ih). The lower shifts of the peaks indicates that the lattice constants of the c-axis in the ice are about 0.3% higher than those in ice Ih, whereas those of the a-axis are almost consist. The results show that bulk of a low-density ice crystal exists in the PDMAA hydrogel. The water molecules, which have a significant interaction with the polymer chains, play an important role in the chemical and mechanical properties of the hydrogel.

Oral presentation

$$f$$-electron states in RPd$$_5$$Al$$_2$$ (R: Pr, Nd)

Metoki, Naoto; Yamauchi, Hiroki; Kitazawa, Hideaki*; Suzuki, Hiroyuki*; Hagihara, Masato*; Masuda, Takatsugu*; Matsuda, Masaaki*; Aczel, A. A.*; Songxue, C.*; Hong, T.*; et al.

no journal, , 

In order to elucidate the 5$$f$$-electron states in the heavy electron superconductor NpPd$$_5$$Al$$_2$$, neutron scattering experiments of the rare earth based iso-structural family have been carried out. The observed crystal field excitations of PrPd$$_5$$Al$$_2$$ and NdPd$$_5$$Al$$_2$$ were analyzed via the crystal field Hamiltonian with tetragonal symmetry, diagonalized analytically. The experimentally obtained crystal field parameters $$A_{lm}$$were very similar in CePd$$_5$$Al$$_2$$, PrPd$$_5$$Al$$_2$$, and NdPd$$_5$$Al$$_2$$, indicating a common effective charge potential in this series. We succeeded to clarify the 5$$f$$ electron states of NpPd$$_5$$Al$$_2$$ and UPd$$_5$$Al$$_2$$ in comparison with these results.

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