A new phototransistor with uni-travelling-carrier and optically gradual coupling properties

Based on appropriate combination of different band-gap InGaAsP, a new edge-coupled two-terminal double heterojunction phototransistor (ECTT-DHPT) was designed and fabricated, which is double heterojunction, free-aluminium, and works under uni-travelling-carrier mode and optically gradual coupling mode. This device is fully compatible with monolithic micro-wave integrated circuits (MMIC) and heterojunction bipolar transistor (HBT) in material and process. The DC characteristics reveal that the new ECTT-DHPT can perform good optoelectronic mix operation and linear amplification operation by optically biased at two appropriate value respectively. Responsivity of more than 52 A/W and dark current of 70 nA (when V-EC = 1 V) were obtained.

A New Edge-Coupled Two-Terminal Double Heterojunction Phototransistor (ECTT-DHPT) and Its DC Characteristics

A new ECTT-DHPT with InGaAsP(lambda=1.55 mu m) as base and InGaAsP(lambda=1.3 mu m) as collector as well as waveguide was designed and fabricated, the DC characteristics reveal that the ECTT-DRPT can perform good optoelectronic mix operation and linear amplification operation by optically biased at two appropriate value respectively. Responsivity of more than 52A/W and dark current of 70nA (when V-ce=1V) were obtained.

Dual gate photo-thin film transistor with high photoconductive gain for high reliability, and low noise flat panel transparent imager

In this presentation, we report excellent electrical and optical characteristics of a dual gate photo thin film transistor (TFT) with bi-layer oxide channel, which was designed to provide virgin threshold voltage (V T) control, improve the negative bias illumination temperature stress (NBITS) reliability, and offer high photoconductive gain. In order to address the photo-sensitivity of phototransistor for the incoming light, top transparent InZnO (IZO) gate was employed, which enables the independent gate control of dual gate photo-TFT without having any degradation of its photosensitivity. Considering optimum initial V T and NBITS reliability for the device operation, the top gate bias was judiciously chosen. In addition, the speed and noise performance of the photo-TFT is competitive with silicon photo-transistors, and more importantly, its superiority lies in optical transparency. © 2011 IEEE.

A novel high sensitivity CE-PTHPT for optical fiber communication

Planar punch through heterojunction phototransistors with a novel emitter control electrode and ion- implanted isolation (CE-PTHPT) are investigated. The phototransistors have a working voltage of 3-10V and high sensitivity at low input power. The base of the transistor is completely depleted under operating condition. Base current is zero. The CE-PTHPT has an increased speed and a decreased noise. The novel CE-PTHPT has been fabricated in this paper. The optical gain of GaAlAs/GaAs CE-PTHPT for the incident light power 1.3 and 43nw with the wavelength of 0.8 mu m reached 1260 and 8108. The input noise current calculated is 5.46 x 10(-16) A/H-z(1/2). For polysilicon emitter CE-PTHPT, the optical gain is 3083 at the input power of 0.174 mu w. The optical gain of InGaAs/InP CE-PTHPT reaches 350 for an incident power of 0.3 mu w at the wavelength of 1.55 mu m. The CE-PTHPT detectors is promising as photo detectors for optical fiber communication system.

Organic field-effect transistors and phototransistors based on amorphous materials

A comparison between the charge transport properties in low molecular amorphous thin films of spiro-linked compound and their corresponding parent compound has been demonstrated. The field-effect transistor method is used for extracting physical parameters such as field-effect mobility of charge carriers, ON/OFF ratios, and stability. In addition, phototransistors have been fabricated and demonstrated for the first time by using organic materials. In this case, asymmetrically spiro-linked compounds are used as active materials. The active materials used in this study can be divided into three classes, namely Spiro-linked compounds (symmetrically spiro-linked compounds), the corresponding parent-compounds, and photosensitive spiro-linked compounds (asymmetrically spiro-linked com-pounds). Some of symmetrically spiro-linked compounds used in this study were 2,2',7,7'-Tetrakis-(di-phenylamino)-9,9'-spirobifluorene (Spiro-TAD),2,2',7,7'-Tetrakis-(N,N'-di-p-methylphenylamino)-9,9'-spirobifluorene (Spiro-TTB), 2,2',7,7'-Tetra-(m-tolyl-phenylamino)-9,9'-spirobifluorene (Spiro-TPD), and 2,2Ž,7,7Ž-Tetra-(N-phenyl-1-naphtylamine)-9,9Ž-spirobifluorene (Spiro alpha-NPB). Related parent compounds of the symmetrically spiro-linked compound used in this study were N,N,N',N'-Tetraphenylbenzidine (TAD), N,N,N',N'-Tetrakis(4-methylphenyl)benzidine (TTB), N,N'-Bis(3-methylphenyl)-(1,1'-biphenyl)-4,4'-diamine (TPD), and N,N'-Diphenyl-N,N'-bis(1-naphthyl)-1,1'-biphenyl-4,4'-diamine (alpha-NPB). The photosensitive asymmetrically spiro-linked compounds used in this study were 2,7-bis-(N,N'-diphenylamino)-2',7'-bis(biphenyl-4-yl)-9,9'-spirobifluorene (Spiro-DPSP), and 2,7-bis-(N,N'-diphenylamino)-2',7'-bis(spirobifluorene-2-yl)-9,9'-spirobifluorene (Spiro-DPSP^2). It was found that the field-effect mobilities of charge carriers in thin films of symmetrically spiro-linked compounds and their corresponding parent compounds are in the same order of magnitude (~10^-5 cm^2/Vs). However, the thin films of the parent compounds were easily crystallized after the samples have been exposed in ambient atmosphere and at room temperature for three days. In contrast, the thin films and the transistor characteristics of symmetrically spiro-linked compound did not change significantly after the samples have been stored in ambient atmosphere and at room temperature for several months. Furthermore, temperature dependence of the mobility was analyzed in two models, namely the Arrhenius model and the Gaussian Disorder model. The Arrhenius model tends to give a high value of the prefactor mobility. However, it is difficult to distinguish whether the temperature behaviors of the material under consideration follows the Arrhenius model or the Gaussian Disorder model due to the narrow accessible range of the temperatures. For the first time, phototransistors have been fabricated and demonstrated by using organic materials. In this case, asymmetrically spiro-linked compounds are used as active materials. Intramolecular charge transfer between a bis(diphenylamino)biphenyl unit and a sexiphenyl unit leads to an increase in charge carrier density, providing the amplification effect. The operational responsivity of better than 1 A/W can be obtained for ultraviolet light at 370 nm, making the device interesting for sensor applications. This result offers a new potential application of organic thin film phototransistors as low-light level and low-cost visible blind ultraviolet photodetectors.

