2018/12/12 by Jonas Wätzel, Jamal Berakdar · 7 citations
Materials Science · Physics and Astronomy · #Generator (circuit theory) #Laser #Materials science #Mechanical and Optical Resonators #Metamaterials and Metasurfaces Applications #Nanoscopic scale #Nanotechnology #Nuclear physics #Optics #Orbital Angular Momentum in Optics #Phase (matter) #Physics #Power (physics) #Swift #Thermodynamics #Toroid #Ultrashort pulse #cond-mat.mes-hall #quant-ph
paper · pdf · doi:10.1002/qute.201800096
published in Advanced Quantum Technologies 2(1-2) (Wiley) · 9 pages, 10 figures
arxiv created 2018/12/12 · openalex created_date 2018/12/22 · openalex publication_date 2018/12/28 · arxiv updated 2019/01/01 · openalex updated_date 2026/08/05
Abstract Efficient and flexible schemes for a swift, field‐free control of the phase in quantum devices have far‐reaching impact on energy‐saving operation of quantum computing, data storage, and sensoring nanodevices. A novel approach for an ultrafast generation of a field‐free vector potential that is tunable in duration, sign, and magnitude, allowing to impart non‐invasive, spatiotemporally controlled changes to the quantum nature of nanosystems is reported. The method relies on triggering a steady‐state toroidal moment in a donut‐shaped nanostructure that serves as a vector‐potential generator and quantum phase modulator. Irradiated by moderately intense, few cycle THz pulses with appropriately shaped polarization states, the nano donut is brought to a steady‐state where a nearby object does not experience electric or magnetic fields but feels the photo‐generated vector potential. Designing the time structure of the driving THz pulses allows for launching picosecond trains of vector potentials which is the key for a contact‐free optimal control of quantum coherent states. This research can trigger a new class of ultrafast quantum devices operated and switched in an energy‐efficient, contact and field‐free manner, enabling new techniques for use in quantum information, magnetic nanostructures, and superconducting tunnel junctions as well as in toroidally ordered systems and multiferroics.