Fig. 6 Global phase diagram.

Slides:

Advertisements

Similar presentations

Empirical mutation-selection phase diagram of tumor evolution.

Advertisements

Empirical mutation-selection phase diagram of tumor evolution.

Mechanochemical Symmetry Breaking in Hydra Aggregates

Shock-Wave Exploration of the High-Pressure Phases of Carbon

Fig. 2 Evolution of structural and magnetic properties.

Fig. 4 Pupil shape and image quality in the model sheep eye.

Fig. 4 Schematic illustration of the pH-mediated reorganization of the interchain hydrogen bond network of the PSPMA brushes. Schematic illustration of.

Fig. 1 Sensing scheme with an atomic spin sensor.

Fig. 2 New bathymetry. New bathymetry. (A) Uninterpreted bathymetry. Black lines represent seismic profiles acquired. The white line shows the position.

Fig. 4 Estimations of nonlinear functionals of a single-qubit state with the quantum Fredkin gate. Estimations of nonlinear functionals of a single-qubit.

Fig. 4 3D reconfiguration of liquid metals for electronics.

Spatial-temporal pattern of lower-crustal effective viscosities

The rain-fed maize growing niche in the southwestern United States, A

Fig. 2 Reaction kinetics in single-molecule junctions with OEEFs and in NMR tube. Reaction kinetics in single-molecule junctions with OEEFs and in NMR.

Fig. 1 Evolution of magnetic field lines around a foreshock bubble in the GSE-XY plane (z = 0): Results of a hybrid simulation. Evolution of magnetic field.

Fig. 2 Zeeman splitting of the plateau and associated Kondo feature.

Reproduction of reentrant supercurrent data in a closed quantum dot

Fig. 3 Electron PSD in various regions.

Experimental supercurrent and corresponding quantum dot modeling

Fig. 2 Ferroelectric domains resolved in WTe2 single crystals.

Fig. 3 Piezoresistive e-skin with interlocked microdome arrays for simultaneous detection of static pressure and temperature. Piezoresistive e-skin with.

Fig. 1 Schematics and design of the device structure.

Fig. 1 Cryo-EM structure of yeast Elp123 showing its active site.

Stability and demographic responses of ant communities to warming

Fig. 3 Controlled phase shift.

Fig. 2 Reconstructed global mean temperatures.

Fig. 1 Bioinspired design of AAD for promoting wound contraction.

Fig. 1 AMOC stability in modern climate and AMOC response under global warming. AMOC stability in modern climate and AMOC response under global warming.

Fig. 2 Four types of MJO propagation patterns along the equator.

Fig. 1 Phase diagram and FS topologies.

Fig. 2 Variation of the SHC with carrier lifetime.

Fig. 3 Correlation between magnetoresistance and emergence of superconductivity. Correlation between magnetoresistance and emergence of superconductivity.

Fig. 4 Memristive characteristics in a 1T-TaS2 nano-thick crystal.

Fig. 1 1T-TaS2 single crystals with reduced thickness.

Fig. 5 Schematic phase diagrams of Ising spin systems and Mott transition systems. Schematic phase diagrams of Ising spin systems and Mott transition systems.

Fig. 1 Crystal structure and superconductivity in fcc fullerides.

Experimental phase diagram of zero-bias conductance peaks in superconductor/semiconductor nanowire devices by Jun Chen, Peng Yu, John Stenger, Moïra Hocevar,

by Yoshifumi Tokiwa, Boy Piening, Hirale S. Jeevan, Sergey L

Fig. 4 Randomized benchmarking measurement.

Fig. 2 Transient modeling results.

Fig. 5 Predictions of the efficacy of sickling inhibitors with the kinetic model. Predictions of the efficacy of sickling inhibitors with the kinetic model.

Fig. 4 Relationships between light and economic parameters.

Fig. 1 Environmental conditions and concentrations of floating plastic debris in the Arctic Ocean. Environmental conditions and concentrations of floating.