Synthese und Charakterisierung von Spirocyclopentadithiophenen

Im Rahmen dieser Arbeit wurde eine Syntheseroute zu einem neuartigen heteroanalogen Spirobifluoren auf Basis von Thiophen entwickelt und optimiert. Der neue Spirokern konnte durch Anbringung von Elektronendonor- bzw. Elektronenakzeptorgruppen funktionalisiert werden. Die erhaltenen Funktionsmaterialien wurden spektroskopisch (Ultraviolet-Visible, Fluoreszenz), thermoanalytisch (Thermogravimetrische Analyse, Differential Thermo Analysis, Differential Scanning Calorimetry), elektrochemisch (Cyclovoltammetrie) sowie teilweise mittels Feldeffekttransistor charaktrisiert.Zur Totalsynthese des neuen auf Thiophen basierenden Spirokerns 4,4´-Spirobi[cyclopenta[2,1-b:3,4-b´]dithiophen] (SCPDT) wurde eine Syntheseroute entworfen, die ausgehend von Thiophen keine weiteren aufwändigen Precursormoleküle voraussetzt. Durch die Anbringung von stabilisierenden Endgruppen war es möglich neuartige Funktionsmaterialien mit niedrigem HOMO-LUMO-Gap herzustellen. Die phenyl- bzw. biphenylsubstituierten Spirocyclopentadithiophene 4P-SCPDT und 4BP-SCPDT sind im Vergleich zu den analogen, auf Spirobifluoren basierenden Verbindungen (Spiroquaterthiophen und Spirosexiphenyl) deutlich leichter oxidier- und reduzierbar. Das erniedrigte HOMO-LUMO-Gap ist auch im Absorptions- und Fluoreszenzspektrum durch die im Vergleich zu den spirobifluorenanalogen Molekülen bathochrome bzw. bathofluore Verschiebung deutlich erkennbar. Sehr gut sind die Ergebnisse der Feldeffekttransistor- und Phototransistor-Messungen an aufgedampfem 4P-SCPDT. So lässt sich eine Lochbeweglichkeit von 2*10^-4 cm2/Vs ermitteln. Dies ist die höchste Lochbeweglichkeit, die bei Spiromolekülen im amorphen Film mit einem bottom-contact FET gemessen wurde, wobei die Grenzfläche zwischen Elektrode und Halbleiter noch nicht optimiert wurde. Selbst nach zehnmonatiger Lagerung unter Atmosphärenbedingungen bei Raumtemperatur konnten nahezu die gleichen Werte gemessen werden. Dieses Ergebnis unterstreicht die morphologische Stabilität des amorphen Filmes. Unter Bestrahlung mit UV-Licht zeigt sich ein ausgeprägter photovoltaischer Effekt. Das überrascht, da 4P-SCPDT kein typisches Donor-Akzeptor-Molekül ist. Das gemessene Ansprechvermögen (Verhältnis des elektrischen Output zum optischen Input) ist höher als das von polykristallinem Kupfer-Phthalocyanin (CuPc), konjugierten Polymeren oder anderen Spiromolekülen. Um die Lochleitungs- bzw. Elektronenleitungseigenschaften zu optimieren wurden desweiteren noch Diphenylaminophenyl-, Diphenylaminothiophenyl-, Perfluorhexylthiophenyl und Tricyanovinyl-Endgruppen an den den SCPDT-Kern angebracht und die erhaltenen Funktionsmaterialien charakterisiert.

Photodetection with gate-controlled lateral BJTs from standard CMOS technology

The silicon-based gate-controlled lateral bipolar junction transistor (BJT) is a controllable four-terminal photodetector with very high responsivity at low-light intensities. It is a hybrid device composed of a MOSFET, a lateral BJT, and a vertical BJT. Using sufficient gate bias to operate the MOS transistor in inversion mode, the photodetector allows for increasing the photocurrent gain by 106 at low light intensities when the base-emitter voltage is smaller than 0.4 V, and BJT is off. Two operation modes, with constant voltage bias between gate and emitter/source terminals and between gate and base/body terminals, allow for tuning the photoresponse from sublinear to slightly above linear, satisfying the application requirements for wide dynamic range, high-contrast, or linear imaging. MOSFETs from a standard 0.18-μm triple-well complementary-metal oxide semiconductor technology with a width to length ratio of 8 μm /2 μm and a total area of ∼ 500μm2 are used. When using this area, the responsivities are 16-20 kA/W. © 2001-2012 IEEE.