Skip to main content
Home
Department Of Physics text logo
  • Research
    • Our research
    • Our research groups
    • Our research in action
    • Research funding support
    • Summer internships for undergraduates
  • Study
    • Undergraduates
    • Postgraduates
  • Engage
    • For alumni
    • For business
    • For schools
    • For the public
Menu
CMP
Credit: Jack Hobhouse

Shuaifeng Hu

Postdoctoral Research Assistant

Research theme

  • Photovoltaics and nanoscience

Sub department

  • Condensed Matter Physics

Research groups

  • Snaith group
shuaifeng.hu@physics.ox.ac.uk
Robert Hooke Building, room G24
Google Scholar
  • About
  • Publications

Steering Lu3N clusters in C76-78 cages: cluster configuration dominated by cage transformation.

Nanoscale 14:46 (2022) 17290-17296

Authors:

Pengwei Yu, Shuaifeng Hu, Xinyue Tian, Wangqiang Shen, Pengyuan Yu, Kun Guo, Yunpeng Xie, Lipiao Bao, Xing Lu

Abstract:

While the strong interaction between the internal unit and the fullerene cage inside metallofullerenes is widely acknowledged, how the cage transformation interacts with the cluster configuration remains elusive. For this purpose, we herein synthesized three metallofullerene molecules with an easy-to-compare cluster configuration and cage arrangement, namely Lu3N@Cs(17 490)-C76, Lu3N@C2(22 010)-C78, and Lu3N@D3h(5)-C78. The three lutetium-based nitride clusterfullerenes (NCFs) with small C76-78 carbon cages were synthesized by a modified arc-discharge method and their structures were unambiguously confirmed by X-ray crystallography. Notably, the cage transformation from Cs(17 490)-C76 to C2(22 010)-C78via a simple C2-unit insertion leads to a remarkable configuration change of the encapsulated Lu3N cluster from an unusual asymmetric plane to a common symmetric one. This close correlation between the cluster configuration and cage transformation is further confirmed by the pyramidal Lu3N cluster in Lu3N@D3h(5)-C78 other than the symmetric planar Lu3N unit in Lu3N@C2(22 010)-C78, as a result of an even larger difference in the cage arrangement. Astonishingly, such a cluster shrinkage, accompanied by an increase in the cage size from Cs(17 490)-C76 to D3h(5)-C78, is dramatically opposite to the cluster expansion with cage elongation found in La2C2- or Y2C2-based metallofullerenes.
More details from the publisher
More details
More details

Perovskite/perovskite tandem solar cells in the substrate configuration with potential for bifacial operation

ACS Materials Letters American Chemical Society 4:12 (2022) 2638-2644

Authors:

Lidón Gil-Escrig, Shuaifeng Hu, Kassio PS Zanoni, Abhyuday Paliwal, M Angeles Hernández-Fenollosa, Cristina Roldán-Carmona, Michele Sessolo, Atsushi Wakamiya, Henk J Bolink

Abstract:

Perovskite/perovskite tandem solar cells have recently exceeded the record power conversion efficiency (PCE) of single-junction perovskite solar cells. They are typically built in the superstrate configuration, in which the device is illuminated from the substrate side. This limits the fabrication of the solar cell to transparent substrates, typically glass coated with a transparent conductive oxide (TCO), and adds constraints because the first subcell that is deposited on the substrate must contain the wide-bandgap perovskite. However, devices in the substrate configuration could potentially be fabricated on a large variety of opaque and inexpensive substrates, such as plastic and metal foils. Importantly, in the substrate configuration the narrow-bandgap subcell is deposited first, which allows for more freedom in the device design. In this work, we report perovskite/perovskite tandem solar cells fabricated in the substrate configuration. As the substrate we use TCO-coated glass on which a solution-processed narrow-bandgap perovskite solar cell is deposited. All of the other layers are then processed using vacuum sublimation, starting with the charge recombination layers, then the wide-bandgap perovskite subcell, and finishing with the transparent top TCO electrode. Proof-of-concept tandem solar cells show a maximum PCE of 20%, which is still moderate compared to those of best-in-class devices realized in the superstrate configuration yet higher than those of the corresponding single-junction devices in the substrate configuration. As both the top and bottom electrodes are semitransparent, these devices also have the potential to be used as bifacial tandem solar cells.
More details from the publisher
Details from ORA
More details
More details

