The Molecule–Metal Interface 2013
DOI: 10.1002/9783527653171.ch7
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Fundamental Electronic Structure of Organic Solids and Their Interfaces by Photoemission Spectroscopy and Related Methods

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Cited by 3 publications
(5 citation statements)
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“…alkali metal doping, and formation of metal-molecule and molecule-molecule interfaces with stronger chemical interactions) produces new electronic states [72][73][74][75][76][77][78][79][80][81], electronic states for superconducting phase [7,82], and in some cases enhance a wave function localization to result in a Mott-Hubbard insulator even at room temperature, giving a half-filled energy level in the gap (I, III, V) [83][84][85] (see sections 5.4.3.5). • A tiny amount of excess charges injected into the packing structure can produce larger changes in the electronic structure than supposed (formation of a very small polaron, small polaron, and large polaron, and related geometrical structure change in the molecule and molecular crystal as well) (I, III, IV) [33,43,[86][87][88] (see section 5.2.1).…”
Section: Summary Of Important Features Of Molecular Solids: the Natur...mentioning
confidence: 99%
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“…alkali metal doping, and formation of metal-molecule and molecule-molecule interfaces with stronger chemical interactions) produces new electronic states [72][73][74][75][76][77][78][79][80][81], electronic states for superconducting phase [7,82], and in some cases enhance a wave function localization to result in a Mott-Hubbard insulator even at room temperature, giving a half-filled energy level in the gap (I, III, V) [83][84][85] (see sections 5.4.3.5). • A tiny amount of excess charges injected into the packing structure can produce larger changes in the electronic structure than supposed (formation of a very small polaron, small polaron, and large polaron, and related geometrical structure change in the molecule and molecular crystal as well) (I, III, IV) [33,43,[86][87][88] (see section 5.2.1).…”
Section: Summary Of Important Features Of Molecular Solids: the Natur...mentioning
confidence: 99%
“…• There are various phonons with largely deferent energies (in the order of 10 −1 -10 −3 eV), which originate from intramolecular vibrations and intermolecular/crystal vibrations. These phonons result in a variety of electronphonon coupling, which give various quasiparticles and hierarchical polarons with different polaron binding energies [10,11,88] that impact not only on charge transport dynamics but also produce gap states (I, III, IV) [86,87,93,94] (see section 5.2.1). • Both thin film and bulk organic semiconductor materials have highly anisotropic electronic properties, such as molecular-orientation-dependent electronic states, anisotropic charge transport, and anisotropic optical properties (I, III, IV) [54,[95][96][97][98][99] (see section 5.1.1).…”
Section: Summary Of Important Features Of Molecular Solids: the Natur...mentioning
confidence: 99%
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“…Different values for IE and EA can be obtained from cyclic voltammetry (CV) and from direct/inverse photoelectron spectroscopy (PES/IPES). The energy gaps determined by optical absorption, photocurrent measurements, CV, scanning tunnelling spectroscopy (STS) or PES/IPES differ from each other [40][41][42][43][44][45][46]. Two main reasons for these deviations should be considered here.…”
Section: Introductionmentioning
confidence: 99%
“…First of all, the measurements are done on samples prepared by the same techniques as the films used in devices. Additionally, the creation of a hole by PES and the insertion of an electron by IPES in thin films is the closest experimental access to the transport level because the final states after PES/ IPES excitation are similar to the transport states [41,45]. These transport levels for electrons and hole are defined by the molecular radical ion, where the charge carrier is located, and the interaction with the polarisable environment [2,47].…”
Section: Introductionmentioning
confidence: 99%