Abstract:Quantum entanglement is a fundamental phenomenon which, on the one hand, reveals deep connections between quantum mechanics, gravity and the space-time [1, 2]; on the other hand, has practical applications as a key resource in quantum information processing [3]. While it is routinely achieved in photon-atom ensembles [4], entanglement involving the solid-state [5-7] or macroscopic objects [8] remains challenging albeit promising for both fundamental physics and technological applications. Here, we report entan… Show more
“…We have observed a set of three replica luminescent peaks at ~21.4 meV below the dark exciton and exciton-polarons (or trions) in the negatively and positively charged Fermi sea. The redshift energy (21.4 meV) matches the energy of the zone-center E" chiral phonons in monolayer WSe2 [37][38][39]. The replica emission exhibits parallel gating dependence and the same g-factors as the dark excitonic states, but follows distinct optical selection rules.…”
mentioning
confidence: 61%
“…Furthermore, recent research shows that coherent dark exciton can be formed between two valleys [27]. A valley-coherent dark exciton can decay into a pair of photon and phonon with entangled chirality, as reported for quantum-dot excitons in monolayer WSe2 [37] (see Supplementary Materials [40]). Such entanglement functionality, together with the long and detectable valley polarization of the dark excitonic states and replicas, shall open a new venue for fundamental exciton research and novel valleytronic applications.…”
Monolayer WSe2 hosts long-lived dark excitonic states with robust valley polarization, but thus far lacks an experimental signature to identify their valley pseudospin. Here we reveal a set of three replica luminescent peaks at ~21.4 meV below the dark exciton, negative and positive dark exciton-polarons (or trions) in monolayer WSe2. The redshift energy matches the energy of the zone-center E" chiral phonons. The replicas exhibit parallel gate dependence and the same g-factors as the dark excitonic states, but follow the valley selection rules of bright excitonic states. While the dark states exhibit out-of-plane transition dipole and linearly polarized emission in the in-plane directions, their phonon replicas exhibit in-plane transition dipole and circularly polarized emission in the out-ofplane directions. Symmetry analysis shows that the K-valley dark exciton decays into a left-handed chiral phonon and a right-handed photon, whereas the K'-valley dark exciton decays into a right-handed phonon and a left-handed photon. Such chiral-phonon replicas can help identify the dark-state valley pseudospin and explore the intriguing excitonphonon interactions in monolayer WSe2.
“…We have observed a set of three replica luminescent peaks at ~21.4 meV below the dark exciton and exciton-polarons (or trions) in the negatively and positively charged Fermi sea. The redshift energy (21.4 meV) matches the energy of the zone-center E" chiral phonons in monolayer WSe2 [37][38][39]. The replica emission exhibits parallel gating dependence and the same g-factors as the dark excitonic states, but follows distinct optical selection rules.…”
mentioning
confidence: 61%
“…Furthermore, recent research shows that coherent dark exciton can be formed between two valleys [27]. A valley-coherent dark exciton can decay into a pair of photon and phonon with entangled chirality, as reported for quantum-dot excitons in monolayer WSe2 [37] (see Supplementary Materials [40]). Such entanglement functionality, together with the long and detectable valley polarization of the dark excitonic states and replicas, shall open a new venue for fundamental exciton research and novel valleytronic applications.…”
Monolayer WSe2 hosts long-lived dark excitonic states with robust valley polarization, but thus far lacks an experimental signature to identify their valley pseudospin. Here we reveal a set of three replica luminescent peaks at ~21.4 meV below the dark exciton, negative and positive dark exciton-polarons (or trions) in monolayer WSe2. The redshift energy matches the energy of the zone-center E" chiral phonons. The replicas exhibit parallel gate dependence and the same g-factors as the dark excitonic states, but follow the valley selection rules of bright excitonic states. While the dark states exhibit out-of-plane transition dipole and linearly polarized emission in the in-plane directions, their phonon replicas exhibit in-plane transition dipole and circularly polarized emission in the out-ofplane directions. Symmetry analysis shows that the K-valley dark exciton decays into a left-handed chiral phonon and a right-handed photon, whereas the K'-valley dark exciton decays into a right-handed phonon and a left-handed photon. Such chiral-phonon replicas can help identify the dark-state valley pseudospin and explore the intriguing excitonphonon interactions in monolayer WSe2.
“…In addition, the single photon emission has been realized with several approaches, such as heterostructures driven electrically [13], nanoscale strain engineering [14][15][16][17] and sub-nm focused helium ion irradiation [18], which are mostly defect related. Meanwhile, the properties of such a 2D host of quantum emitters have been intensely investigated, including 3D localized trions in heterostuctures [19], manipulation of fine structure splitting (FSS) [20] and photon-phonon interaction [21]. Furthermore, the optical initialization of a single spin-valley in charged WSe 2 quantum dots [22] and the ability to deterministically load either a single electron or single hole into a Van der Waals heterostructure quantum device via a Coulomb blockade [23] have been demonstrated, which enable a new class of quantum-confined spin system to store and process information.…”
Monolayer transition metal dichalcogenides have recently attracted great interests because the quantum dots embedded in monolayer can serve as optically active single photon emitters. Here, we provide an interpretation of the recombination mechanisms of these quantum emitters through polarization-resolved and magneto-optical spectroscopy at low temperature. Three types of defect-related quantum emitters in monolayer tungsten diselenide (WSe 2 ) are observed, with different exciton g factors of 2.02, 9.36 and unobservable Zeeman shift, respectively. The various magnetic response of the spatially localized excitons strongly indicate that the radiative recombination stems from the different transitions between defect-induced energy levels, valance and conduction bands. Furthermore, the different g factors and zerofield splittings of the three types of emitters strongly show that quantum dots embedded in monolayer have various types of confining potentials for localized excitons, resulting in electron-hole exchange interaction with a range of values in the presence of anisotropy. Our work further sheds light on the recombination mechanisms of defect-related quantum emitters and paves a way toward understanding the role of defects in single photon emitters in atomically thin semiconductors. * xlxu@iphy.ac.cn arXiv:2002.03526v1 [cond-mat.mes-hall]
“…This gives rise to potential applications in valleytronics and phononâchiralityâbased phononics . In quantum dots of WSe 2 , the entanglement between chiral phonons and optical excitation have also been reported very recently …”
The discovery of graphene has stimulated the search for and investigations into other 2D materials because of the rich physics and unusual properties exhibited by many of these layered materials. Transition metal dichalcogenides (TMDs), black phosphorus, and SnSe among many others, have emerged to show highly tunable physical and chemical properties that can be exploited in a whole host of promising applications. Alongside the novel electronic and optical properties of such 2D semiconductors, their thermal transport properties have also attracted substantial attention. Here, a comprehensive review of the unique thermal transport properties of various emerging 2D semiconductors is provided, including TMDs, blackâ and blueâphosphorene among others, and the different mechanisms underlying their thermal conductivity characteristics. The focus is placed on the phononârelated phenomena and issues encountered in various applications based on 2D semiconductor materials and their heterostructures, including thermoelectric power generation and electronâphonon coupling effect in photoelectric and thermal transistor devices. A thorough understanding of phonon transport physics in 2D semiconductor materials to inform thermal management of nextâgeneration nanoelectronic devices is comprehensively presented along with strategies for controlling heat energy transport and conversion.
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