Depopulation of Single-Phthalocyanine Molecular Orbitals upon Pyrrolic-Hydrogen Abstraction on Graphene
Source abstract
Abstract
Single-molecule chemistry with a scanning tunneling microscope has preponderantly been performed on metal surfaces. The molecule-metal hybridization, however, is often detrimental to genuine molecular properties and obscures their changes upon chemical reactions. We used graphene on Ir(111) to reduce the coupling between Ir(111) and adsorbed phthalocyanine molecules. By local electron injection from the tip of a scanning tunneling microscope the two pyrrolic H atoms were removed from single phthalocyanines. The detachment of the H atom pair induced a strong modification of the molecular electronic structure, albeit with no change in the adsorption geometry. Spectra and maps of the differential conductance combined with density functional calculations unveiled the entire depopulation of the highest occupied molecular orbital upon H abstraction. Occupied π states of intact molecules are proposed to be emptied via intramolecular electron transfer to dangling σ states of H-free N atoms.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Molecular Junctions and Nanostructures · Surface Chemistry and Catalysis · 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
Department of Chemistry, UMR ENS-CNRS-UPMC 8640, Ecole Normale Supérieure, F-75005 Paris, France
References (64)
Show source-provided references
1. 10.1038/325419a010.1038/325419a0 ↗
2. 10.1038/344524a010.1038/344524a0 ↗
3. 10.1126/science.268.5217.159010.1126/science.268.5217.1590 ↗
4. 10.1103/PhysRevLett.85.277710.1103/PhysRevLett.85.2777 ↗
5. 10.1103/PhysRevLett.90.06610710.1103/PhysRevLett.90.066107 ↗
6. 10.1103/PhysRevLett.93.19680610.1103/PhysRevLett.93.196806 ↗
7. 10.1126/science.109955710.1126/science.1099557 ↗
8. 10.1126/science.112488110.1126/science.1124881 ↗
9. 10.1063/1.152115310.1063/1.1521153 ↗
10. 10.1088/0953-8984/17/13/00310.1088/0953-8984/17/13/003 ↗
11. 10.1002/pssb.20124839210.1002/pssb.201248392 ↗
12. 10.1088/0034-4885/77/5/05650210.1088/0034-4885/77/5/056502 ↗
13. 10.1016/j.surfrep.2015.04.00110.1016/j.surfrep.2015.04.001 ↗
14. 10.1126/science.107867510.1126/science.1078675 ↗
15. 10.1103/PhysRevLett.95.19610210.1103/PhysRevLett.95.196102 ↗
16. 10.1103/PhysRevLett.95.22550310.1103/PhysRevLett.95.225503 ↗
17. 10.1103/PhysRevLett.100.03680710.1103/PhysRevLett.100.036807 ↗
18. 10.1021/ja807876c10.1021/ja807876c ↗
19. 10.1021/ja105110d10.1021/ja105110d ↗
20. 10.1002/anie.20080330510.1002/anie.200803305 ↗
21. 10.1103/PhysRevB.78.23340110.1103/PhysRevB.78.233401 ↗
22. 10.1073/pnas.100666110710.1073/pnas.1006661107 ↗
23. 10.1021/jp311420d10.1021/jp311420d ↗
24. 10.1021/jp203861910.1021/jp2038619 ↗
25. 10.1021/ja904907z10.1021/ja904907z ↗
26. 10.1063/1.356139810.1063/1.3561398 ↗
27. 10.1063/1.359027710.1063/1.3590277 ↗
28. 10.1103/PhysRevB.84.24543610.1103/PhysRevB.84.245436 ↗
29. 10.1021/jp304068a10.1021/jp304068a ↗
30. 10.1021/jp306439h10.1021/jp306439h ↗
31. 10.1021/nl401265f10.1021/nl401265f ↗
32. 10.1063/1.490128310.1063/1.4901283 ↗
33. 10.1103/PhysRevLett.111.23680110.1103/PhysRevLett.111.236801 ↗
34. 10.1088/1367-2630/16/9/09304710.1088/1367-2630/16/9/093047 ↗
35. 10.1021/jacs.5b0555810.1021/jacs.5b05558 ↗
36. 10.1002/anie.20110095010.1002/anie.201100950 ↗
37. 10.1063/1.350268210.1063/1.3502682 ↗
38. 10.1063/1.277073210.1063/1.2770732 ↗
39. 10.1038/nnano.2011.21110.1038/nnano.2011.211 ↗
40. 10.1016/j.susc.2014.05.01510.1016/j.susc.2014.05.015 ↗
41. 10.1016/0039-6028(96)00163-X10.1016/0039-6028(96)00163-X ↗
42. Despite the strong reduction of the local density of states around the Fermi level, the molecular orbital at 0.5 V leading to the rich internal structure may still influence constant-current STM images at −0.5 V owing to its evanescent tail at the Fermi level. Similar observations were reported for Xe atoms on Ni(110), where the Xe 6s orbital was several eV above the Fermi energy and still contributed to STM images acquired at bias voltages close to 0 V.(64)
43. 10.1016/j.cplett.2007.03.00110.1016/j.cplett.2007.03.001 ↗
44. 10.1021/jp711454810.1021/jp7114548 ↗
45. 10.1021/nl104452x10.1021/nl104452x ↗
46. 10.1126/science.111344910.1126/science.1113449 ↗
47. 10.1103/PhysRevLett.104.17680210.1103/PhysRevLett.104.176802 ↗
48. 10.1103/PhysRevLett.107.03610110.1103/PhysRevLett.107.036101 ↗
49. 10.1021/jp512247n10.1021/jp512247n ↗
50. 10.1063/1.47852210.1063/1.478522 ↗
51. 10.1007/s00214-010-0852-110.1007/s00214-010-0852-1 ↗
52. 10.1063/1.354854610.1063/1.3548546 ↗
53. 10.1103/PhysRevB.88.20540310.1103/PhysRevB.88.205403 ↗
54. 10.1002/andp.20140009110.1002/andp.201400091 ↗
55. 10.1103/PhysRevB.50.1795310.1103/PhysRevB.50.17953 ↗
56. 10.1103/PhysRevLett.77.386510.1103/PhysRevLett.77.3865 ↗
57. 10.1016/0927-0256(96)00008-010.1016/0927-0256(96)00008-0 ↗
58. 10.1103/PhysRevB.54.1116910.1103/PhysRevB.54.11169 ↗
59. 10.1103/PhysRevB.59.175810.1103/PhysRevB.59.1758 ↗
60. 10.1002/jcc.2049510.1002/jcc.20495 ↗
61. 10.1088/0953-8984/23/39/39500110.1088/0953-8984/23/39/395001 ↗
62. 10.1103/PhysRevLett.50.199810.1103/PhysRevLett.50.1998 ↗
63. 10.1016/S1573-4331(08)00012-710.1016/S1573-4331(08)00012-7 ↗
64. 10.1126/science.272.5270.192110.1126/science.272.5270.1921 ↗