n-type WS2 crystals XRD data from WS2 crystals Raman spectrum of WS2 crystals HRTEM data collected from WS2 crystals PL data collected from undoped WS2 crystals Characteristics of n-type WS2 crystals

n-type WS2 crystals

$650.00

14 years of growth optimization in chemical vapor transport (CVT) as well as flux growth lead to our flawless WS2 crystals: Our large size (~1cm in size) vdW WS2 crystals are treated as gold standards in 2D materials field. Our n-type WS2 crystals are doped with Re or Au atoms at ~1E17-1E18 cm-3 range. WS2 crystals from 2Dsemiconductors are known for its superior valleytronic performance, perfect crystallization, defect free structure, extremely narrow PL bandwidths, clean PL spectra (free of bound exciton shoulders), and high carrier mobility. Thousands of scientific articles have cited us and used these crystals for scientific accuracy and clean signals. Please also see our n- and p-type WS2 crystals doped with Au, Re, Nb, or other transition metal atoms. Please note that doping into TMDCs greatly reduce the crystallization time (growth speeds), thus electronically doped TMDCs measure smaller than undoped (intrinsic) TMDCs.

Typical characteristics of WS2 crystals from 2Dsemiconductors

ws2-n-type-characteristics.png

Growth method matters> Flux zone or CVT growth method? Contamination of halides and point defects in layered crystals are well known cause for their reduced electronic mobility, reduced anisotropic response, poor e-h recombination, low-PL emission, and lower optical absorption. Flux zone technique is a halide free technique used for synthesizing truly semiconductor grade vdW crystals. This method distinguishes itself from chemical vapor transport (CVT) technique in the following regard: CVT is a quick (~2 weeks) growth method but exhibits poor crystalline quality and the defect concentration reaches to 1E11 to 1E12 cm-2 range. In contrast, flux method takes long (~3 months) growth time, but ensures slow crystallization for perfect atomic structuring, and impurity free crystal growth with defect concentration as low as 1E9 - 1E10 cm-2. During check out just state which type of growth process is preferred. Unless otherwise stated, 2Dsemiconductors ships Flux zone crystals as a default choice. 

http://meetings.aps.org/Meeting/MAR18/Session/K36.3

http://meetings.aps.org/Meeting/MAR17/Session/V1.14

XRD data collected from WS2 crystals

ws2-xrd.png

Raman spectrum collected from WS2 monolayers

ws2-raman.png

PL spectrum collected from monolayer WS2 on SiO2/Si substrates

pl-ws2.png

SIMS purity datasets collected from WS2 crystals

ws2-sims.png

 HRTEM images collected from WS2 crystals

wse2-crystal-structure.png

 

Partial List of Published Articles from This Product

Summary: Publications from MIT, Washington, MIT, Berkeley, Stanford, and Princeton teams at top journals like Nature Nanotechnology, Nano Letters, and Advanced Materials

Control of Exciton Valley Coherence in Transition Metal Dichalcogenide Monolayers, Phys. Rev. Lett. 117, 187401 (2016)

T. Scrace et. al. "Magnetoluminescence and valley polarized state of a two-dimensional electron gas in WS2 monolayers" Nature Nanotechnology 10, 603–607 (2015) doi:10.1038/nnano.2015.78

J. He et. al. "Electron transfer and coupling in graphene–tungsten disulfide van der Waals heterostructures" Nature Communications 5, Article number: 5622 (2014)

Measurement of the optical dielectric function of monolayer transition-metal dichalcogenides: MoS2, MoSe2, WS2, and WSe2, Yilei Li, Alexey Chernikov, Xian Zhang, Albert Rigosi, Heather M. Hill, Arend M. van der Zande, Daniel A. Chenet, En-Min Shih, James Hone, and Tony F. Heinz; Phys. Rev. B 90, 205422 (2014)

UT Austin - A. P. Nayak et. al. "Pressure-Modulated Conductivity, carrier Density, and Mobility of Multilayered Tungsten Disulfide" ACS Nano 10.1021/acsnano.5b03295

N. Peimyoo et. al. Nonblinking, Intense Two-Dimensional Light Emitter: Monolayer WS2 Triangles ACS Nano, 2013, 7 (12), pp 10985–10994

Manish Chhowalla, "Two-dimensional semiconductors for transistors" Nature Reviews Materials 1, Article number: 16052 (2016) doi:10.1038/natrevmats.2016.52

Tongay et. al. "Defects activated photoluminescence in two-dimensional semiconductors: interplay between bound, charged, and free excitons" Scientific Reports 3, Article number: 2657 (2013)

