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<jats:p>Non-vanishing electromagnetic properties of neutrinos have been predicted by many theories beyond the Standard Model, and an enhanced neutrino magnetic moment can have profound implications for fundamental physics. The XENON1T experiment recently detected an excess of electron recoil events in the 1–7 keV energy range, which can be compatible with solar neutrino magnetic moment interaction at a most probable value of <jats:italic>μ<jats:sub>ν</jats:sub> </jats:italic> = 2.1 × 10<jats:sup>−11</jats:sup> <jats:italic>μ</jats:italic> <jats:sub>B</jats:sub>. However, tritium backgrounds or solar axion interaction in this energy window are equally plausible causes. Upcoming multi-tonne noble liquid detectors will test these scenarios more in depth, but will continue to face similar ambiguity. We report a unique capability of future large liquid scintillator detectors to help resolve the potential neutrino magnetic moment scenario. With <jats:italic>O</jats:italic>(100) kton⋅year exposure of liquid scintillator to solar neutrinos, a sensitivity of <jats:italic>μ<jats:sub>ν</jats:sub> </jats:italic> &lt; 10<jats:sup>−11</jats:sup> <jats:italic>μ</jats:italic> <jats:sub>B</jats:sub> can be reached at an energy threshold greater than 40 keV, where no tritium or solar axion events but only neutrino magnetic moment signal is still present.</jats:p>

<jats:p>The transition energies, E1 transitional oscillator strengths of the spin-allowed as well as the spin-forbidden and the corresponding transition rates, and complete M1, E2, M2 forbidden transition rates for 1<jats:italic>s</jats:italic> <jats:sup>2</jats:sup>, 1<jats:italic>s</jats:italic>2<jats:italic>s</jats:italic>, and 1<jats:italic>s</jats:italic>2<jats:italic>p</jats:italic> states of He I, are investigated using the multi-configuration Dirac–Hartree–Fock method. In the subsequent relativistic configuration interaction computations, the Breit interaction and the QED effect are considered as perturbation, separately. Our transition energies, oscillator strengths, and transition rates are in good agreement with the experimental and other theoretical results. As a result, the QED effect is not important for helium atoms, however, the effect of the Breit interaction plays a significant role in the transition energies, the oscillator strengths and transition rates.</jats:p>

<jats:p>The single- and double-electron capture (SEC, DEC) processes of He<jats:sup>2+</jats:sup> ions colliding with Ne atoms are studied by utilizing the full quantum-mechanical molecular-orbital close-coupling method. Total and state-selective SEC and DEC cross sections are presented in the energy region of 2 eV/u to 20 keV/u. Results show that the dominant reaction channel is Ne<jats:sup>+</jats:sup>(2<jats:italic>s</jats:italic>2<jats:italic>p</jats:italic> <jats:sup>6</jats:sup> <jats:sup>2</jats:sup> <jats:italic>S</jats:italic>) + He<jats:sup>+</jats:sup>(1<jats:italic>s</jats:italic>) in the considered energy region due to strong couplings with the initial state Ne(2<jats:italic>s</jats:italic> <jats:sup>2</jats:sup>2<jats:italic>p</jats:italic> <jats:sup>6</jats:sup> <jats:sup>1</jats:sup> <jats:italic>S</jats:italic>) + He<jats:sup>2+</jats:sup> around the internuclear distance of 4.6 a.u. In our calculations, the SEC cross sections decrease initially and then increase whereby, the minimum point is around 0.38 keV/u with the increase of collision energies. After considering the effects of the electron translation factor (ETF), the SEC cross sections are increased by 15%–25% nearby the energy region of keV/u and agree better with the available results. The DEC cross sections are smaller than those of SEC because of the larger energy gaps and no strong couplings with the initial state. Due to the Demkov-type couplings between DEC channel Ne<jats:sup>2+</jats:sup>(2s<jats:sup>2</jats:sup>2<jats:italic>p</jats:italic> <jats:sup>4</jats:sup> <jats:sup>1</jats:sup> <jats:italic>S</jats:italic>) + He(1<jats:italic>s</jats:italic> <jats:sup>2</jats:sup>) and the dominating SEC channel Ne<jats:sup>+</jats:sup>(2<jats:italic>s</jats:italic>2<jats:italic>p</jats:italic> <jats:sup>6</jats:sup> <jats:sup>2</jats:sup> <jats:italic>S</jats:italic>) + He<jats:sup>+</jats:sup>(1<jats:italic>s</jats:italic>), the DEC cross sections increase with increasing impact energies. Good consistency can also be found between the present DEC and the experimental measurements in the overlapping energy region.</jats:p>

