Electrical Transport — Modification of metal-organic interface using F4-TCNQ for enhanced hole injection properties in optoelectronic devices

Measurement evidence

Electrical Transport

Modification of metal-organic interface using F4-TCNQ for enhanced hole injection properties in optoelectronic devices · Rana O., Srivastava R., Chauhan G. et al. · Physica Status Solidi (A) Applications and Materials Science · 2012 · 2539-2545

4 measurement groups · 20 results

Reported values remain attached to the sample, method, conditions, extraction quality and source location that produced them.

J-V measurement and SCLC comparison

alpha-NPD hole-only devices with F4-TCNQ interfaces · Thin Film

F4-TCNQ thickness varied from 0, 1, 5 and 7 nm; observed current density compared with calculated SCLC J value.

Atmosphere
vacuum conditions
Geometry
ITO/F4-TCNQ(x nm)/alpha-NPD(250 nm)/F4-TCNQ(x nm)/Au
Context
model hole-only devices with unmodified and modified interfaces
Measurement source
p005 / article p.2543 · Results and discussion · Figure 3c
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
ITO Fermi level to alpha-NPD HOMO offset0.6 eVText
Rounded Reported
p005 / article p.2543 · Results and discussion · Figure 3c
alpha-NPD HOMO level5.5 eVText
Rounded Reported
p003 / article p.2541 · Experimental
F4-TCNQ thickness required for ohmic contact to alpha-NPDMarked as a best value within this paper7 nmabout in conclusionsText
Rounded Reported
p005 / article p.2543 · Results and discussion · Figure 3c

J-V measurement and injection-efficiency comparison with Child-law SCLC current

m-MTDATA hole-only devices with F4-TCNQ interfaces · Thin Film

J-V measured with Keithley 2400 in a vacuum cryostat; injection efficiency eta = Jobs/JSCLC calculated using dielectric constant 3 and TOF mobility literature values.

Temperature
room temperature
Atmosphere
vacuum conditions
Geometry
ITO/F4-TCNQ(x nm)/m-MTDATA(250 nm)/F4-TCNQ(x nm)/Au
Context
model hole-only devices with unmodified and 1 nm F4-TCNQ-modified interfaces
Measurement source
p005 / article p.2543 · Results and discussion · Figure 3a
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
m-MTDATA injection efficiency with bare electrodes at 3 V0.08Text
Exact Reported
p005 / article p.2543 · Results and discussion · Figure 3a
m-MTDATA HOMO level used in experimental design5.0 eVText
Rounded Reported
p003 / article p.2541 · Experimental
m-MTDATA injection efficiency after 1 nm F4-TCNQ interface layerMarked as a best value within this papernear to unity for all applied voltagesnear toText
Approximate
p005 / article p.2543 · Results and discussion · Figure 3a
F4-TCNQ thickness required for ohmic contact to m-MTDATAMarked as a best value within this paper1 nmText
Rounded Reported
p006 / article p.2544 · Conclusions

J-V measurement and SCLC comparison

spiro-TAD hole-only devices with F4-TCNQ interfaces · Thin Film

F4-TCNQ thickness varied from 0 to 7 nm; observed current density compared with calculated SCLC J value.

Atmosphere
vacuum conditions
Geometry
ITO/F4-TCNQ(x nm)/spiro-TAD(250 nm)/F4-TCNQ(x nm)/Au
Context
model hole-only devices with unmodified and modified interfaces
Measurement source
p005 / article p.2543 · Results and discussion · Figure 3b
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
ITO Fermi level to spiro-TAD HOMO offsetabout 0.5 eVaboutText
Approximate
p005 / article p.2543 · Results and discussion · Figure 3b
spiro-TAD HOMO level5.4 eVText
Rounded Reported
p003 / article p.2541 · Experimental
F4-TCNQ thickness required for ohmic contact to spiro-TADMarked as a best value within this paper7 nmText
Rounded Reported
p005 / article p.2543 · Results and discussion · Figure 3b

Kelvin probe method / scanning Kelvin probe microscopy incorporated with AFM

F4-TCNQ-coated Al, In, Ag, ITO and Au substrate series · Thin Film

Surface potential measured in ambient conditions; grounded metal films and gold probe head; work function estimated by adding surface-potential difference to probe work function.

Atmosphere
ambient conditions
Geometry
conducting substrate with F4-TCNQ thin film
Context
model F4-TCNQ/substrate interfaces, including x = 0 control
Measurement source
p003 / article p.2541 · Experimental · Figure 1
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Ag substrate work function near 7 nm F4-TCNQapproximately 5.3 eV at 7 nm from Figure 1avisual estimate from plotted axisFigure Axis
Approximate
p003 / article p.2541 · Results and discussion · Figure 1a
Al substrate work function with 7 nm F4-TCNQ4.3 eVText
Rounded Reported
p003 / article p.2541 · Results and discussion · Figure 1a
In substrate work function near 7 nm F4-TCNQapproximately 4.7 eV at 7 nm from Figure 1avisual estimate from plotted axisFigure Axis
Approximate
p003 / article p.2541 · Results and discussion · Figure 1a
F4-TCNQ-modified ITO and Au work function at 7 nm reported in Introduction5.35 eV for 7 nm adsorbed layerText
Rounded Reported
p002 / article p.2540 · Introduction
Oxygen-plasma-treated ITO work function4.8 eVText
Rounded Reported
p003 / article p.2541 · Experimental
ITO and Au substrate work function with 7 nm F4-TCNQMarked as a best value within this paper5.37 eVText
Rounded Reported
p003 / article p.2541 · Results and discussion · Figure 1a
Approximate saturation work function of modified substratesMarked as a best value within this papersaturate at about 5.37 eVaboutText
Approximate
p003 / article p.2541 · Results and discussion · Figure 1b
Bare conducting-substrate work-function range3.7-5.1 eVText
Range
p002 / article p.2540 · Introduction
Maximum work-function increase after F4-TCNQ modificationMarked as a best value within this paperabout 0.6 eV in nearly all casesaboutText
Approximate
p003 / article p.2541 · Results and discussion · Figure 1a
F4-TCNQ thickness for work-function saturationMarked as a best value within this paperabout 7 nmaboutText
Approximate
p003 / article p.2541 · Results and discussion · Figure 1a