Electrically controlled superconducting states at the heterointerface SrTiO3_3/LaAlO3_3

We study the symmetry of Cooper pair in a two-dimensional Hubbard model with the Rashba-type spin-orbit interaction as a minimal model of electron gas generated at a heterointerface of SrTiO$_3$/LaAlO$_3$. Solving the Eliashberg equation based on the third-order perturbation theory, we find that the gap function consists of the mixing of the spin-singlet $d_{xy}$-wave component and the spin-triplet $(p_x\pm ip_y)$-wave one due to the broken inversion symmetry originating from the Rashba-type spin-orbit interaction. The ratio of the d-wave and the p-wave component continuously changes with the carrier concentration. We propose that the pairing symmetry is controlled by tuning the gate voltage.Comment: 4 pages, 4 figures; added reference

High throughput methodology for synthesis, screening, and optimization of solid state Lithium ion electrolytes

A study of the lithium ion conductor Li3xLa2/3–xTiO3 solid solution and the surrounding composition space was carried out using a high throughput physical vapor deposition system. An optimum total ionic conductivity value of 5.45 × 10–4 S cm–1 was obtained for the composition Li0.17La0.29Ti0.54 (Li3xLa2/3–xTiO3x = 0.11). This optimum value was calculated using an artificial neural network model based on the empirical data. Due to the large scale of the data set produced and the complexity of synthesis, informatics tools were required to analyze the data. Partition analysis was carried out to determine the synthetic parameters of importance and their threshold values. Multivariate curve resolution and principal component analysis were applied to the diffraction data set. This analysis enabled the construction of phase distribution diagrams, illustrating both the phases obtained and the compositional zones in which they occur. The synthetic technique presented has significant advantages over other thin film and bulk methodologies, in terms of both the compositional range covered and the nature of the materials produce

Fulde-Ferrell-Larkin-Ovchinnikov State in the absence of a Magnetic Field

We propose that in a system with pocket Fermi surfaces, a pairing state with a finite total momentum q_tot like the Fulde-Ferrell-Larkin-Ovchinnikov state can be stabilized even without a magnetic field. When a pair is composed of electrons on a pocket Fermi surface whose center is not located at Gamma point, the pair inevitably has finite q_tot. To investigate this possibility, we consider a two-orbital model on a square lattice that can realize pocket Fermi surfaces and we apply fluctuation exchange approximation. Then, by changing the electron number n per site, we indeed find that such superconducting states with finite q_tot are stabilized when the system has pocket Fermi surfaces.Comment: 4 pages, 5 figure

Early effects of 7.5% hypertonic saline solution on splanchnic perfusion after hemorrhagic shock

PURPOSE: To evaluate the effects of SSH resuscitation on systemic and splanchnic hemodynamic variables in an experimental model of controlled hemorrhagic shock. METHODS: Ten mongrel dogs were bled (20 ml/min) to a target mean arterial pressure (MAP) of 40±5 mmHg. After 30 minutes of shock, animals received SSH infused in 5-minute and they were observed for 60 minutes thereafter. Systemic hemodynamics were evaluated through a Swan-Ganz and arterial catheters while gastrointestinal tract perfusion by a catheter inside the portal vein, an ultrasonic flowprobe around portal vein blood flow (PVBF) and a gastric tonometer. Splanchnic oxygen delivery and consumption, intramucosal pH and veno-arterial, portal-arterial and mucosal-arterial pCO2-gradients (Dap-a pCO2, Dvp-a pCO2 e Dt-a pCO2, respectively) were assessed. RESULTS: Hemorrhage (29.8±2.4ml/Kg) induced significant decreases in MAP (125±6 to 42±1 mmHg), in CO (1.9±0.2 to 0.6±0.1 L/min), and PVBF (504±73 to 126±12 ml/min) while significant increases were detected in Dap-a pCO2 (5.3±0.8 to 19.9±1.6 mmHg) Dvp-a pCO2 (5.4±1.4 to 22.6±2.1 mmHg) and Dt-a pCO2 (6.1±1.1 to 43.8±7.5 mmHg). SSH infusion promoted only partial benefits in systemic and splanchnic blood flows. Reduced pCO2 gradients but fewer effects in Dt-a pCO2 were observed. CONCLUSION: The SSH infusion promoted partial systemic and splanchnic hemodynamic benefits. Those benefits were especially poor at the splanchnic microcirculation, as evaluated by Dt-a pCO2. In addition, systemic and regional oxygen-derived variables do not reflect the regional microcirculation disturbances. Gastrointestinal tonometry clearly represents a useful tool for monitoring splanchnic perfusion in patients in hemodynamic shock.OBJETIVO: Avaliar os efeitos hemodinâmicos sistêmicos e esplâncnico da expansão volêmica inicial com SSH em modelo de choque hemorrágico controlado. MÉTODOS: Dez cães foram submetidos a sangramento controlado (20 ml/min) até uma pressão arterial média de 40±5 mmHg (PAM). Após 30 minutos de choque, receberam 4 ml/Kg de SSH em 5 minutos e posteriormente observados sem intervenções adicionais durante 60 minutos. As variáveis hemodinâmicas sistêmicas foram obtidas de um cateter arterial e de um cateter de Swan-Ganz, enquanto as regionais através da cateterização da veia porta, fluxômetro ultrassônico na veia porta e um tonômetro na cavidade. A oferta, taxa de extração e consumo esplâncnico de oxigênio, pH intramucoso e os gradientes veno-arterial, porta-arterial e mucosa-arterial da pCO2 (Dap-a pCO2, Dvp-a pCO2 e Dt-a pCO2, respectivamente), foram calculados. RESULTADOS: A hemorragia (29,8±2,4 ml/Kg) reduziu a pressão arterial média (125±6 para 42±1 mmHg), o DC (1,9±0,2 para 0,6±0,1 L/min) e o fluxo porta (504±73 para 126±12 ml/min), enquanto elevou o Dap-a pCO2 (5,3±0,8 para 19,9±1,6 mmHg), Dvp-a pCO2 (5,4±1,4 para 22,6±2,1 mmHg) e o Dt-a pCO2 (6,1±1,1 para 43,8±7,5 mmHg). A infusão de SSH resultou em recuperação parcial dos fluxos sistêmico e porta. Atenuou os gradientes de CO2 com menor impacto sobre o Dt-a pCO2. CONCLUSÃO: A SSH promoveu benefícios parciais na perfusão sistêmica e esplâncnica, os quais foram especialmente limitados na microcirculação regional, como demonstrado pelo Dt-a pCO2. Além disso, as variáveis sistêmicas e regionais dependentes de oxigênio, não refletem a adequação da perfusão da mucosa gástrica, enfatizando a importância da monitorização deste território - pela tonometria - durante os estados de choque.USP FM InCorUNIFESP-EPM Depto. de CirurgiaUSP FM Depto. de CardiopneumologiaUNIFESP, EPM, Depto. de CirurgiaSciEL