<jats:p>Based on the Wigner function in local equilibrium, we derive hydrodynamical quantities for a system of polarized spin-1/2 particles: the particle number current density, the energy-momentum tensor, the spin tensor, and the dipole moment tensor. Compared with ideal hydrodynamics without spin, additional terms at the first and second orders in the Knudsen number <jats:italic>Kn</jats:italic> and the average spin polarization <jats:italic>χ<jats:sub>s</jats:sub> </jats:italic> have been derived. The Wigner function can be expressed in terms of matrix-valued distributions, whose equilibrium forms are characterized by thermodynamical parameters in quantum statistics. The equations of motion for these parameters are derived by conservation laws at the leading and next-to-leading order <jats:italic>Kn</jats:italic> and <jats:italic>χ<jats:sub>s</jats:sub> </jats:italic>.</jats:p>

<jats:p>Two-dimensional honeycomb crystals have inspired intense research interest for their novel properties and great potential in electronics and optoelectronics. Here, through molecular beam epitaxy on SrTiO<jats:sub>3</jats:sub>(001), we report successful epitaxial growth of metal-rich chalcogenide Fe<jats:sub>2</jats:sub>Te, a honeycomb-structured film that has no direct bulk analogue, under Te-limited growth conditions. The structural morphology and electronic properties of Fe<jats:sub>2</jats:sub>Te are explored with scanning tunneling microscopy and angle resolved photoemission spectroscopy, which reveal electronic bands cross the Fermi level and nearly flat bands. Moreover, we find a weak interfacial interaction between Fe<jats:sub>2</jats:sub>Te and the underlying substrates, paving a newly developed alternative avenue for honeycomb-based electronic devices.</jats:p>

<jats:p>Lithium plays an increasingly important role in scientific and industrial processes, and it is extremely important to extract lithium from a high Mg<jats:sup>2+</jats:sup>/Li<jats:sup>+</jats:sup> mass ratio brine or to recover lithium from the leachate of spent lithium-ion batteries. Conventional wisdom shows that Li<jats:sup>+</jats:sup> with low valence states has a much weaker adsorption (and absorption energy) with graphene than multivalent ions such as Mg<jats:sup>2+</jats:sup>. Here, we show the selective adsorption of Li<jats:sup>+</jats:sup> in thermally reduced graphene oxide (rGO) membranes over other metal ions such as Mg<jats:sup>2+</jats:sup>, Co<jats:sup>2+</jats:sup>, Mn<jats:sup>2+</jats:sup>, Ni<jats:sup>2+</jats:sup>, or Fe<jats:sup>2+</jats:sup>. Interestingly, the adsorption strength of Li<jats:sup>+</jats:sup> reaches up to 5 times the adsorption strength of Mg<jats:sup>2+</jats:sup>, and the mass ratio of a mixed Mg<jats:sup>2+</jats:sup>/Li<jats:sup>+</jats:sup> solution at a very high value of 500 : 1 can be effectively reduced to 0.7 : 1 within only six experimental treatment cycles, demonstrating the excellent applicability of the rGO membranes in the Mg<jats:sup>2+</jats:sup>/Li<jats:sup>+</jats:sup> separation. A theoretical analysis indicates that this unexpected selectivity is attributed to the competition between cation–<jats:italic>π</jats:italic> interaction and steric exclusion when hydrated cations enter the confined space of the rGO membranes.</jats:p>

