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Volumn 94, Issue 25, 2009, Pages

Temperature dependent charge-injection at the metal-organic semiconductor interface and density of states in pristine and doped pentacene

Author keywords

[No Author keywords available]

Indexed keywords

CARRIER INJECTION; DENSITY OF STATE; ELECTRICAL TRANSPORT; F4-TCNQ; HOLE INJECTION BARRIERS; METAL-ORGANIC SEMICONDUCTOR INTERFACES; PENTACENE; PENTACENE INTERFACE; PHYSICAL MECHANISM; TEMPERATURE DEPENDENT; TETRAFLUORO-TETRACYANOQUINODIMETHANE;

EID: 67649494448     PISSN: 00036951     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.3159835     Document Type: Article
Times cited : (15)

References (25)
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    • (2002) Org. Electron. , vol.3 , pp. 53
    • Gao, W.1    Kahn, A.2
  • 9
    • 0037113669 scopus 로고    scopus 로고
    • 0163-1829,. 10.1103/PhysRevB.66.195336
    • A. R. Volkel, R. A. Street, and D. Knipp, Phys. Rev. B 0163-1829 66, 195336 (2002). 10.1103/PhysRevB.66.195336
    • (2002) Phys. Rev. B , vol.66 , pp. 195336
    • Volkel, A.R.1    Street, R.A.2    Knipp, D.3
  • 15
    • 67649571631 scopus 로고    scopus 로고
    • Thesis, University of Basel.
    • C. Vanoni, Thesis, University of Basel, 2007.
    • (2007)
    • Vanoni, C.1
  • 19
    • 67649568066 scopus 로고    scopus 로고
    • The ratio A was evaluated from the ratio of the deposited thickness (6 ML for the doped and 20 ML for the undoped PC nanocrystal) equal to ∼0.3 and the ratio of the effective PC channel width of ∼1 observed by SEM of actual nanojunction, see Ref..
    • The ratio A was evaluated from the ratio of the deposited thickness (6 ML for the doped and 20 ML for the undoped PC nanocrystal) equal to ∼0.3 and the ratio of the effective PC channel width of ∼1 observed by SEM of actual nanojunction, see Ref..
  • 20
  • 21
    • 67649552162 scopus 로고    scopus 로고
    • We ascribe the difficulty to apply TLM method to undoped PC TFTs to the large non-Ohmic contact properties and its considerable influence on the short channel devices at low temperatures.
    • We ascribe the difficulty to apply TLM method to undoped PC TFTs to the large non-Ohmic contact properties and its considerable influence on the short channel devices at low temperatures.
  • 23
    • 0000606264 scopus 로고    scopus 로고
    • 0163-1829,. 10.1103/PhysRevB.57.12964
    • M. C. J. M. Vissenberg and M. Matters, Phys. Rev. B 0163-1829 57, 12964 (1998). 10.1103/PhysRevB.57.12964
    • (1998) Phys. Rev. B , vol.57 , pp. 12964
    • Vissenberg, M.C.J.M.1    Matters, M.2
  • 24
    • 67649527412 scopus 로고    scopus 로고
    • Here, pac was evaluated from the positive threshold gate voltage shift of ∼1 V of the doped-PC TFT compared to the pristine-PC TFT at room temperature. The total concentration of the F4 TCNQ molecules co-deposited in the PC film is equal to ∼4× 1019 cm-3. Therefore, the fraction of the electronically active F4 TCNQ is in the order of 10-2. Previous estimates of the doping efficiency of F4 TCNQ molecule to PC returned a value equal to ∼0.1 holes/dopant in vacuum. The lower doping efficiency by a factor of about 10 observed here, is ascribed to the brief (∼5 min) exposure of the sample to the ambient air during the transfer from the PC deposition chamber to the cryostat (see also Ref.).
    • Here, pac was evaluated from the positive threshold gate voltage shift of ∼1 V of the doped-PC TFT compared to the pristine-PC TFT at room temperature. The total concentration of the F4 TCNQ molecules co-deposited in the PC film is equal to ∼4× 1019 cm-3. Therefore, the fraction of the electronically active F4 TCNQ is in the order of 10-2. Previous estimates of the doping efficiency of F4 TCNQ molecule to PC returned a value equal to ∼0.1 holes/dopant in vacuum. The lower doping efficiency by a factor of about 10 observed here, is ascribed to the brief (∼5 min) exposure of the sample to the ambient air during the transfer from the PC deposition chamber to the cryostat (see also Ref.).
  • 25
    • 67649533855 scopus 로고    scopus 로고
    • The doping-induced states observed here is potentially consistent with the previously observed Vg -dependence of Rc in TFTs (Ref.); An increase of Rc upon increasing the negative Vg above 10 V can be ascribed to the resonantlike-injection from Au into the doping-induced states detuned by Vg.
    • The doping-induced states observed here is potentially consistent with the previously observed Vg -dependence of Rc in TFTs (Ref.); An increase of Rc upon increasing the negative Vg above 10 V can be ascribed to the resonantlike-injection from Au into the doping-induced states detuned by Vg.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.