Origin of the Weak Pseudo-gap Behaviors in Na_{0.35}CoO_2: Absence of Small Hole Pockets

We analyze the ``normal electronic states'' of Na_{0.35}CoO_2 based on the effective d-p model with full d-orbital freedom using the fluctuation-exchange (FLEX) approximation. They sensitively depend on the topology of the Fermi surfaces, which changes as the crystalline electric splitting (CES) due to the trigonal deformation. We succeed in reproducing the weak pseudo-gap behaviors in the density of states (DOS) and in the uniform magnetic susceptibility below 300K, assuming that six small hole-pockets predicted by LDA band calculations are absent. When they exist, on the contrary, then ``anti-pseudo-gap behaviors'' should inevitably appear. Thus, the present study strongly supports the absence of the small hole-pockets in Na_{0.35}CoO_2, as reported by recent ARPES measurements. A large Fermi surface around the \Gamma-point would account for the superconductivity in water-intercalated samples.Comment: 5pages, to appear in J. Phys. Soc. Jpn. Vol.74 (2005) No.

Flat bands in topological media

Topological media are systems whose properties are protected by topology and thus are robust to deformations of the system. In topological insulators and superconductors the bulk-surface and bulk-vortex correspondence gives rise to the gapless Weyl, Dirac or Majorana fermions on the surface of the system and inside vortex cores. Here we show that in gapless topological media, the bulk-surface and bulk-vortex correspondence is more effective: it produces topologically protected gapless fermions without dispersion -- the flat band. Fermion zero modes forming the flat band are localized on the surface of topological media with protected nodal lines and in the vortex core in systems with topologically protected Fermi points (Weyl points). Flat band has an extremely singular density of states, and we show that this property may give rise in particular to surface superconductivity which could exist even at room temperature.Comment: 9 pages, 5 figures, version to appear in JETP Letter

Deformation of Electronic Structures Due to CoO6 Distortion and Phase Diagrams of NaxCoO2.yH2O

Motivated by recently reported experimental phase diagrams, we study the effects of CoO6 distortion on the electronic structure in NaxCoO2.yH2O. We construct the multiband tight-binding model by employing the LDA result. Analyzing this model, we show the deformation of band dispersions and Fermi-surface topology as functions of CoO2-layer thickness. Considering these results together with previous theoretical ones, we propose a possible schematic phase diagram with three successive phases: the extended s-wave superconductivity (SC), the magnetic order, and the spin-triplet SC phases when the Co valence number s is +3.4. A phase diagram with only one phase of spin-triplet SC is also proposed for the s=+3.5 case.Comment: 4 pages, 5 figure

Weak-Coupling Theory for Multiband Superconductivity Induced by Jahn-Teller Phonons

Emergence of superconductivity in a two-band system coupled with breathing and Jahn-Teller phonons is discussed in a weak-coupling limit. With the use of a standard quantum mechanical procedure, the phonon-mediated attraction is derived. From the analysis of the model including such attraction, a BCS-like formula for a superconducting transition temperature $T_{\rm c}$ is obtained. When only the breathing phonon is considered, $T_{\rm c}$ is the same as that of the one-band model. On the other hand, when Jahn-Teller phonons are active, $T_{\rm c}$ is significantly enhanced by the interband attraction even within the weak-coupling limit. Relevance of the present result to actual materials such as iron pnictides is briefly commented.Comment: 4 pages, 3 figures

Topology of Andreev Bound States with Flat Dispersion

A theory of dispersionless Andreev bound states on surfaces of time-reversal invariant unconventional superconductors is presented. The generalized criterion for the dispersionless Andreev bound state is derived from the bulk-edge correspondence, and the chiral spin structure of the dispersionless Andreev bound states is argued from which the Andreev bound state is stabilized. Then we summarize the criterion in a form of index theorems. The index theorems are proved in a general framework to certify the bulk-edge correspondence. As concrete examples, we discuss (i) dxy-wave superconductor (ii) px-wave superconductor, and (iii) noncentrosymmetric superconductors. In the last example, we find a peculiar time-reversal invariant Majorana fermion. The time-reversal invariant Majorana fermion shows an unusual response to the Zeeman magnetic field, which can be used to identify it experimentally.Comment: 56 pages, 11 figures, references are adde