X Li et al. "Determining layer number of twodimensional flakes of transition-metal dichalcogenides by the Raman intensity from substrates" Nanotechnology 27 (2016) 145704

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    14 years of growth optimization in chemical vapor transport (CVT) as well as flux growth lead to our flawless WS2 crystals: Our large size (~1cm in size) vdW WS2 crystals are treated as gold standards in 2D materials field. Our n-type WS2 crystals are doped with Re or Au atoms at ~1E17-1E18 cm-3 range. WS2 crystals from 2Dsemiconductors are known for its superior valleytronic performance, perfect crystallization, defect free structure, extremely narrow PL bandwidths, clean PL spectra (free of bound exciton shoulders), and high carrier mobility. Thousands of scientific articles have cited us and used these crystals for scientific accuracy and clean signals. Please also see our n- and p-type WS2 crystals doped with Au, Re, Nb, or other transition metal atoms. Please note that doping into TMDCs greatly reduce the crystallization time (growth speeds), thus electronically doped TMDCs measure smaller than undoped (intrinsic) TMDCs.

    Typical characteristics of WS2 crystals from 2Dsemiconductors

    ws2-n-type-characteristics.png

    Growth method matters> Flux zone or CVT growth method? Contamination of halides and point defects in layered crystals are well known cause for their reduced electronic mobility, reduced anisotropic response, poor e-h recombination, low-PL emission, and lower optical absorption. Flux zone technique is a halide free technique used for synthesizing truly semiconductor grade vdW crystals. This method distinguishes itself from chemical vapor transport (CVT) technique in the following regard: CVT is a quick (~2 weeks) growth method but exhibits poor crystalline quality and the defect concentration reaches to 1E11 to 1E12 cm-2 range. In contrast, flux method takes long (~3 months) growth time, but ensures slow crystallization for perfect atomic structuring, and impurity free crystal growth with defect concentration as low as 1E9 - 1E10 cm-2. During check out just state which type of growth process is preferred. Unless otherwise stated, 2Dsemiconductors ships Flux zone crystals as a default choice. 

    http://meetings.aps.org/Meeting/MAR18/Session/K36.3

    http://meetings.aps.org/Meeting/MAR17/Session/V1.14

    XRD data collected from WS2 crystals

    ws2-xrd.png

    Raman spectrum collected from WS2 monolayers

    ws2-raman.png

    PL spectrum collected from monolayer WS2 on SiO2/Si substrates

    pl-ws2.png

    SIMS purity datasets collected from WS2 crystals

    ws2-sims.png

     HRTEM images collected from WS2 crystals

    wse2-crystal-structure.png

     

    Partial List of Published Articles from This Product

    Summary: Publications from MIT, Washington, MIT, Berkeley, Stanford, and Princeton teams at top journals like Nature Nanotechnology, Nano Letters, and Advanced Materials

    Control of Exciton Valley Coherence in Transition Metal Dichalcogenide Monolayers, Phys. Rev. Lett. 117, 187401 (2016)

    T. Scrace et. al. "Magnetoluminescence and valley polarized state of a two-dimensional electron gas in WS2 monolayers" Nature Nanotechnology 10, 603–607 (2015) doi:10.1038/nnano.2015.78

    J. He et. al. "Electron transfer and coupling in graphene–tungsten disulfide van der Waals heterostructures" Nature Communications 5, Article number: 5622 (2014)

    Measurement of the optical dielectric function of monolayer transition-metal dichalcogenides: MoS2, MoSe2, WS2, and WSe2, Yilei Li, Alexey Chernikov, Xian Zhang, Albert Rigosi, Heather M. Hill, Arend M. van der Zande, Daniel A. Chenet, En-Min Shih, James Hone, and Tony F. Heinz; Phys. Rev. B 90, 205422 (2014)

    UT Austin - A. P. Nayak et. al. "Pressure-Modulated Conductivity, carrier Density, and Mobility of Multilayered Tungsten Disulfide" ACS Nano 10.1021/acsnano.5b03295

    N. Peimyoo et. al. Nonblinking, Intense Two-Dimensional Light Emitter: Monolayer WS2 Triangles ACS Nano, 2013, 7 (12), pp 10985–10994

    Manish Chhowalla, "Two-dimensional semiconductors for transistors" Nature Reviews Materials 1, Article number: 16052 (2016) doi:10.1038/natrevmats.2016.52

    Tongay et. al. "Defects activated photoluminescence in two-dimensional semiconductors: interplay between bound, charged, and free excitons" Scientific Reports 3, Article number: 2657 (2013)

    X Li et al. "Determining layer number of twodimensional flakes of transition-metal dichalcogenides by the Raman intensity from substrates" Nanotechnology 27 (2016) 145704