Abstract:The most widely used architecture in large-area amorphous silicon (a-Si) flat panel imagers is a passive pixel sensor (PPS), which consists of a detector and a readout switch. While the PPS has the advantage of being compact and amenable toward high-resolution imaging, reading small PPS output signals requires external column charge amplifiers that produce additional noise and reduce the minimum readable sensor input signal. This work presents a current-mediated amorphous silicon active pixel readout circuit t… Show more
“…6. The lower limit of the integration is usually determined from the frame rate of the imager [6]. From the noise spectrum in Fig.…”
Section: Measurements and Discussionmentioning
confidence: 99%
“…Using the theory presented previously in this section, the contribution from various noise sources is presented in Table 1. In order to produce low-noise images for X-ray modalities like fluoroscopy throughout the dosage range, the total electronic noise should be less than the quantum noise, which is approximately 1000 electrons for a-Se photoconductors at electric fields of 10 V/µm at fluoroscopy energy levels [6]. Table 1 shows that the total input referred noise is below the quantum noise limit of the X-ray imager.…”
Section: Measurements and Discussionmentioning
confidence: 99%
“…Since r oA (=1/λI dsA , λ = 0.04 typically for a-Si TFTs [6]) >> r oR we can simplify the above expression to yield, …”
“…6. The lower limit of the integration is usually determined from the frame rate of the imager [6]. From the noise spectrum in Fig.…”
Section: Measurements and Discussionmentioning
confidence: 99%
“…Using the theory presented previously in this section, the contribution from various noise sources is presented in Table 1. In order to produce low-noise images for X-ray modalities like fluoroscopy throughout the dosage range, the total electronic noise should be less than the quantum noise, which is approximately 1000 electrons for a-Se photoconductors at electric fields of 10 V/µm at fluoroscopy energy levels [6]. Table 1 shows that the total input referred noise is below the quantum noise limit of the X-ray imager.…”
Section: Measurements and Discussionmentioning
confidence: 99%
“…Since r oA (=1/λI dsA , λ = 0.04 typically for a-Si TFTs [6]) >> r oR we can simplify the above expression to yield, …”
“…The time dependence of (1) can be calculated as [2] and (b) AMI pixel circuit [3] According to (2), the current of the GP pixel circuits increases as it ages. Moreover, the major effect is due to C g2 , which is representative of charge injection component.…”
Section: Transient Shiftsmentioning
confidence: 99%
“…It has, therefore, become attractive for low-cost large-area backplanes for active matrix organic light emitting diode (AMOLED) displays [1] and active matrix imagers (AMIs) [2]. Figure 1 shows two different pixel circuits proposed for AMOLED displays [1] and X-ray imaging [3]. In the AMOLED pixel circuit, the current flowing through the OLED is controlled by an a-Si:H TFT (T1) while in the sensor pixel circuit, T1 is used to amplify the signal.…”
A reliable driving scheme that can compensate for the inherent instability of hydrogenated amorphous silicon (a-Si:H) thin film transistors (TFTs) is essential for implementation of large-area devices including displays and sensor arrays for bio-imaging applications. In particular, for high precision and high-resolution devices, the technique should be accurate and fast. A new driving scheme is presented that enables control of the DC and transient shift in the threshold voltage (V T ) and gate voltage of drive/amplifier TFT, while fulfilling the timing requirements for the different applications. The transient shift in the gate voltage has been known to contribute as much as 10% error in controlling the DC shift in the V T whereas it is less than 0.5% for the driving scheme presented here.
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