Using the crossover temperature T0, the coherence length along the c axis, ξc(0), was determined.

Features of Excess Conductivity Behavior in a Magnetic Superconductor Dy$_{0.6}$Y$_{0.4}$Rh$_{3.85}$Ru$_{0.15}$B$_4$

The crossover temperature T0 determines the coherence length along the c axis is ξc(0) = 0.

Effect of annealing on a pseudogap state in untwinned YBa2Cu3O7−δ single crystals

Inhibition of thermal activation was observed, leaving the macroscopic quantum tunneling as the dominant effect well beyond the crossover temperature.

Josephson Junctions as Single Microwave Photon Counters: Simulation and Characterization

Below TB in FC mode, the magnetization decreases with temperature until 36 K; this temperature is the crossover temperature TCr related to the anisotropy of the barriers, indicative of macroscopic quantum tunneling.

Macroscopic Quantum Tunneling in PdO Nanoparticles

Such a result questions the commonly applied ‘Stickel operator’ routine as the reliable tool for determining the dynamic crossover temperature.

Long-Range Static and Dynamic Previtreous Effects in Supercooled Squalene - Impact of Strong Electric Field

This result questions the commonly applied ‘Stickel operator’ routine as the most reliable tool for determining the dynamic crossover temperature.

Long-Range Static and Dynamic Previtreous Effects in Supercooled Squalene—Impact of Strong Electric Field

In absence of magnetic field, the addition of Ag in YBCO shift various crossover temperatures of paracoherent state and 3D fluctuations dominate the mean-field region.

Study on excess conductivity in YBCO + xAg composites

Investigations of dynamic relaxation are significant for understanding the nature of glasses, liquids, and the critical issues of glass formation and transition, dynamic and structural heterogeneities, flow behaviour and flow units, various crossover temperatures, deformations, aging and rejuvenation, stability, crystallization, and the mechanical and physical properties of glasses.

Dynamic relaxations and relaxation-property relationships in metallic glasses

Forward and inverse spin crossover temperatures are determined.

PHYSICOCHEMICAL STUDY OF SPIN CROSSOVER IN THE IRON(II) NAPHTHALENE-2-SULFONATE COMPLEX WITH 4-AMINO-1,2,4-TRIAZOLE

All tris(pyrazolyl)borate complexes retain the spin crossover properties of their parent compound, with spin crossover temperatures ranging from 350 to 430 K.

Amine‐Functionalized Spin Crossover Building Blocks

A size-dependent crossover temperature is found, above which the hydration of the alkanes is favored in the aqueous urea solution.

Effect of urea on the hydration and aggregation of hydrophobic and amphiphilic solute models: Implications to protein aggregation.

The term pseudogap denotes a suppression of the density of states between a doping-dependent crossover temperature, T * ( p ) , and the (lower) SC transition temperature, T c ( p ).

Linking the pseudogap in the cuprates with local symmetry breaking: A commentary

Finally, we provide an estimate of ξ as a function of T^{*}, finding a mild power law divergence, ξ∼(T^{*}-T_{d})^{-α/3}, with T_{d} the dynamical crossover temperature and α falling in the range α∈[0.

Relation between Heterogeneous Frozen Regions in Supercooled Liquids and Non-Debye Spectrum in the Corresponding Glasses.

Here we report a saturation of the electrical resistivity in Zr_{64}Ni_{36} and Cu_{50}Zr_{50} liquids above a dynamical crossover temperature for the viscosity (T_{A}).

Resistivity Saturation in Metallic Liquids Above a Dynamical Crossover Temperature Observed in Measurements Aboard the International Space Station.

The thermal widths grow rapidly above the chiral crossover temperature Tcp, indicating the dissociation of mesons at high temperatures.

Thermal properties of light mesons from holography

Properties of QCD matter change significantly around the chiral crossover temperature, and the effects on $U(1)_A$ and topological susceptibilities, as well as the meson spectrum have been studied with much care.

Symmetries of the light hadron spectrum in high temperature QCD.

Different from Cu75Ag25 and Cu25Ag75 melts of which the crossover temperature T c is below the liquidus temperature, the T c of Cu54.

Abnormal dynamic behavior and structural origin of Cu-Ag eutectic melt

At vanishing chemical potential, we report a crossover temperature T c ( 0 ) = ( 156.

The QCD crossover at zero and non-zero baryon densities from Lattice QCD

We find that the abrupt deviation from the Fermi liquid behavior in the electron self-energy results in the kink feature at low energy scale and that the kink is directly related to the coherence-incoherence crossover temperature scale.

