Skip to main content
. 2017 Apr 20;7:46561. doi: 10.1038/srep46561

Table 1. Experimental data on the carbon-metal distance d C and the energy shift ΔE IS between the interface state and the surface state for single layers of flat-lying organic molecules and graphene layers on metal surfaces.

# System dC(Å) ΔEIS(eV)
2 ZnPc/Cu(111) 2.49(3)41 0.2241
3 F16ZnPc/Cu(111) 2.66(10)41 0.1241
4 PTCDA/Ag(111)(LT-Phase) 2.81(2)44 0.56(3)6
5 PTCDA/Ag(100) 2.81(2)40 0.95(7)7
6 CuPc/PTCDA/Ag(111) 2.8145 0.7246
7 PTCDA/Ag(111) 2.86(1)37 0.665
8 NTCDA/Ag(111) 3.00(2)47 0.44(2)6,26
9 TiOPc/Ag(111) 3.00(3)48 0.3146
10 H2Pc/Ag(111) 3.07(7)49 0.32(3)50
11 Tc/Ag(111) 3.1643 0.2251
12 PFPEN/Ag(111) 3.16(6)52 0.21(6)46
15 PTCDA/Au(111) 3.27(2)53 0.164(4)11
1 g/Ru(0001)(L-Area) 2.20(7)54,55,56,57 1.67(7)54
13 g/Cu(111) 3.2636 0.2458
14 g/Cu(111) 3.2636 0.1559
16 g/15ML-Ag(111)/Ir(111) 3.3336 0.2060
17 g/Ir(111) 3.38(4)61, * 0.0062
18 g/Ru(0001)(H-Area) 3.70(7)54,55,56,57 0.00(6)54
  PTCDA/Ag(100)(DFT) 2.81(2)40 0.637
  PTCDA/Ag(111)(DFT) 2.86(1)53 0.5624
  NTCDA/Ag(111)(DFT) 3.00(2)47 0.3224

The numbering corresponds to that of the data points in Fig. 3 in addition, results of DFT calculations are listed for NTCDA and PTCDA on Ag surfaces.(Annotations: energy relative to the one of the respective surface resonance of the bare substrate, relative to energy of Shockley state of the bare substrate from ref. 63, *average distance).