Photon counting performance of amorphous selenium and its dependence on detector structure

Photon counting detectors (PCD) have the potential to improve x-ray imaging, however they are still hindered by high production costs and performance limitations. By using amorphous Selenium (a-Se) the cost of PCDs can be significantly reduced compared to currently used crystalline semiconductors and enable large area deposition. To overcome the limitation of low carrier mobility and low charge conversion gain in a-Se, we are developing a novel direct conversion a-Se field-Shaping multi-Well Avalanche Detector (SWAD). SWADs multi-well, dual grid design creates separate non-avalanche interaction (bulk) and avalanche sensing (well) regions, achieving depth-independent avalanche gain. Unipolar time differential (UTD) charge sensing, combined with tunable avalanche gain in the well region allows for fast timing and comparable charge conversion gain to crystalline semiconductors. In the present work we developed a probability based numerical simulation to model the charge generation, transport and signal collection of three different a-Se detector configurations and systematically show the improvements in energy resolution attributed to UTD charge sensing and avalanche gain. Pulse height spectra (PHS) for each detector structure, exposed to a filtered 241Am source, are simulated and compared against previously published PHS measurements of a conventional a-Se detector. We observed excellent agreement between our simulation of planar a-Se and the measured results. The energy resolution of each generated PHS was estimated by the full-width-at-half-maximum (FWHM) of the primary photo-peak. The energy resolution significantly improved from ~33 keV for the planar a-Se detector to ~7 keV for SWAD utilizing UTD charge sensing and avalanche gain.

[1]  Björn Cederström,et al.  Physical characterization of a scanning photon counting digital mammography system based on Si-strip detectors. , 2007, Medical physics.

[2]  William C. Barber,et al.  Fast photon counting CdTe detectors for diagnostic clinical CT: dynamic range, stability, and temporal response , 2010, Medical Imaging.

[3]  Polad M Shikhaliev,et al.  Photon counting multienergy x-ray imaging: effect of the characteristic x rays on detector performance. , 2009, Medical physics.

[4]  Erik Fredenberg,et al.  Spectral and dual-energy X-ray imaging for medical applications , 2018, 2101.00873.

[5]  S. Ramo Currents Induced by Electron Motion , 1939, Proceedings of the IRE.

[6]  I. Sechopoulos A review of breast tomosynthesis. Part I. The image acquisition process. , 2013, Medical physics.

[7]  John A. Rowlands,et al.  Photon counting pixel architecture for x-ray and gamma-ray imaging applications , 2007, SPIE Medical Imaging.

[8]  Erik Fredenberg,et al.  Energy resolution of a photon-counting silicon strip detector , 2010, 2101.07789.

[9]  S. Kasap,et al.  Modelling of photoinduced discharge of photoreceptors under pulsed photoexcitation: small and large signal xerographic time-of-flight analysis , 2000 .

[10]  M. Z. Kabir,et al.  Sensitivity of x-ray photoconductors: Charge trapping and absorption-limited universal sensitivity curves , 2002 .

[11]  Fumihiko Andoh,et al.  A CMOS imager hybridized to an avalanche multiplied film , 1997 .

[12]  R. K. Swank Absorption and noise in x‐ray phosphors , 1973 .

[13]  Mats Danielsson,et al.  Single-shot dual-energy subtraction mammography with electronic spectrum splitting: feasibility. , 2006, European journal of radiology.

[14]  J A Rowlands,et al.  X-ray imaging with amorphous selenium: Pulse height measurements of avalanche gain fluctuations. , 2006, Medical physics.

[15]  John A. Rowlands,et al.  Measurement of x-ray photogeneration in amorphous selenium , 1999 .

[16]  Nataly Wieberneit,et al.  Characterization of Cystic Lesions by Spectral Mammography: Results of a Clinical Pilot Study , 2016, Investigative radiology.

[17]  Denny L. Y. Lee Selenium detector with a grid for selenium charge gain , 2005, SPIE Medical Imaging.

[18]  W Zhao,et al.  A field-shaping multi-well avalanche detector for direct conversion amorphous selenium. , 2013, Medical physics.

