journal article·2020-07-02

Dissimilar Decoupling Behavior of Two-Dimensional Materials on Metal Surfaces

Alexander Mehler, Nicolas Néel, Jörg Kröger

Publisher page

Abstract

The efficiency of hexagonal boron nitride and graphene to separate the hydrocarbon molecule C64H36 from Ru(0001) and Pt(111) surfaces is explored in low-temperature scanning tunneling microscopy and spectroscopy experiments. Both 2D materials enable the observation of the Franck-Condon effect in both frontier orbitals. On hexagonal boron nitride, vibronic progression with two vibrational energies gives rise to sharp orbital sidebands that are clearly visible up to the second order of the vibrational quantum number with different Huang-Rhys factors. In contrast, on graphene, orbital and vibronic spectroscopic signatures exhibit broad line shapes, with the second-order progression being hardly discriminable. Only a single vibrational quantum energy leaves its fingerprint in the Franck-Condon spectrum.
Source: europepmc · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Graphene research and applications · Surface and Thin Film Phenomena · Quantum and electron transport phenomena

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Institut für Physik, Technische Universität Ilmenau, D-98693 Ilmenau, Germany

Funding

Deutsche Forschungsgemeinschaft

References (65)

Show source-provided references
1. 10.1126/science.107867510.1126/science.1078675 ↗
2. 10.1103/PhysRevLett.95.19610210.1103/PhysRevLett.95.196102 ↗
3. 10.1126/science.110107710.1126/science.1101077 ↗
4. 10.1126/science.112539810.1126/science.1125398 ↗
5. 10.1103/PhysRevLett.92.20610210.1103/PhysRevLett.92.206102 ↗
6. 10.1021/ja105110d10.1021/ja105110d ↗
7. 10.1103/PhysRevB.78.23340110.1103/PhysRevB.78.233401 ↗
8. 10.1021/acsnano.8b0741410.1021/acsnano.8b07414 ↗
9. 10.1126/science.109955710.1126/science.1099557 ↗
10. 10.1103/PhysRevLett.94.02680310.1103/PhysRevLett.94.026803 ↗
11. 10.1126/science.114436610.1126/science.1144366 ↗
12. 10.1016/j.surfrep.2018.10.00110.1016/j.surfrep.2018.10.001 ↗
13. 10.1088/0953-8984/26/44/44300110.1088/0953-8984/26/44/443001 ↗
14. 10.1021/nn501459v10.1021/nn501459v ↗
15. 10.1039/C7NR06860C10.1039/C7NR06860C ↗
16. 10.1021/nn404840h10.1021/nn404840h ↗
17. 10.1021/nl503956p10.1021/nl503956p ↗
18. 10.1021/acsnano.5b0374110.1021/acsnano.5b03741 ↗
19. 10.1088/1361-648X/aaf54c10.1088/1361-648X/aaf54c ↗
20. 10.1038/s41467-019-10610-510.1038/s41467-019-10610-5 ↗
21. 10.1038/nature0423310.1038/nature04233 ↗
22. 10.1038/nnano.2008.26810.1038/nnano.2008.268 ↗
23. 10.1016/j.susc.2008.08.03710.1016/j.susc.2008.08.037 ↗
24. 10.1021/la062990t10.1021/la062990t ↗
25. 10.1016/j.susc.2010.01.00310.1016/j.susc.2010.01.003 ↗
26. 10.1021/ja311773510.1021/ja3117735 ↗
27. 10.1038/ncomms1384310.1038/ncomms13843 ↗
28. 10.1116/1.512548610.1116/1.5125486 ↗
29. 10.1021/acs.nanolett.8b0030410.1021/acs.nanolett.8b00304 ↗
30. 10.1039/tf926210053610.1039/tf9262100536 ↗
31. 10.1103/PhysRev.28.118210.1103/PhysRev.28.1182 ↗
32. Huang K. · Proc. R. Soc. London, Ser. A · 1950 · 204 · 40610.1098/rspa.1950.0184 ↗
33. 10.1103/PhysRevLett.105.23610110.1103/PhysRevLett.105.236101 ↗
34. 10.1103/PhysRevB.75.24541210.1103/PhysRevB.75.245412 ↗
35. 10.1103/PhysRevB.81.07541810.1103/PhysRevB.81.075418 ↗
36. 10.1103/PhysRevLett.105.21610210.1103/PhysRevLett.105.216102 ↗
37. 10.1016/j.tsf.2018.01.00910.1016/j.tsf.2018.01.009 ↗
38. 10.1063/1.354362410.1063/1.3543624 ↗
39. 10.1016/j.susc.2012.07.00510.1016/j.susc.2012.07.005 ↗
40. 10.1039/C8CP07569G10.1039/C8CP07569G ↗
41. 10.1103/PhysRevB.78.07340110.1103/PhysRevB.78.073401 ↗
42. 10.1103/PhysRevB.87.03542010.1103/PhysRevB.87.035420 ↗
43. 10.1016/j.cplett.2007.03.00110.1016/j.cplett.2007.03.001 ↗
44. 10.1103/PhysRevLett.91.19680110.1103/PhysRevLett.91.196801 ↗
45. 10.1103/PhysRevB.70.03340110.1103/PhysRevB.70.033401 ↗
46. 10.1103/PhysRevLett.75.391810.1103/PhysRevLett.75.3918 ↗
47. 10.1016/0039-6028(82)90379-X10.1016/0039-6028(82)90379-X ↗
48. 10.1103/PhysRevB.79.04540710.1103/PhysRevB.79.045407 ↗
49. 10.1103/PhysRevB.80.24541110.1103/PhysRevB.80.245411 ↗
50. 10.1103/PhysRevB.87.24541410.1103/PhysRevB.87.245414 ↗
51. 10.1103/PhysRevB.84.24543610.1103/PhysRevB.84.245436 ↗
52. 10.1088/1367-2630/16/5/05303610.1088/1367-2630/16/5/053036 ↗
53. 10.1088/0953-8984/20/18/18400110.1088/0953-8984/20/18/184001 ↗
54. 10.1103/PhysRevB.77.08542110.1103/PhysRevB.77.085421 ↗
55. 10.1021/acsnano.6b0598210.1021/acsnano.6b05982 ↗
56. 10.1103/PhysRevB.86.15515110.1103/PhysRevB.86.155151 ↗
57. 10.1021/jp045289b10.1021/jp045289b ↗
58. 10.1002/cphc.20040061610.1002/cphc.200400616 ↗
59. 10.1103/PhysRevLett.98.16610310.1103/PhysRevLett.98.166103 ↗
60. 10.1039/C5CP03761A10.1039/C5CP03761A ↗
61. 10.1103/PhysRevLett.94.12610210.1103/PhysRevLett.94.126102 ↗
62. 10.1088/1367-2630/9/5/15310.1088/1367-2630/9/5/153 ↗
63. 10.1088/0953-8984/20/22/22300110.1088/0953-8984/20/22/223001 ↗
64. 10.1088/1367-2630/11/12/12500610.1088/1367-2630/11/12/125006 ↗
65. 10.1063/1.243241010.1063/1.2432410 ↗