Direct observation of kink evolution due to Hund’s coupling on approach to metal-insulator transition in NiS2−xSex

The crossover temperature scales as $q_0^3$, where $q_0$ is the minimal wavevector for umklapp scattering.

Scattering mechanisms and electrical transport near an Ising nematic quantum critical point

The crossover temperature increases with NPs size, suggesting a size-dependent blocking magnetic regime.

Control of Multiferroic properties in BiFeO3 nanoparticles

The crossover temperature increases with increasing pressure.

Density and Volumetric Properties of Binary Mixtures of CO2 + Hexadecane from (303.2 to 473.2) K and Pressures up to 50.0 MPa

Using the crossover temperature T0, the coherence length along the c axis, ξc(0), was determined.

Features of Excess Conductivity Behavior in a Magnetic Superconductor Dy$_{0.6}$Y$_{0.4}$Rh$_{3.85}$Ru$_{0.15}$B$_4$

The crossover temperature T0 determines the coherence length along the c axis is ξc(0) = 0.

Effect of annealing on a pseudogap state in untwinned YBa2Cu3O7−δ single crystals

In a supercooled liquid, the crossover temperature T_{c} separates a high-temperature region of diffusive dynamics from a low-temperature region of activated dynamics.

Jump-precursor state emerges below the crossover temperature in supercooled o-terphenyl.

We also show how the parameter ψ(T) that measures the role of fluctuations embedded in the system on size of the cooperatively reorganizing cluster (CRC) and the crossover temperature T_{a} depend on the intermolecular interactions.

How attractive and repulsive interactions affect structure ordering and dynamics of glass-forming liquids.

10.1016/j.nuclphysa.2020.121782

We present the continuum extrapolation of the crossover temperature based on different observables at several lattice spacings.

The crossover line in the (T, μ)-phase diagram of QCD

We also suggest a simple theoretical model to describe the tunneling effects in the vicinity of the crossover temperature (the temperature where tunneling becomes the dominating mechanism).

Entanglement Effect and Angular Momentum Conservation in a Nonseparable Tunneling Treatment.

10.1016/j.applthermaleng.2020.116489

Based on the results, the combustion mode changes, which implies a transition from the surface to the submerged combustion mode of the PMB, and were directly compared with the crossover temperature.

Characteristics of large-area porous media burner applicable to direct-fired non-oxidizing annealing furnace

The evidence provided here for the onset of cooperativity, marked by a crossover temperature, TA (which is usually above the liquidus temperature), is accompanied by the onset of development of more spatially extended structural order in the liquids.

Breakdown of the Stokes-Einstein relationship and rapid structural ordering in CuZrAl metallic glass-forming liquids.

Different from the commonly used maximum change in chiral condensate, we propose defining the crossover temperature using the Mott transition of pseudo-Goldstone bosons, which, by definition, guarantees Goldstone's theorem.

Chiral crossover characterized by Mott transition at finite temperature * * Supported by the NSFC (11775165)

10.1103/PhysRevE.103.L050601

In a supercooled liquid, the crossover temperature T_{c} separates a high-temperature region of diffusive dynamics from a low-temperature region of activated dynamics.

Jump-precursor state emerges below the crossover temperature in supercooled o-terphenyl.

10.1021/acs.inorgchem.0c03593

The series spans a broad range of spin-crossover temperatures (T1/2) for the LS ⇌ HS equilibrium in solution, with the exception of compound 6 which remains high-spin (S = 2) down to 210 K.

Widening the Window of Spin-Crossover Temperatures in Bis(formazanate)iron(II) Complexes via Steric and Noncovalent Interactions

10.1016/J.PHYSB.2021.412860

The crossover temperature between the intervals is in the range 20–30 K.

Universal temperature corrections to the conductivity of niobium-carbon nanocomposites

Hence, present investigation was targeted to evaluate the changes taking place in heat stability, ζ-potential, particle size, apparent viscosity, pH, turbidity and crossover temperature of storage (G′) and loss (G″) modulus of high-protein BSM based UF retentates as a function of homogenization and sodium hydrogen phosphate (SHP) addition.

Homogenization and sodium hydrogen phosphate induced effect on physical and rheological properties of ultrafilterd concentrated milk

10.1140/epjb/s10051-020-00041-3

For finite-size systems, it is found that a crossover temperature can be used to characterize the transition to a single-domain-type magnet.

Kinematic interaction and condensation factor in two-dimensional quantum Heisenberg ferromagnet

We also discuss that one has to be careful in analyzing the crossover temperature from the positive to negative magnetoresistance.

