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Tailoring energy levels in quantum systems via Hamiltonian control parameters is essential for designing quantum thermodynamic devices and materials. However, conventional approaches to manipulating finite-size quantum systems, such as tuning external fields or system size, typically lead to uniform shifts across the spectrum, limiting the scope of spectral engineering. A recently introduced technique, known as the size-invariant shape transformation, overcomes this limitation by introducing a new control parameter that deforms the potential landscape without altering the system's size parameters, thereby enabling nonuniform scaling of energy levels. This new degree of freedom-referred to as the shape parameter-gives rise to quantum shape effects in the thermodynamics of confined systems, which are conceptually distinct from quantum size effects. Here, we explore the fundamental limits of nonuniform level scaling in the spectra by asking: what is the minimal quantum system in which such behavior can arise? We demonstrate that even a two-level system can exhibit the thermodynamic consequences of quantum shape effects, including spontaneous transitions into lower-entropy states, a phenomenon absent in classical thermodynamics for noninteracting systems. We identify the spectral origin of these unconventional thermodynamic behaviors as geometry-induced asymmetric level coupling, in which the ground-state energy and energy gap respond in opposite ways to changes in a shape parameter. This asymmetry naturally extends to many-level systems, where the thermally averaged energy spacing and ground-state energy evolve in opposite directions. To characterize unconventional thermodynamic behaviors, we construct thermodynamic spontaneity maps, identifying regions of energy-driven and entropy-driven spontaneous processes in ground-state energy versus energy gap space. These effects emerge under quasistatic, isothermal changes of a shape degree of freedom and illustrate how the confinement geometry alone can enable unconventional thermodynamic behaviors that are otherwise exclusive to interacting or open systems. We argue that any scaling-invariant local parameter transformation that induces asymmetric-level coupling can be used to engineer similar responses, making this a broadly applicable framework. Our results deepen the theoretical foundations of the quantum shape effect and introduce a route to spectral gap control, with potential applications in isolating computational subspaces within quantum information platforms.
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http://dx.doi.org/10.1103/hpkh-n3kv | DOI Listing |
Light Sci Appl
September 2025
National Laboratory of Solid State Microstructures, Key Laboratory of Intelligent Optical Sensing and Manipulation, College of Engineering and Applied Sciences, Nanjing University, 210023, Nanjing, China.
Planar optical elements incorporating space-varying Pancharatnam-Berry phase have revolutionized the manipulation of light fields by enabling continuous control over amplitude, phase, and polarization. While previous research focusing on linear functionalities using apolar liquid crystals (LCs) has attracted much attention, extending this concept to the nonlinear regime offers unprecedented opportunities for advanced optical processing. Here, we demonstrate the reconfigurable nonlinear Pancharatnam-Berry LC diffractive optics in photopatterned ion-doped ferroelectric nematics.
View Article and Find Full Text PDFPhys Rev Lett
August 2025
University of Southern Denmark, Centre for Nano Optics, Campusvej 55, Odense M DK-5230, Denmark.
Controlling the spontaneous emission of nanoscale quantum emitters (QEs) is crucial for developing advanced photon sources required in many areas of modern nanophotonics, including quantum information technologies. Conventional approaches to shaping photon emission are based on using bulky configurations, while approaches recently developed in quantum metaphotonics suffer from limited capabilities in achieving desired polarization states and directionality, failing to provide on-demand photon sources tailored precisely to technological needs. Here, we propose a universal approach to designing versatile photon sources using on-chip QE-coupled meta-optics that enable direct transformations of QE-excited surface plasmon polaritons into spatially propagating photon streams with arbitrary polarization states, directionality, and amplitudes via both resonance and geometric phases supplied by scattering meta-atoms.
View Article and Find Full Text PDFNano Lett
September 2025
School of Materials Science and Engineering, Peking University, Beijing 100871, People's Republic of China.
High-density mirror twin boundaries (MTBs) embedded in two-dimensional (2D) transition metal dichalcogenides (TMDCs) have emerged as fascinating platforms for exploring charge density wave and Tomonaga-Luttinger liquid-related issues. However, the reversible manipulation of high-density MTBs in 2D TMDCs remains challenging. Herein, we report the first fabrication of high-density MTB loops in ultrathin 1T-NiTe on the SrTiO(001) substrate, by postannealing as-grown 1T-NiTe under Te-deficient conditions.
View Article and Find Full Text PDFJ Phys Condens Matter
September 2025
Department of Physics, Temple University, Barton Hall, Philadelphia, PA 19122-6082, USA, Philadelphiaa, Pennsylvania, 19122, UNITED STATES.
We examine the magnetic excitations of an Anderson lattice model with a Vshaped pseudogap arising from nodal hybridization. The model produces a V-shaped pseudogap in the electronic density of states near the Fermi energy. It lies close to an antiferromagnetic quantum critical point and features lowdimensional Fermi surfaces, aligning with experimental observations of CeNiSn.
View Article and Find Full Text PDFACS Appl Mater Interfaces
September 2025
L. V. Pisarzhevsky Institute of Physical Chemistry of NASU SE "RADMA", 31, pr. Nauky ave, Kyiv 03680, Ukraine.
The effect of electron irradiation ( = 1.8 MeV) on the optical properties of polyethylene glycol 400-multiwalled carbon nanotube (PEG-400/MWCNT) nanocomposite films was studied within an absorbed dose range of 0 to 0.4 MGy.
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