Operational stability, low light performance, and long-lived transients in mixed-halide perovskite solar cells with a monolayer-based hole extraction layer

Solar Energy Materials and Solar Cells Elsevier 245 (2022) 111885

Authors:

Richard Murdey, Yasuhisa Ishikura, Yuko Matsushige, Shuaifeng Hu, Jorge Pascual, Minh Anh Truong, Tomoya Nakamura, Atsushi Wakamiya
More details from the publisher
More details

Materials to Improve the Performance of Sn-Based Perovskite Solar Cells

Institute of Electrical and Electronics Engineers (IEEE) 00 (2022) 10-11

Authors:

Atsushi Wakamiya, Shuaifeng Hu, Tomoya Nakamura, Taketo Handa, Takumi Yamada, Minh Anh Truong, Richard Murdey, Yoshihiko Kanemitsu
More details from the publisher
More details

Cluster-Geometry-Associated Metal-Metal Bonding in Trimetallic Carbide Clusterfullerenes.

Inorganic chemistry 61:29 (2022) 11277-11283

Authors:

Shuaifeng Hu, Pei Zhao, Bo Li, Pengwei Yu, Le Yang, Masahiro Ehara, Peng Jin, Takeshi Akasaka, Xing Lu

Abstract:

Geometry configurations of the metallic clusters play a significant role in the involved bonding nature. Herein, we report the crystallographic characterization of unprecedented erbium-based trimetallic clusterfullerenes, namely, Er3C2@Ih(7)-C80, in which the inner Er3C2 cluster presents a lifted bat ray configuration with the C2 unit elevated by ∼1.62 Å above the Er3 plane. Within the plane, the Er···Er distances for Er1···Er2, Er1···Er2A, and Er2···Er2A are 3.4051(15), 3.4051(15), and 3.3178(15) Å, respectively, falling into the range of the metal-metal bonding. Density functional theory calculations unveil the three-center-one-electron Er-Er-Er bond in Er3C2@Ih(7)-C80 with one electron shared by three metals, and thus, its exceptional electronic structure can be expressed as (Er3)8+(C2)2-@C806-. Interestingly, with the further observation on the geometry configurations of the encapsulated clusters in M3C2@C2n (M = Sc, Y, and Lu) series, we find that the lifted bat ray configuration of the inner cluster is explicitly associated with the formation of the bonding interactions between the inner metals. This finding provides insights into the nature of metal-metal bonding and gives guidelines for the design of the single-molecule magnet.
More details from the publisher
More details
More details

Pagination

  • First page First
  • Previous page Prev
  • …
  • Page 4
  • Page 5
  • Page 6
  • Page 7
  • Current page 8
  • Page 9
  • Page 10
  • Page 11
  • Page 12
  • Next page Next
  • Last page Last

Footer Menu

  • Contact us
  • Giving to the Dept of Physics
  • Work with us
  • Media

User account menu

  • Log in

Follow us

FIND US

Clarendon Laboratory,

Parks Road,

Oxford,

OX1 3PU

CONTACT US

Tel: +44(0)1865272200

University of Oxfrod logo Department Of Physics text logo
IOP Juno Champion logo Athena Swan Silver Award logo

© University of Oxford - Department of Physics

Cookies | Privacy policy | Accessibility statement

Built by: Versantus

  • Home
  • Research
  • Study
  • Engage
  • Our people
  • News & Comment
  • Events
  • Our facilities & services
  • About us
  • Current students
  • Staff intranet