[19]  Katsuyuki Taguchi,et al.  Spatio-energetic cross talk in photon counting detectors: Detector model and correlated Poisson data generator. , 2016 .

[20]  K. Taguchi,et al.  Vision 20/20: Single photon counting x-ray detectors in medical imaging. , 2013, Medical physics.

[21]  J. A. Rowlands,et al.  Unipolar time-differential charge sensing in non-dispersive amorphous solids , 2013 .

[22]  John A. Rowlands,et al.  Photon counting readout pixel array in 0.18-μm CMOS technology for on-line gamma-ray imaging of 103palladium seeds for permanent breast seed implant (PBSI) brachytherapy , 2008, SPIE Medical Imaging.

[23]  E. Nygard,et al.  Photon counting energy dispersive detector arrays for x-ray imaging , 2007, 2007 IEEE Nuclear Science Symposium Conference Record.

[24]  Kenkichi Tanioka,et al.  Electroded avalanche amorphous selenium (a-Se) photosensor. , 2012, Current applied physics : the official journal of the Korean Physical Society.

[25]  E. Montroll,et al.  Anomalous transit-time dispersion in amorphous solids , 1975 .

[26]  Wei Zhao,et al.  Toward Scintillator High‐Gain Avalanche Rushing Photoconductor Active Matrix Flat Panel Imager (SHARP‐AMFPI): Initial fabrication and characterization , 2018, Medical physics.

[27]  Erik Fredenberg,et al.  A photon-counting detector for dual-energy breast tomosynthesis , 2009, Medical Imaging.

[28]  Erik Fredenberg,et al.  Breast‐density measurement using photon‐counting spectral mammography , 2017, Medical physics.

[29]  S. Kasap,et al.  Study of photogenerated charge carrier dispersion in chlorinated a‐Se:0.3%As by the interrupted field time‐of‐flight technique , 1993 .

[30]  D. Bale,et al.  CdZnTe Semiconductor Detectors for Spectroscopic X-ray Imaging , 2008, IEEE Transactions on Nuclear Science.

[31]  W. Heindel,et al.  Digital mammography screening with photon-counting technique: can a high diagnostic performance be realized at low mean glandular dose? , 2014, Radiology.

[32]  Wei Zhao,et al.  Development of solid-state avalanche amorphous selenium for medical imaging. , 2015, Medical physics.

[33]  R. F. Wagner,et al.  SNR and DQE analysis of broad spectrum X-ray imaging , 1985 .

[34]  Wei Zhao,et al.  SWAD: transient conductivity and pulse-height spectrum , 2017, Medical Imaging.

[35]  W. Shockley Currents to Conductors Induced by a Moving Point Charge , 1938 .

[36]  Bahaa Ghammraoui,et al.  Investigating the feasibility of classifying breast microcalcifications using photon‐counting spectral mammography: A simulation study , 2017, Medical physics.

[37]  Taly Gilat Schmidt,et al.  Optimal "image-based" weighting for energy-resolved CT. , 2009, Medical physics.

[38]  K. Taketoshi,et al.  An avalanche-mode amorphous Selenium photoconductive layer for use as a camera tube target , 1987, IEEE Electron Device Letters.

[39]  Safa Kasap,et al.  Amorphous selenium and its alloys from early xeroradiography to high resolution X‐ray image detectors and ultrasensitive imaging tubes , 2009 .

[40]  M. Danielsson,et al.  Computer simulations and performance measurements on a silicon strip detector for edge-on imaging , 1999, 1999 IEEE Nuclear Science Symposium. Conference Record. 1999 Nuclear Science Symposium and Medical Imaging Conference (Cat. No.99CH37019).

[41]  J. Rowlands,et al.  Direct-conversion flat-panel imager with avalanche gain: feasibility investigation for HARP-AMFPI. , 2008, Medical physics.

[42]  G. Pfister,et al.  Dispersive (non-Gaussian) transient transport in disordered solids , 1978 .

[43]  G. W. Wright,et al.  Factors limiting the performance of CdZnTe detectors , 2005, IEEE Transactions on Nuclear Science.

[44]  G. Pellegrini,et al.  Performance limits of a 55-/spl mu/m pixel CdTe detector , 2006, IEEE Transactions on Nuclear Science.