GSTDTAP

浏览/检索结果: 共4条,第1-4条 帮助

已选(0)清除 条数/页:   排序方式:
Performance-limiting nanoscale trap clusters at grain junctions in halide perovskites 期刊论文
NATURE, 2020, 580 (7803) : 360-+
作者:  van den Brink, Susanne C.;  Alemany, Anna;  van Batenburg, Vincent;  Moris, Naomi;  Blotenburg, Marloes;  Vivie, Judith;  Baillie-Johnson, Peter;  Nichols, Jennifer;  Sonnen, Katharina F.;  Arias, Alfonso;  van Oudenaarden, Alexander
收藏  |  浏览/下载:27/0  |  提交时间:2020/07/03

Halide perovskite materials have promising performance characteristics for low-cost optoelectronic applications. Photovoltaic devices fabricated from perovskite absorbers have reached power conversion efficiencies above 25 per cent in single-junction devices and 28 per cent in tandem devices(1,2). This strong performance (albeit below the practical limits of about 30 per cent and 35 per cent, respectively(3)) is surprising in thin films processed from solution at low-temperature, a method that generally produces abundant crystalline defects(4). Although point defects often induce only shallow electronic states in the perovskite bandgap that do not affect performance(5), perovskite devices still have many states deep within the bandgap that trap charge carriers and cause them to recombine non-radiatively. These deep trap states thus induce local variations in photoluminescence and limit the device performance(6). The origin and distribution of these trap states are unknown, but they have been associated with light-induced halide segregation in mixed-halide perovskite compositions(7) and with local strain(8), both of which make devices less stable(9). Here we use photoemission electron microscopy to image the trap distribution in state-of-the-art halide perovskite films. Instead of a relatively uniform distribution within regions of poor photoluminescence efficiency, we observe discrete, nanoscale trap clusters. By correlating microscopy measurements with scanning electron analytical techniques, we find that these trap clusters appear at the interfaces between crystallographically and compositionally distinct entities. Finally, by generating time-resolved photoemission sequences of the photo-excited carrier trapping process(10,11), we reveal a hole-trapping character with the kinetics limited by diffusion of holes to the local trap clusters. Our approach shows that managing structure and composition on the nanoscale will be essential for optimal performance of halide perovskite devices.


  
Observation of the Kondo screening cloud 期刊论文
NATURE, 2020, 579 (7798) : 210-+
作者:  Shahnawaz, Mohammad;  Mukherjee, Abhisek;  Pritzkow, Sandra;  Mendez, Nicolas;  Rabadia, Prakruti;  Liu, Xiangan;  Hu, Bo;  Schmeichel, Ann;  Singer, Wolfgang;  Wu, Gang;  Tsai, Ah-Lim;  Shirani, Hamid;  Nilsson, K. Peter R.;  Low, Phillip A.;  Soto, Claudio
收藏  |  浏览/下载:11/0  |  提交时间:2020/07/03

When a magnetic impurity exists in a metal, conduction electrons form a spin cloud that screens the impurity spin. This basic phenomenon is called the Kondo effect(1,2). Unlike electric-charge screening, the spin-screening cloud(3-6) occurs quantum coherently, forming spin-singlet entanglement with the impurity. Although the spins interact locally around the impurity, the Kondo cloud can theoretically spread out over several micrometres. The cloud has not so far been detected, and so its physical existence-a fundamental aspect of the Kondo effect-remains controversial(7,8). Here we present experimental evidence of a Kondo cloud extending over a length of micrometres, comparable to the theoretical length xi(K). In our device, a Kondo impurity is formed in a quantum dot(2,9-11), coupling on one side to a quasi-one-dimensional channel(12) that houses a Fabry-Perot interferometer of various gate-defined lengths L exceeding one micrometre. When we sweep a voltage on the interferometer end gate-separated by L from the quantum dot-to induce Fabry-Perot oscillations in conductance we observe oscillations in the measured Kondo temperature T-K, which is a signature of the Kondo cloud at distance L. When L is less than xi(K) the T-K oscillation amplitude becomes larger as L becomes smaller, obeying a scaling function of a single parameter L/xi(K), whereas when L is greater than xi(K) the oscillation is much weaker. Our results reveal that xi(K) is the only length parameter associated with the Kondo effect, and that the cloud lies mostly within a length of xi(K). Our experimental method offers a way of detecting the spatial distribution of exotic non-Fermi liquids formed by multiple magnetic impurities or multiple screening channels(13-16) and of studying spin-correlated systems.


  
Initial Leader Properties During the Preliminary Breakdown Processes of Lightning Flashes and Their Associations With Initiation Positions 期刊论文
JOURNAL OF GEOPHYSICAL RESEARCH-ATMOSPHERES, 2019, 124 (14) : 8025-8042
作者:  Zheng, Dong;  Shi, Dongdong;  Zhang, Yang;  Zhang, Yijun;  Lyu, Weitao;  Meng, Qing
收藏  |  浏览/下载:8/0  |  提交时间:2019/11/27
initial leader  preliminary breakdown process  flash initiation  charge distribution  charge density  
Regional distribution effects of different electricity network tariff designs with a distributed generation structure: The case of Germany 期刊论文
ENERGY POLICY, 2018, 113: 97-111
作者:  Hinz, Fabian;  Schmidt, Matthew;  Moest, Dominik
收藏  |  浏览/下载:2/0  |  提交时间:2019/04/09
Grid charge  Network tariff  Transmission grid  Distribution grid  Grid extension  Demography