• Creation of the most perfect graphene

    From ScienceDaily@1:317/3 to All on Wed Aug 25 21:30:28 2021
    Creation of the most perfect graphene
    New discovery allows for scalable production of fold-free and ad-layer
    free single-crystal graphene

    Date:
    August 25, 2021
    Source:
    Institute for Basic Science
    Summary:
    Researchers have achieved growth and characterization of large
    area, single-crystal graphene that has no wrinkles, folds, or
    adlayers. It can be said to be the most perfect graphene that has
    been grown and characterized, to date.



    FULL STORY ==========================================================================
    A team of researchers led by Director Rod Ruoff at the Center for Multidimensional Carbon Materials (CMCM) within the Institute for
    Basic Science (IBS), including graduate students at the Ulsan National Institute of Science and Technology (UNIST), have achieved growth and characterization of large area, single-crystal graphene that has no
    wrinkles, folds, or adlayers. It can be said to be the most perfect
    graphene that has been grown and characterized, to date.


    ========================================================================== Director Ruoff notes, "This pioneering breakthrough was due to many contributing factors, including human ingenuity and the ability of the
    CMCM researchers to reproducibly make large-area single-crystal Cu-Ni(111) foils, on which the graphene was grown by chemical vapor deposition
    (CVD) using a mixture of ethylene with hydrogen in a stream of argon
    gas." Student Meihui Wang, Dr.

    Ming Huang, and Dr. Da Luo along with Ruoff undertook a series of
    experiments of growing single-crystal and single-layer graphene on such 'home-made' Cu-Ni (111) foils under different temperatures.

    The team had previously reported single-crystal and adlayer-free films
    of graphene which were grown using methane at temperatures of ~1320
    Kelvin (K) degrees on Cu(111) foils. Adlayers refer to small "islands"
    of regions that have another layer of graphene present. However, these
    films always contained long "folds" that are the consequence of tall
    wrinkles that form as the graphene is cooled from the growth temperature
    down to room temperature. This results in an undesirable reduction in
    the performance of graphene field effect transistor (GFET) if the "fold"
    is in the active region of the GFET. The folds also contain "cracks"
    that lower the mechanical strength of the graphene.

    The next exciting challenge was thus eliminating these folds.

    CMCM researchers first implemented a series of 'cycling' experiments that involved "cycling" the temperature immediately after growing the graphene
    at 1320 K. These experiments showed that the folds are formed at or above
    1020 K during the cooling process. After learning this, the team decided
    to grow graphene on Cu-Ni(111) foils at several different temperatures
    around 1020 K, which led to a discovery that large-area, high-quality, fold-free, and adlayer- free single-crystal graphene films can be grown in
    a temperature range between 1000 K and 1030 K. "This fold-free graphene
    film forms as a single crystal over the entire growth substrate because
    it shows a single orientation over a large- area low-energy electron diffraction (LEED) patterns," noted SEONG Won Kyung, a senior research
    fellow in CMCM who installed the LEED equipment in the center.

    GFETs were then patterned on this single-crystal fold-free graphene
    in a variety of directions by UNIST graduate student Yunqing Li. These
    GFETs showed remarkably uniform performance with average room temperature electron and hole mobilities of 7.0 +/- 1.0 x 103 cm2 V-1 s-1. Li notes,
    "Such remarkably uniform performance is possible because the fold-free
    graphene film is a single crystal with essentially no imperfections." Importantly, the research team was able to achieve "scaling up" of
    graphene production using this method. The graphene was successfully
    grown on 5 foils (dimension 4 cm x 7 cm) simultaneously in a 6-inch
    diameter home-built quartz furnace. "Our method of growing fold-free
    graphene films is very reproducible, with each foil yielding two identical pieces of high-quality graphene films on both sides of the foil," and
    "By using the electrochemical bubbling transfer method, graphene can
    be delaminated in about 1 minute and the Cu-Ni(111) foil can be quickly
    readied for the next growth/transfer cycle," notes Meihui Wang.

    Ming Huang adds, "When we tested the weight loss of Cu-Ni(111) foils
    after 5 runs of growth and transfers, the net loss was only 0.0001
    grams. This means that our growth and transfer methods using the
    Cu-Ni(111) can be performed repeatedly, essentially indefinitely."
    In the process of achieving fold-free single-crystal graphene, the
    researchers also discovered the reasons behind the formation of these
    folds. High- resolution TEM imaging was performed by student CHOE Myeonggi
    and Prof. LEE Zonghoon (a group leader in CMCM and professor at UNIST)
    to observe the cross- sections of the samples grown above 1040 K. They discovered that the deadhesion, which is the cause of the folds, is
    initiated at the "bunched step edge" regions between the single crystal Cu-Ni(111) plateaus. "This deadhesion at the bunched step edge regions
    triggers the formation of graphene folds perpendicular to the step edge direction," noted co-corresponding author Luo.

    Ruoff further notes that "We discovered that step-bunching of a Cu-Ni(111)
    foil surface suddenly occurs at about 1030 K, and this 'surface
    reconstruction' is the reason why the critical growth temperature of
    fold-free graphene is at ~1030 K or below." Such large-area fold-free single-crystal graphene film allows for the straightforward fabrication
    of integrated high-performance devices oriented in any direction over
    the entire graphene film. These single-crystal graphene films will be
    important for further advances in basic science, which will lead to
    new applications in electronic, photonic, mechanical, thermal, and
    other areas. The near-perfect graphene is also useful for stacking,
    either with itself and/or with other 2D materials, to further expand
    the range of likely applications. Given that the Cu-Ni(111) foils can
    be used repeatedly and that the graphene can be transferred to other
    substrates in less than one minute, the scalable manufacturing using
    this process is also highly promising.

    ========================================================================== Story Source: Materials provided by Institute_for_Basic_Science. Note:
    Content may be edited for style and length.


    ========================================================================== Journal Reference:
    1. Wang, M., Huang, M., Luo, D. et al. Single-crystal, large-area,
    fold-free
    monolayer graphene. Nature, 2021 DOI: 10.1038/s41586-021-03753-3 ==========================================================================

    Link to news story: https://www.sciencedaily.com/releases/2021/08/210825113619.htm

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