Hot Carrier Induced Leakage Current Instability in Metal Induced Laterally Crystallized n-type Poly-Silicon Thin Film Transistors

2006 ◽  
Author(s):  
Zhen Zhu ◽  
Mingxiang Wang ◽  
Dongli Zhang ◽  
Man Wong
Keyword(s):  
Thin Film ◽  
Leakage Current ◽  
Thin Film Transistors ◽  
Silicon Thin Film ◽  
Hot Carrier ◽  
Poly Silicon ◽  
Current Instability

Hot Carrier Effect in Low Temperature Poly-Silicon Thin Film Transistors

2000 ◽  
Author(s):  
Y. Uraoka ◽  
T. Hatayama ◽  
T. Fuyuki ◽  
T. Kawamura ◽  
Y. Tsuchihashi
Keyword(s):  
Thin Film ◽  
Low Temperature ◽  
Thin Film Transistors ◽  
Silicon Thin Film ◽  
Hot Carrier ◽  
Poly Silicon ◽  
Carrier Effect ◽  
Hot Carrier Effect

Hydrogen in Ultralow Temperature SiO2for Nanocrystalline Silicon Thin Film Transistors

2004 ◽  
Vol 814 ◽  
Author(s):  
Alex Kattamis ◽  
I-Chun Cheng ◽  
Steve Allen ◽  
Sigurd Wagner
Keyword(s):  
Thin Film ◽  
Leakage Current ◽  
Current Density ◽  
Thin Film Transistors ◽  
Secondary Ion Mass Spectrometry ◽  
Crystalline Silicon ◽  
Chemical Vapor ◽  
Nanocrystalline Silicon ◽  
Film Deposition ◽  
Silicon Thin Film

AbstractNanocrystalline silicon is a candidate material for fabricating thin film transistors with high carrier mobilities on plastic substrates. A major issue in the processing of nanocrystalline silicon thin film transistors (nc-Si:H TFTs) at ultralow temperatures is the quality of the SiO2gate dielectric. SiO2deposited at less than 250°C by radio frequency plasma enhanced chemical vapor deposition (rf-PECVD), and not annealed at high temperature after deposition, exhibits high leakage current and voltage shifts when incorporated into TFT's. Secondary ion mass spectrometry (SIMS) measurements show that the hydrogen concentration (NH) in PECVD oxide deposited at 150°C on crystalline silicon (x-Si) is ∼ 0.8 at. %. This is much higher than in thermal oxides on x-Si, which display concentrations of less than 0.003 at. %. The leakage current density for thermal oxides on x-Si at a bias of 10 V is ∼9×10−6A/cm2whereas for 200°C PECVD oxides on nc-Si:H the current is ∼1×10−4A/cm2. As the temperature of the SiO2deposition is reduced to 150°C the current density rises by up to two orders of magnitude more. The H which is suspected to cause the leakage current across the PECVD oxide originates from the nc-Si:H substrate and the SiH4source gas. We analyzed the 300-nm gate oxide in capacitor structures of Al / SiO2/n+nc-Si:H / Cr / glass, Al / SiO2/ n+nc-Si:H / x-Si, and Al / SiO2/ x-Si. Vacuum annealing the nc-Si:H prior to PECVD of the oxide drives H out of the nc-Si:H film and reduces the amount of H incorporated into the oxide that is deposited on top. SiO2film deposition from SiH4and N2O at high He dilution has a still greater effect on lowering NH. The leakage current at a 10 V bias dropped from ∼1×10−4A/cm2to about ∼2×10−6A/cm2using He dilution at 250°C, and the vacuum anneal of the nc-Si:H lowered it by an additional factor of two. Thus we observe that both the nc-Si:H anneal and the SiO2deposition at high He dilution lessen the gate leakage current.

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