Photoemission measurements reveal energy level shifts toward the Fermi level when a strong electron acceptor ͑tetrafluoro-tetracyanoquinodimethane, F4-TCNQ͒ is deposited on pristine layers of 4,4Ј ,4Љ-tris͑N , N-diphenyl-amino͒triphenylamine ͑TDATA͒ or 4,4Ј-bis͑N-carbazolyl͒biphenyl ͑CBP͒. The shifts of the TDATA and CBP energy levels toward the Fermi level of the Au substrate could, in principle, arise from p-type doping of the intrinsic organic layers. While this indeed takes place in TDATA, doping of CBP by F4-TCNQ, i.e., charge transfer complex formation, does not occur. The shifts observed in CBP arise from the diffusion of F4-TCNQ toward the Au substrate, which modifies the buried metal surface potential, leading to a realignment of the energy levels of the organic overlayer. © 2009 American Institute of Physics. ͓DOI: 10.1063/1.3213547͔ Strong electron acceptor molecules are frequently used for electrical doping of hole transport layers in organic electronic devices. 1-4 They yield improved device performance due to organic/organic ͑O/O͒ charge transfer complex ͑CTC͒ formation in the codeposited thin films, which increases the layer conductivity and lowers the hole injection barrier ͑HIB; defined as energy difference between E F and the highest occupied molecular orbital onset͒ at the anode ͑p-type doping͒. Strong electron acceptors can also be used to precisely adjust the energy levels at organic/metal ͑O/M͒ interfaces, 5,6 even in the absence of doping. In this case, an O/M CTC ͑Ref. 7͒ is formed, which increases the effective substrate surface potential and thus reduces the HIB for any subsequently deposited organic material. 5,6 Note that HIB lowering due to O/M CTC formation may be misinterpreted as p-type doping of the organic layer ͑O/O CTC͒ because a shift of the donor energy levels toward the substrate Fermi level ͑E F ͒ occurs in both cases. Acceptors are often small molecules like tetrafluoro-tetracyanoquinodimethane ͑F4-TCNQ͒ ͓chemical structure shown in Fig. 1͑a͔͒, which can readily diffuse throughout crystalline organic layers; 8 furthermore, diffusion through amorphous organic layers may also occur, particularly when intermolecular interactions are weak. In such cases, the acceptor may reach the metal substrate ͓Fig. 1͑b͔͒ via diffusion and may form O/M CTCs. It may thus be difficult to identify the underlying mechanism that results in observed energy level shifts for organic donor/acceptor heterosystems, as O/M CTC formation may mimic p-type doping.To clarify the role of acceptor interdiffusion on the energy levels in organic heterosystems, we used ultraviolet photoelectron spectroscopy ͑UPS͒ to investigate the combination of F4-TCNQ with the donor 4,4Ј ,4Љ-tris͑N , N-diphenyl-amino͒triphenylamine ͑TDATA͒ and 4 , 4Ј-di͑N-carbazolyl͒biphenyl ͑CBP͒ ͓Fig. 1͑a͔͒, respectively, on Au substrates. While TDATA can be doped with F4-TCNQ, 9,10 the ionization energy of CBP with 6.3 eV ͑Ref. 11͒ is too large to allow for CTC formation with F4-TCNQ. Both TDATA and CBP form amorphous films, 12 which rul...