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Volumn 88, Issue 23, 2013, Pages

Imprint of transition metal d orbitals on a graphene Dirac cone

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EID: 84892385355     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.88.235431     Document Type: Article
Times cited : (34)

References (38)
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    • The vanishing of the 2D peak is also laser frequency dependent. At sample locations where the 2D peak intensity is virtually undetectable at one laser energy (e.g., 633 nm laser), it is observable at another laser energy (e.g., 514 nm laser). See Sec. of Supplemental Material (Ref.).
    • The vanishing of the 2D peak is also laser frequency dependent. At sample locations where the 2D peak intensity is virtually undetectable at one laser energy (e.g., 633 nm laser), it is observable at another laser energy (e.g., 514 nm laser). See Sec. of Supplemental Material (Ref.).


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