Intervalley Tunneling and Crossover from the Positive to Negative Interlayer Magnetoresistance in Quasi-Two-Dimensional Dirac Fermion System with or without Mass Gap

10.1021/acs.jpclett.0c03626

Mimicking experimental conditions, our enhanced-sampling atomistic simulations of CI2 surrounded by lysozyme and bovine serum albumin reproduce this destabilization but also provide evidence of a crossover temperature above which lysozyme is found to become stabilizing, as previously predicted by analysis of thermodynamic data.

Stabilizing or Destabilizing: Simulations of Chymotrypsin Inhibitor 2 under Crowding Reveal Existence of a Crossover Temperature.

As temperature emerges, the TLL phase is crossover into QC regimes with a crossover temperature connecting to a universal linear line T*∼|θ-θc1,2| that ends at θc1,2 upon cooling down to 0K, providing a new clue to capture QCP.

A quantum correlation test of quantum criticality in transverse-field Ising chain with Dzyaloshinskii-Moriya interaction

Our principal focus is on changes of topology of the phase diagram of confined water and establishing trends of behavior of the crossover temperature between condensation and evaporation on the strength of water-graphite interaction potential.

Phase behavior of water-like models in nanoscopic pores of slit shape. Predictions from a density functional theory

10.1016/J.ACTAMAT.2021.116705

Different from Cu75Ag25 and Cu25Ag75 melts of which the crossover temperature T c is below the liquidus temperature, the T c of Cu54.

Abnormal dynamic behavior and structural origin of Cu-Ag eutectic melt

These binder rheological indices included the Superpave intermediate-temperature PG (PGI), the Glover-Rowe (G-R) parameter, the crossover temperature (Tδ = 45°), the rheological index (R-value), and ΔTc.

Relationship between Rheological Indices and Cracking Performance of Virgin, Recycled, and Rejuvenated Asphalt Binders and Mixtures

10.1103/PhysRevE.103.052105

We also show how the parameter ψ(T) that measures the role of fluctuations embedded in the system on size of the cooperatively reorganizing cluster (CRC) and the crossover temperature T_{a} depend on the intermolecular interactions.

How attractive and repulsive interactions affect structure ordering and dynamics of glass-forming liquids.

These two ordering processes show a collapsed time evolution at the crossover temperature consistent with the onset of the theoretical deviation.

Crystal growth in deeply undercooled Ni50Al50: Signature of the ordering sequence at the interface.

10.1016/J.COMBUSTFLAME.2020.12.006

Results show that increasing methanol in a blend promotes reactivity at high temperatures and inhibits it at low temperatures, with the crossover temperature occurring at approximately 970–980 K with it being almost independent of pressure.

Understanding the antagonistic effect of methanol as a component in surrogate fuel models: A case study of methanol/n-heptane mixtures

10.1140/EPJB/E2019-100063-8

A transition from the 2D to the 3D region was observed in different fields at a crossover temperature as the temperature increased.

Excess conductivity in nano-carbon doped MgB2 superconductor

10.1016/J.CONBUILDMAT.2019.03.017

The performance improvement was reflected in BMS having lower viscosities, stiffnesses, shear susceptibilities, crossover temperatures, while having higher m-values and failure strains compared to RAS asphalt.

Durability of bio-modified recycled asphalt shingles exposed to oxidation aging and extended sub-zero conditioning

A remarkably strong variation in the crossover temperature and the lifetime of the skyrmion is found as a function of the values of parameters in the extended Heisenberg Hamiltonian, i.

Magnetic Skyrmion Annihilation by Quantum Mechanical Tunneling.

Crossover temperature from 2D to 3D (TLD) decreased in the mean-field region as a resultant dominance of 3D region by increasing of Ag in YBCO matrix.

Conductivity Fluctuation and Some Parameters of High temperature Superconductor Polycrystalline Y 1 Ba 2 Cu 3 O 7−δ doped with Silver Nanoparticles

10.1140/epjc/s10052-020-8243-9

We find that a relatively strong increase of diffusion coefficient from crossover temperature $T_c$ toward high temperature is preferred by data.

Data-driven extraction of heavy quark diffusion in quark-gluon plasma

As a result, a predicted dynamic change at a specific temperature (crossover temperature) is evidenced by a derivative-based representation of the relaxation time data.

Evidence for a dynamics crossover and its implication on the freezing temperature determination of relaxor ferroelectrics

10.1080/14680629.2019.1589559

Moreover, two parameters, crossover temperature, Tδ=45°, and the difference in critical temperature, ΔTc, were used to evaluate the aging properties of the materials.