<jats:p>Magnetic exchange interactions (MEIs) define networks of coupled magnetic moments and lead to a surprisingly rich variety of their magnetic properties. Typically MEIs can be estimated by fitting experimental results. Unfortunately, how many MEIs need to be included in the fitting process for a material is unclear a priori, which limits the results obtained by these conventional methods. Based on linear spin-wave theory but without performing matrix diagonalization, we show that for a general quadratic spin Hamiltonian, there is a simple relation between the Fourier transform of MEIs and the sum of square of magnon energies (SSME). We further show that according to the real-space distance range within which MEIs are considered relevant, one can obtain the corresponding relationships between SSME in momentum space. By directly utilizing these characteristics and the experimental magnon energies at only a few high-symmetry <jats:italic>k</jats:italic> points in the Brillouin zone, one can obtain strong constraints about the range of exchange path beyond which MEIs can be safely neglected. Our methodology is also generally applicable for other Hamiltonian with quadratic Fermi or Boson operators.</jats:p>

<jats:p>Coupling of a phase transition to electron and phonon transports provides extra degree of freedom to improve the thermoelectric performance, while the pertinent experimental and theoretical studies are still rare. Particularly, the impaction of chemical compositions and phase transition characters on the abnormal thermoelectric properties across phase transitions are largely unclear. Herein, by varying the Cu content <jats:italic>x</jats:italic> from 1.75 to 2.10, we systemically investigate the crystal structural evolution, phase transition features, and especially the thermoelectric properties during the phase transition for Cu<jats:sub> <jats:italic>x</jats:italic> </jats:sub>Se. It is found that the addition of over-stoichiometry Cu in Cu<jats:sub> <jats:italic>x</jats:italic> </jats:sub>Se could alter the phase transition characters and suppress the formation of Cu vacancies. The critical scatterings of phonons and electrons during phase transitions strongly enhance the Seebeck coefficient and diminish the thermal conductivity, leading to an ultrahigh dimensionless thermoelectric figure of merit of ∼1.38 at 397 K in Cu<jats:sub>2.10</jats:sub>Se. With the decreasing Cu content, the critical electron and phonon scattering behaviors are mitigated, and the corresponding thermoelectric performances are reduced. This work offers inspirations for understanding and tuning the thermoelectric transport properties during phase transitions.</jats:p>

<jats:p>Two-dimensional (2D) topological insulators present a special phase of matter manifesting unique electronic properties. Till now, many monolayer binary compounds of Sb element, mainly with a honeycomb lattice, have been reported as 2D topological insulators. However, research of the topological insulating properties of the monolayer Sb compounds with square lattice is still lacking. Here, by means of the first-principles calculations, a monolayer SbI with square lattice is proposed to exhibit the tunable topological properties by applying strain. At different levels of the strain, the monolayer SbI shows two different structural phases: buckled square structure and buckled rectangular structure, exhibiting attracting topological properties. We find that in the buckled rectangular phase, when the strain is greater than 3.78%, the system experiences a topological phase transition from a nontrivial topological insulator to a trivial insulator, and the structure at the transition point actually is a Dirac semimetal possessing two type-I Dirac points. In addition, the system can achieve the maximum global energy gap of 72.5 meV in the topological insulator phase, implying its promising application at room temperature. This study extends the scope of 2D topological physics and provides a platform for exploring the low-dissipation quantum electronics devices.</jats:p>

<jats:p>In the transport studies of topological insulators, microflakes exfoliated from bulk single crystals are often used because of the convenience in sample preparation and the accessibility to high carrier mobilities. Here, based on finite element analysis, we show that for the non-Hall-bar shaped topological insulator samples, the measured four-point resistances can be substantially modified by the sample geometry, bulk and surface resistivities, and magnetic field. Geometry correction factors must be introduced for accurately converting the four-point resistances to the longitudinal resistivity and Hall resistivity. The magnetic field dependence of inhomogeneous current density distribution can lead to pronounced positive magnetoresistance and nonlinear Hall effect that would not exist in the samples of ideal Hall bar geometry.</jats:p>