Multiple hot-carrier collection in photo-excited graphene Moiré superlattices

Morié-engineered graphene devices can collect multiple electrons per absorbed photon, promising efficient optoelectronics. In conventional light-harvesting devices, the absorption of a single photon only excites one electron, which sets the standard limit of power-conversion efficiency, such as the Shockley-Queisser limit. In principle, generating and harnessing multiple carriers per absorbed photon can improve efficiency and possibly overcome this limit. We report the observation of multiple hot-carrier collection in graphene/boron-nitride Moiré superlattice structures. A record-high zero-bias photoresponsivity of 0.3 A/W (equivalently, an external quantum efficiency exceeding 50%) is achieved using graphene’s photo-Nernst effect, which demonstrates a collection of at least five carriers per absorbed photon. We reveal that this effect arises from the enhanced Nernst coefficient through Lifshtiz transition at low-energy Van Hove singularities, which is an emergent phenomenon due to the formation of Moiré minibands. Our observation points to a new means for extremely efficient and flexible optoelectronics based on van der Waals heterostructures.

[1]  P. Wei,et al.  Strong interfacial exchange field in the graphene/EuS heterostructure. , 2015, Nature materials.

[2]  Zaiyao Fei,et al.  Photo-Nernst current in graphene , 2015, Nature Physics.

[3]  P. Wei,et al.  Strong Interfacial Exchange Field in 2D Material/Magnetic-Insulator Heterostructures: Graphene/EuS , 2015 .

[4]  L Piatkowski,et al.  Generation of photovoltage in graphene on a femtosecond timescale through efficient carrier heating. , 2015, Nature nanotechnology.

[5]  T. Seyller,et al.  Tunable carrier multiplication and cooling in graphene. , 2015, Nano letters.

[6]  P. Avouris,et al.  Photodetectors based on graphene, other two-dimensional materials and hybrid systems. , 2014, Nature nanotechnology.

[7]  H. Kurz,et al.  Experimental verification of carrier multiplication in graphene. , 2014, Nano letters.

[8]  A. V. Kretinin,et al.  Detecting topological currents in graphene superlattices , 2014, Science.

[9]  Zhiwen Shi,et al.  Observation of an intrinsic bandgap and Landau level renormalization in graphene/boron-nitride heterostructures , 2014, Nature Communications.

[10]  T. Taniguchi,et al.  Photoinduced doping in heterostructures of graphene and boron nitride. , 2014, Nature nanotechnology.

[11]  K. Novoselov,et al.  Hierarchy of Hofstadter states and replica quantum Hall ferromagnetism in graphene superlattices , 2014, Nature Physics.

[12]  C. A. Nelson,et al.  Exceeding the Shockley–Queisser limit in solar energy conversion , 2013 .

[13]  K. L. Shepard,et al.  One-Dimensional Electrical Contact to a Two-Dimensional Material , 2013, Science.

[14]  Xiangshan Chen,et al.  Infrared absorption by graphene–hBN heterostructures , 2013, 1309.2292.

[15]  Takashi Taniguchi,et al.  Epitaxial growth of single-domain graphene on hexagonal boron nitride. , 2013, Nature materials.

[16]  K. L. Shepard,et al.  Hofstadter’s butterfly and the fractal quantum Hall effect in moiré superlattices , 2013, Nature.

[17]  T. Taniguchi,et al.  Massive Dirac Fermions and Hofstadter Butterfly in a van der Waals Heterostructure , 2013, Science.

[18]  F. Guinea,et al.  Cloning of Dirac fermions in graphene superlattices , 2012, Nature.

[19]  A. Geim,et al.  Generic miniband structure of graphene on a hexagonal substrate , 2012, 1211.4711.

[20]  A. Centeno,et al.  Photoexcitation cascade and multiple hot-carrier generation in graphene , 2012, Nature Physics.

[21]  K. Novoselov,et al.  Ultrafast collinear scattering and carrier multiplication in graphene , 2012, Nature Communications.

[22]  F. Koppens,et al.  Photoexcited carrier dynamics and impact-excitation cascade in graphene , 2012, 1209.4346.

[23]  Pablo Jarillo-Herrero,et al.  Emergence of superlattice Dirac points in graphene on hexagonal boron nitride , 2012, Nature Physics.

[24]  Takashi Taniguchi,et al.  Hot Carrier–Assisted Intrinsic Photoresponse in Graphene , 2011, Science.

[25]  Charles M Marcus,et al.  Hot carrier transport and photocurrent response in graphene. , 2011, Nano letters.

[26]  A. Knorr,et al.  Carrier multiplication in graphene. , 2010, Nano letters.

[27]  A. Reina,et al.  Observation of Van Hove singularities in twisted graphene layers , 2009, 0912.2102.

[28]  A. M. van der Zande,et al.  Photo-thermoelectric effect at a graphene interface junction. , 2009, Nano letters.

[29]  N. Ong,et al.  Thermopower and Nernst effect in graphene in a magnetic field , 2008, 0812.2866.

[30]  P. Kim,et al.  Thermoelectric and magnetothermoelectric transport measurements of graphene. , 2008, Physical review letters.

[31]  F. Guinea,et al.  The electronic properties of graphene , 2007, Reviews of Modern Physics.

[32]  H. Aoki,et al.  Topological analysis of the quantum Hall effect in graphene: Dirac-Fermi transition across van Hove singularities and edge versus bulk quantum numbers , 2006, cond-mat/0607669.

[33]  Y. Blanter,et al.  The theory of electronic topological transitions , 1994 .

[34]  R. Markiewicz The topological significance of saddle point van Hove singularities: a comparison of orbital switching and magnetic breakdown , 1994 .

[35]  R S Markiewicz The topological significance of saddle point van Hove singularities: a comparison of orbital switching and magnetic breakdown , 1994 .

[36]  S. Girvin,et al.  Thermoelectric effect in a weakly disordered inversion layer subject to a quantizing magnetic field , 1984 .