## It is shown that the critical end point (CEP) linking the crossover transition with the first-order phase transition still exists and locates at $(\mu_B, T_c) \simeq (390 MeV, 145 MeV)$.

A consistent analysis on QCD phase diagram and meson spectra in the improved soft-wall AdS/QCD

## With the increase of the chemical potential $\mu$, the critical temperature $T_c$ descends towards zero, and the crossover transition turns into a first-order one at some intermediate value of $\mu$, which implies that a critical end point naturally exists in this improved soft-wall model.

Chiral phase transition and QCD phase diagram from AdS/QCD

## We show that when using the set of parameters thus determined, the second order phase transition line (our proxy for the crossover transition) that starts at finite temperature and zero baryon chemical potential converges to the line of first order phase transitions that starts at zero temperature and finite baryon chemical potential to determine the critical end point to lie in the region 5.

On the critical end point in a two-flavor linear sigma model coupled to quarks

## Studies with unimproved actions found the existence of a critical quark mass value at which the crossover transition ends on a second order phase transition and becomes first order for smaller values of the quark mass for the case of both vanishing and imaginary chemical potential.

Critical end points in (2+1)-flavor QCD with imaginary chemical potential

## We find that the critical endpoint linking the crossover transition with the first-order phase transition still exists and locates at (μB,Tc)≃(390  MeV,145  MeV), which along with the crossover line are consistent with lattice result and experimental analysis from relativistic heavy ion collisions.

Octet meson spectra and chiral phase diagram in the improved soft-wall AdS/QCD model

## Film thickness and microstructure critically affect the spin crossover transition of a 2D coordination polymer.

Effect of nanostructuration on the spin crossover transition in crystalline ultrathin films† †Electronic supplementary information (ESI) available: Materials and methods, supplementary figures and tables. See DOI: 10.1039/c8sc04935a

## Specifically, the addition of benzimidazole results in a re-entrant spin crossover transition, i.

Manipulation of the molecular spin crossover transition of Fe(H2B(pz)2)2(bipy) by addition of polar molecules.

10.1007/s11696-019-00781-2

## The variable-temperature EPR measurement confirmed a gradual spin-crossover transition (S = 5/2 ↔ S = 1/2).

A variable-temperature Q- and X-band EPR study of spin-crossover iron(III) Schiff base complex

## Lattice simulations indicate that EWSB in the Standard Model (SM) occurs through a crossover transition, while the presence of new physics beyond the SM could alter this thermal history.

The Electroweak Phase Transition: A Collider Target.

10.1021/acs.analchem.9b01416

## Above the crossover transition, Rmax, per dsDNA molecule dropped rapidly as f-1/2 towards a planarlike monolayer.

Electrochemical Characteristics of DNA Modified Electrode as a Function of Percent Binding.

10.1016/J.PHYSLETB.2019.04.023

## The impact of first order and crossover transitions is also examined.

Fourier coefficients of the net baryon number density and their scaling properties near a phase transition

## In this contribution, we discuss the mapping of the black hole model in the QCD phase diagram and show that the crossover transition, between hadrons and the quark-gluon plasma, ends in a critical point where a first order line begins.

QCD Phase Diagram with a Critical Point from Holography

## The chiral transition behaviors are investigated in the improved soft-wall AdS/QCD model with the solved gravitational background, and the crossover transition can be realized.

Equation of state and chiral transition in soft-wall AdS/QCD with a more realistic gravitational background

10.1103/PHYSREVC.100.054310

## Conclusions: The observation of crossover transitions positioned the isomeric high-spin level of $^{198}$At at an excitation energy of 265(3) keV.

$\alpha$-decay properties of $^{200,202}$FR

10.1038/s41598-019-41337-4

## A pressure-induced metallization along with a Co2+ high-spin (S = 3/2) to low-spin (S = 1/2) crossover transition is observed at high pressure near 70 GPa.

Pressure-induced spin transition and site-selective metallization in CoCl2

10.1007/s11224-019-01463-1

## The studied compounds are shown to be capable of undergoing thermally initiated stepwise or synchronized spin-crossover transitions, in particular involving all the electromeric forms.

Heterospin magnetically active bimetallic Fe and Co complexes of aldiminato-functionalized catechol: a DFT study

10.1103/PHYSREVD.100.114040

## The collision energy dependent buildup of the 2D percolation clusters defines the temperature range $159\ifmmode\pm\else\textpm\fi{}9\text{ }\text{ }\mathrm{MeV}$ of the crossover transition between hadrons to the QGP in reasonable agreement with the lattice quantum chromodynamics (LQCD) pseudocritical temperature value of $155\ifmmode\pm\else\textpm\fi{}9\text{ }\text{ }\mathrm{MeV}$.

Exploring the initial stage of high multiplicity proton-proton collisions by determining the initial temperature of the quark-gluon plasma