Investigation on the combined effect of aging temperatures and cooling medium on rheological properties of asphalt binder based on DSR and BBR

10.1021/acs.inorgchem.9b01356

We also elucidate that the as-synthesized sample with Co enrichment at the Td site shows the better OER activity, and the optimum annealing temperature for more OER active Ca2FeCoO5 should be higher than the crossover temperature.

Transition-Metal Distribution in Brownmillerite Ca2FeCoO5.

The crossover temperature scales as $q_0^3$, where $q_0$ is the minimal wavevector for umklapp scattering.

Scattering mechanisms and electrical transport near an Ising nematic quantum critical point

Our results revealed an increase of the crossover temperature from circa 35 °C at pH 3.

pH dependence of water anomaly temperature investigated by Eu(III) cryptate luminescence

3Tg, which may correspond to the crossover temperature (TB) related to the variation in molecular dynamics, a maximum in.

Studying the Crystal Growth of Selected Active Pharmaceutical Ingredients from Single- and Two-Component Systems above and below the Glass Transition Temperature

10.1103/PhysRevB.100.245126

We have discovered a reentrance effect of the Hall-driven sliding above a crossover temperature at which the Hall constant has been known to change signs.

Charge density wave sliding driven by an interplay of conventional and Hall voltages in NbSe 3 microbridges

We also report evidence from electron and x-ray diffraction which suggests a tendency toward short-range ordering along both wavevectors which persists even well above the crossover temperature.

Suppression of charge density wave order by disorder in Pd-intercalated ErTe 3

10.1103/PhysRevD.101.074511

In the vicinity of the crossover temperature at zero chemical potential, the radius of convergence turns out to be at $\mu_B/T \approx 2$ and roughly temperature independent.

Radius of convergence in lattice QCD at finite $\mu_B$

The crossover temperature increases with NPs size, suggesting a size-dependent blocking magnetic regime.

Control of Multiferroic properties in BiFeO3 nanoparticles

For all microgel sample variants, a crossover temperature, where the elastic contribution to osmotic pressure changes sign, is found to approximate the final temperature after microgel synthesis and also to the free polymer θ temperature.

Structural parameters of soft PNIPAM microgel particles as a function of crosslink density.

In ${\mathrm{RbFe}}_{2}{\mathrm{As}}_{2}$ around 35 K, far below that crossover temperature, we observe a peak in the NQR $1/{T}_{1}$ which is possibly associated with the critical slowing down of electronic nematic fluctuations on approaching the transition to the nematic long-range order.

Charge and nematic orders in A Fe 2 As 2 ( A = Rb , Cs ) superconductors

The storage modulus (G′) and loss modulus (G″) crossover temperature of UF and DF retentates were ~ 57.

Effect of change in pH, heat treatment and diafiltration on properties of medium protein buffalo milk protein concentrate

This link is made using a rheological aging index (RAI), the crossover temperature and a chemical aging index (CAI).

Impact of asphalt aging temperature on chemo-mechanics

10.4028/WWW.SCIENTIFIC.NET/MSF.966.404

With light irradiation, the crossover temperature from one-dimensional to three-dimensional of regio-regular P3HT and ZnO nanoparticles bulk sample was obtained at lower temperature of 10 K compared to previous result at 25 K without light irradiation.

μSR Study with Light Irradiation of P3HT:ZnO Nanoparticles as Active Material of Hybrid Solar Cells

10.1016/J.PHYSB.2019.07.020

This theory allows us to determine the crossover temperatures and the dominant instability as a function of U and V.

Spin and charge fluctuations in a one-dimensional lattice with long-range interactions

10.1016/j.actamat.2019.03.009

We find that the temperature dependence of critical size of the crystalline nuclei contains two distinguishable regimes with the crossover temperature T / T g ≈ 1.

Structure and morphology of crystalline nuclei arising in a crystallizing liquid metallic film

Aging characteristics such as the Gaestel index, sulfoxide and carbonyl indexes, linear viscoelastic strain range, crossover temperature, and Glover–Rowe parameter were analysed for laboratory aged and naturally aged neat and polymer-modified bitumen.

Effect of Aging on Chemical Composition and Rheological Properties of Neat and Modified Bitumen

10.1016/j.combustflame.2020.03.002

Attention is focused on high degrees of dilution, resulting in near-limit flames, with peak temperatures close to the crossover temperature.

Near-limit H2-O2-N2 combustion in nonpremixed counterflow mixing layers

10.1016/J.ACTAMAT.2019.05.057

At a crossover temperature, well below the melting point, we find that the supercooled phase exhibits glassy dynamics which includes a breakdown of the Stokes-Einstein relation and the emergence of spatially heterogeneous dynamics.

Nucleation kinetics in a supercooled metallic glass former

Keywords related to Temperature

Crossover Temperature
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