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TEACHING: PHYS 457    PHYS 559

CURRICULUM VITAE

Contact Information:

Office:152F  Davey Lab, Phone:1-814-863-0090
Lab: S3/S4 Osmond Lab, Phone:1-814-863-0098
Email: liu@phys.psu.edu

Mailing Address:
Department of Physics
The Pennsylvania State University 
104 Davey Lab
University Park, PA 16802
USA

Last Updated:2-12-2009


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Quantum phase transitions and collective phenomena in few-layer crystals

 

Free standing atomically thin crystals have long been thought to be impossible due to predictions made by Landau and others on the absence of a true long-range order in two dimensions.  However, the experimental discovery of graphene, a single atomic sheet of single-crystal graphite demonstrated that both crystalline order and associated electronic band structure can be preserved sufficiently well  atomically thin, mesoscopic size flakes. This provides a playground to study collective phenomena in low dimensions, such as superconductivity, magnetic ordering, or density waves. 

We are currently focused on atomically thin crystals of NbSe2 and other chalcogenides that can be prepared following the same mechanical exfoliation technique developed in graphene research.  Using the so called “scotch tape” method one first cleaves a single crystal of NbSe2, the cleaved NbSe2 is pressed against a substrate of doped Si covered with 300 nm thermally grown SiO2 and then separated.  This process deposits a wide range of thin crystals on the substrate.  We identify the thinnest crystal flakes using an optical microscope under which they show different colors and faintness.  By correlating the optical identification with atomic force microscopy (AFM) and Raman spectroscopy measurements a “color code” is developed, allowing for rapid identification of flake thickness by optical means.  Once identified, electrically contacts to individual crystal flakes are made.  We previously developed a lithography free technique [1] using a thin quartz filament as a shadow mask placed directly on the crystal of interest to prepare three-terminal devices.  This technique allows for rapid fabrication, as well as protecting the crystal from possible contamination and damage from the wide range of solvents required by standard lithographic fabrication.  For other devices, such as Hall bars, a standard e-beam lithography fabrication technique is employed.

Our recent work on atomically thin NbSe2 has demonstrated that superconductivity survives down to a single unit cell of 2H-NbSe2 which has a reduced onset Tc of up to 2.5K.  In these thinnest crystalline NbSe2 flakes we have modulated the superconducting transition temperature  by 200mK (8%) using an electric field produced by 300-nm thermally grown SiO2 as gate dielectric.  This is higher than what is expected from a simple BCS model.  We attribute this to either the multiple-band superconductivity, or enhanced Coulomb repulsion in atomically thin NbSe2 [2].

Contacts:

Neal Staley, nes151 @ psu.edu


Publications
:

[1]N. E. Staley et al., “Lithography-free fabrication of graphene devices,” Appl. Phys. Lett. 90, 143518 (2007).

[2]Neal E. Staley, Jian Wu, Peter Eklund, Ying Liu, Linjun Li and Zhuan Xu, “Electric field effect on superconductivity in atomically thin flakes of NbSe2,” Submitted to PRB (2008) 

 

Optical image of NbSe2 flakes showing the color variation as thickness is reduced.  Gold colored is thickest, while light purple is thinnest in this image. 

 

Atomic force microscopy (AFM) image of single unit cell NbSe2 flakes.  Note the distance that the flake lies above the substrate is sample dependant, therefore folds within the flake are the only way to measure thickness. 

Ebeam lithography patterned hall bar of NbSe2.