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    Intrinsic Nature of Graphene Revealed in Temperature-Dependent Transport of Twisted Multilayer Graphene

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    Graphene in its purest form is expected to exhibit a semiconducting to metallic transition in its temperature-dependent conductivity as a result of the interplay between Coulomb disorder and phonon scattering, the transition temperature, <i>T</i><sub>c</sub>, depending sensitively on the disorder induced carrier density (<i>n</i><sub>c</sub>). Even for good quality graphene, the <i>n</i><sub>c</sub> can be quite high (∼10<sup>12</sup> cm<sup>–2</sup>) and the transition temperature may be placed well above the ambient, practically rendering it to be only semiconducting over a wide range of temperature. Here we report an experimental study on the transport behavior of twisted multilayer graphene (tMLG) exhibiting <i>T</i><sub>c</sub> well below the ambient temperature. The graphene layers in these tMLG are highly decoupled with one another due to the angular rotation among them; as a result, they exhibit very high Raman I<sub>2D</sub>/I<sub>G</sub> values (up to 12) with narrow 2D width (16–24 cm<sup>–1</sup>). The observed <i>T</i><sub>c</sub> values seem to go hand in hand with the Raman I<sub>2D</sub>/I<sub>G</sub> values; a multilayer with mean I<sub>2D</sub>/I<sub>G</sub> value of 4.6 showed a <i>T</i><sub>c</sub> of 180 K, while that with mean I<sub>2D</sub>/I<sub>G</sub> of 4.9 showed lower a <i>T</i><sub>c</sub> of 160 K. Further, another multilayer with even higher mean I<sub>2D</sub>/I<sub>G</sub> value of 6.9 was metallic down to 5 K, indicating a very low disorder. The photoresponse behavior also corroborates well with the transition in transport behavior
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