Method Article

Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials

DOI:

10.3791/53506

January 21st, 2016

In This Article

Summary

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We describe the methodology of mechanical exfoliation and deposition of flakes of novel materials with micron-sized dimensions onto substrate, fabrication of experimental device structures for transport experimentation, and the magnetotransport measurement in a dry helium close-cycle cryostat at temperatures down to 0.300 K and magnetic fields up to 12 T.

Abstract

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Novel electronic materials are often produced for the first time by synthesis processes that yield bulk crystals (in contrast to single crystal thin film synthesis) for the purpose of exploratory materials research. Certain materials pose a challenge wherein the traditional bulk Hall bar device fabrication method is insufficient to produce a measureable device for sample transport measurement, principally because the single crystal size is too small to attach wire leads to the sample in a Hall bar configuration. This can be, for example, because the first batch of a new material synthesized yields very small single crystals or because flakes of samples of one to very few monolayers are desired. In order to enable rapid characterization of materials that may be carried out in parallel with improvements to their growth methodology, a method of device fabrication for very small samples has been devised to permit the characterization of novel materials as soon as a preliminary batch has been produced. A slight variation of this methodology is applicable to producing devices using exfoliated samples of two-dimensional materials such as graphene, hexagonal boron nitride (hBN), and transition metal dichalcogenides (TMDs), as well as multilayer heterostructures of such materials. Here we present detailed protocols for the experimental device fabrication of fragments and flakes of novel materials with micron-sized dimensions onto substrate and subsequent measurement in a commercial superconducting magnet, dry helium close-cycle cryostat magnetotransport system at temperatures down to 0.300 K and magnetic fields up to 12 T.

Introduction

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The pursuit of materials platforms for advanced electronics technology demands methods for high-throughput materials synthesis and subsequent characterization. Novel materials of interest in this pursuit may be produced in bulk by direct reaction synthesis1,2, electrochemical growth3,4, and other methods5 in a more rapid fashion than more involved single crystal thin film deposition techniques such as molecular beam epitaxy or chemical vapor deposition. The conventional method to measure the transport properties of bulk crystal samples is to cleave a rectangular prism-shaped fragment with dimensions of approximately 1 mm x 1 mm x 6 mm ....

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Protocol

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1. Preparation of Substrate

  1. Obtain 4 inch silicon (Si) wafer composed of heavily-doped p-doped Si covered by approximately 300 nm of SiO2. This substrate structure will allow the substrate to serve as a back gate.
  2. Using drafting/design software, design a 1 cm × 1 cm pattern with evenly spaced features, such as enumerated crosses, in the x and y direction to use as positional locators on the substrate for transferred sample flakes and alignment marks for electron beam lithography (Figure 1).
    1. Open a new file in a drafting program such as AutoCAD.
    2. Use polylines to draw the following marks: i) c....

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Results

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Figure 3 shows a typical Hall bar device patterned for the purpose of a low temperature magnetotransport experiment. The optical image in the upper figure shows a successfully-fabricated Graphene/hBN Hall bar; the lower image shows the device schematic with the Landauer-Büttiker edge states that arise from the Landau levels (LLs), a transport mechanism that can be used to calculate the values of the quantized Hall resistances, the experimental investigation of which will .......

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Discussion

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After acquisition of high quality bulk samples, characterized to ensure appropriate composition and structure, samples are patterned into the geometry depicted by exfoliating flakes of sample onto 1 cm × 1 cm pieces of substrate. Substrates composed of heavily p-doped Si covered by approximately 300 nm of SiO2 are preferred as they increase the experimental parameter space by allowing the application of a back gate. Samples must be sufficiently thin — fewer than 10 nm — to produce a suffi.......

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Disclosures

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The authors declare no competing financial interests. Commercial materials, instruments and equipment are identified in this paper to specify the experimental procedure as completely as possible. In no case does such identification imply a recommendation or endorsement by the National Institute of Standards.

Acknowledgements

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This work is supported by the National Institute of Standards and Technology of the United States Department of Commerce.

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Materials

List of materials used in this article
NameCompanyCatalog NumberComments
Cryogenic Limited 12 T CFMSCryogen LimitedCFM-12T-H3- IVTI-25Magnetotransport system customized with modulated field magnet (step 4)
7270 DSP Lock-in amplifierSignal Recovery7270lock-in amplifier for source/drain and voltage measurements (step 4)
GS200 DC Voltage/Current SourceYokogawaGS200Voltage source for gate voltage application (step 4)
2636B System SourcemeterKeithley2636BSourcemeter for source/drain and voltage measurements
DWL 2000 Laser Pattern GeneratorHeidelberg InstrumentsDWL 2000Generate chrome mask for lithography of substrate location/alignment feature pattern (step 1.3)
Suss MicroTec MA6/BA6 Contact AlignerSussMA6Used for the lithography of substrate location/alignment feature pattern (step 1.4.12)
JEOL Direct Write Electron Beam Lithography SystemJEOLJBX 6300-FS Perform high-resolution lithography of devices
Discovery 550 Sputtering SystemDenton VacuumDiscovery 550Perform SiO2 sputtering (step 2.5)
Infinity 22 Electron Beam EvaporatorDenton VacuumInfinty 22Perform Cr/Au deposition (steps 1.5 and 3.7)
Unaxis 790 Reactive Ion EtcherUnaxisUnaxis 790Etch sample into Hall bar structure (step 3.4)
PMMA 495 A4MicroChemPMMA 495 A4Polymer coating/electron beam mask for lithography (step 3.5.1)
PMMA 950 A4MicroChemPMMA 950 A4Polymer coating/electron beam mask for sample dicing and lithography (steps 1.7.3, 3.3.1, and 3.5.2)
S1813 positive photoresistMicroChemS1813 G2Positive photoresist (step 1.4.8)
LOR resistMicroChemLOR 3ALift off resist (step 1.4.3)
1:3 MIBK:IPA PMMA developerMicroChem1:3 MIBK:IPAPMMA developer
MF-321 DeveloperMicroChemMF-321Novolac positive photoresist-compatible developer solution (step 1.4.15)
Diglycidiyl ether-terminated polydimethylsiloxaneSigma AldrichSA 480282For layered material stacking (step 2.6.1)
Polypropylene carbonateSigma AldrichSA 389021For layered material stacking (step 2.6.2)

References

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  1. Doty, F. P. Properties of CdZnTe crystals grown by a high pressure Bridgman method. Journal of Vacuum Science & Technology B. 10 (4), 1418-1422 (1992).
  2. Ikesue, A., Kinoshita, T., Kamata, K., Yoshida, K.

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Tags

Low temperature MagnetotransportNovel MaterialsExfoliated SamplesElectron beam LithographyHall Bar DesignReactive Ion EtchingMetal Contact DepositionSuperconducting MagnetDry Helium CryostatQuantum Hall Effect

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