Entangled Light and Matter: Witnessing Polariton Dynamics in Real Time
![The dynamics of [latex] q^n(t) [/latex] are explored for values of <i>n</i> ranging from 1 to 8, demonstrating a range of behaviors despite the differing units inherent in these observables.](https://arxiv.org/html/2602.11335v1/x3.png)
New simulations reveal that initializing a cavity mode with a single photon unlocks observable light-matter entanglement and oscillating energy exchange in molecular polariton systems.
![The study of a QCD-like gauge-fermion theory-with three colors and three chiral flavors-reveals how a chiral order parameter [latex]\sigma_0(r)[/latex] evolves with spatial separation and temperature, transitioning from a symmetric phase at high temperatures to a precondensation regime-where the condensate exists only over finite length scales-and ultimately to a broken phase characterized by a macroscopic condensate at large distances, with the domain size ξ delineating the extent of precondensation and a UV length scale [latex]r_{UV}[/latex] marking its effective vanishing point.](https://arxiv.org/html/2602.11265v1/x1.png)
![The study delineates the bounds of applicability for critical function space estimations-specifically, for [latex]L^{q}(\mathbb{R}^{n})[/latex] potentials, Strichartz pairs [latex](r,p)[/latex], and the Stein-Tomas extension [latex]L^{2}(\mathbb{S}^{n-1})\to L^{p}(\mathbb{R}^{n})[/latex]-demonstrating that the Kenig-Ruiz-Sogge estimate holds for [latex]p\in[q\_{2},\in fty)[/latex] in two dimensions and [latex]p\in[q\_{n},p\_{n}][/latex] for higher dimensions, thereby establishing a nuanced understanding of their dimensional dependence.](https://arxiv.org/html/2602.12122v1/x3.png)
![The study demonstrates that alterations in the Kondo lattice temperature [latex]T_{K}[/latex]-induced by applied strain-directly modulate electrical resistance, manifesting as a sign change in temperature dependence and a positive elastoresistance under a magnetic field, thereby revealing the interplay between material properties and externally applied forces.](https://arxiv.org/html/2602.12141v1/Fig1.jpg)

![The scaling dimension [latex]\Delta\phi[/latex] is calculated across different [latex]\mathrm{Sp}(10)[/latex] and [latex]\mathrm{Sp}(4)[/latex] models using conformal 2-pt correlators [latex]\mathscr{C}_T[/latex], revealing its dependence on both [latex]\gamma_{12}[/latex] and [latex]R[/latex], and consistently approaching the expected value of [latex]\Delta_J = 2[/latex] while aligning with the critical point previously identified through crossing symmetry.](https://arxiv.org/html/2602.11255v1/x8.png)
![The Sondheimer frequency exhibits a clear dependence on doping concentration, transitioning predictably across the overdoped to underdoped regime under a perpendicular magnetic field-a relationship governed by parameters including a perpendicular transfer integral of [latex]3 \times 10^{-3} \text{eV}[/latex], zero phase shift [latex]\eta = 0[/latex], and a layer thickness ratio of [latex]d/a = 40[/latex].](https://arxiv.org/html/2602.11252v1/x6.png)