Fig. 7 Global change in the collective mass for wild mammals, humans, cattle, and all livestock for the years 1900–2050. Global change in the collective.

Fig. 1 Fractional coverage of the mapping method used in this study.

Fig. 5 Collapsing an excision to become a puckered slit.

Fig. 1 Ultrafast electron calorimetry can measure the dynamic electron temperature and band structure to uncover a new long-lived metastable state mediated.

Fig. 4 Superconductivity gap and specific heat jump.

Experimental observation of dual magnetic states in topological insulators by Wenqing Liu, Yongbing Xu, Liang He, Gerrit van der Laan, Rong Zhang, and.

Fig. 4 Results of MIROC freshwater hosing simulations (0

Field-induced magnetic instability within a superconducting condensate

by Mark T. Edmonds, James L

Fig. 4 Optical properties of the modes guided in twisted coreless PCF.

Fig. 2 Comparison of the observed DRs and the estimates by the VR model and FL. Comparison of the observed DRs and the estimates by the VR model and FL.

Van der Waals engineering of ferromagnetic semiconductor heterostructures for spin and valleytronics by Ding Zhong, Kyle L. Seyler, Xiayu Linpeng, Ran.

Fig. 1 Charge manipulation and readout in diamond.

Fig. 4 Results from experiments with oscillating thermal circuits containing the equivalent of a thermal inductor. Results from experiments with oscillating.

Fig. 2 Particles detected in snow samples collected at different locations from Europe to the Arctic. Particles detected in snow samples collected at different.

Fig. 1 Schematic depiction of a paradigm for rapid and guided discovery of materials through iterative combination of ML with HiTp experimentation. Schematic.

Fig. 1 Sketch and schematic diagram of photobleaching reaction in a strongly coupled system. Sketch and schematic diagram of photobleaching reaction in.

Fig. 2 Observation of type II Weyl nodes in LaAlGe.

Fig. 2 Finite element method (FEM) simulations of the photonic synapse with different structures. Finite element method (FEM) simulations of the photonic.

Coexistence of superconductivity and ferromagnetism in EuFe2(As0. 79P0

Fig. 4 Relationship of plastic ingestion and nesting behavior.

Fig. 2 The working principle and electrical output modulating of BD-TENG by changing the materials of friction layers. The working principle and electrical.

Fig. 3 Global and basin-averaged sampling error compared with reconstructed temperature change. Global and basin-averaged sampling error compared with.

Fig. 1 Crystal structure of the MMOH-MMOD complex.

Fig. 2 Analysis of 1PCTCO2 experiments (JJA seasonal means).

Fig. 5 SEM images of pin and disc wear tests.

Fig. 5 Modeling of the ASE threshold using the kinetic equations and experimental parameter inputs. Modeling of the ASE threshold using the kinetic equations.

Presentation transcript:

Fig. 6 Global phase diagram. Global phase diagram. Electronic phase diagram of fcc RbxCs3−xC60 showing the evolution of Tc (ambient P: solid triangles, high P: unfilled triangles) and the MJTI-to-JTM crossover temperature, T′ (SXRPD: squares; χ(T): stars; 13C, 87Rb, and 133Cs NMR spectroscopy: hexagon with white, color, and black edges, respectively; IR spectroscopy: diamonds), as a function of V. Within the metallic (superconducting) regime, gradient shading from orange to green schematically illustrates the JTM to conventional metal (unconventional to weak-coupling BCS conventional superconductor) crossover. Dashed lines mark experimental V(T) tracks for selected compositions. Upper panels: Evolution of T1u(4) IR lineshape through conventional metal (Rb2CsC60, 30 K), JTM (Rb0.5Cs2.5C60, 37 K), and MJTI (Rb0.35Cs2.65C60,130 K), together with schematic depictions of the respective molecular electronic structure, intermolecular electron hopping, and JT molecular distortion. Lower panel: Variation in superconducting gap divided by Tc, 2Δ0/kBTc, with V. Ruth H. Zadik et al. Sci Adv 2015;1:e1500059 Copyright © 2015, The Authors