Determination of the dead-layer thickness for both p- and n-type HPGe detectors using the two-line method

2017 ◽  
Vol 315 (1) ◽  
pp. 95-101 ◽  
Author(s):  
Truong Thi Hong Loan ◽  
Vu Ngoc Ba ◽  
Truong Huu Ngan Thy ◽  
Huynh Thi Yen Hong ◽  
Ngo Quang Huy
2000 ◽  
Vol 655 ◽  
Author(s):  
L. J. Sinnamon ◽  
R. M. Bowman ◽  
J. M. Gregg

AbstractThin film capacitors with barium strontium titanate (BST) dielectric layers of 7.5 to 950 nm were fabricated by Pulsed Laser Deposition. XRD and EDX analyses confirmed a strongly oriented BST cubic perovskite phase with the desired cation stoichiometry. Room temperature frequency dispersion (ε100 kHz / ε100 Hz) for all capacitors was greater than 0.75. Absolute values for the dielectric constant were slightly lower than expected. This was attributed to the use of Au top electrodes since the same sample showed up to a threefold increase in dielectric constant when Pt was used in place of Au. Dielectric constant as a function of thicknesses greater than 70 nm, was fitted using the series capacitor model. The large interfacial parameter ratio di / εi of 0.40 ± 0.05 nm implied a significant dead-layer component within the capacitor structure. Modelled consideration of the dielectric behaviour for BST films, whose total thickness was below that of the dead layer, predicted anomalies in the plots of d/ ε against d at the dead layer thickness. For the SRO/BST/Au system studied, no anomaly was observed. Therefore, either (i) 7.5 nm is an upper limit for the total dead layer thickness in this system, or (ii) dielectric collapse is not associated with a distinct interfacial dead layer, and is instead due to a through-film effect.


2016 ◽  
Vol 40 (9) ◽  
pp. 096001 ◽  
Author(s):  
Hao Jiang ◽  
Qian Yue ◽  
Yu-Lan Li ◽  
Ke-Jun Kang ◽  
Yuan-Jing Li ◽  
...  

2009 ◽  
Vol 51 (9) ◽  
pp. 1929-1934 ◽  
Author(s):  
E. V. Ubyĭvovk ◽  
D. K. Loginov ◽  
I. Ya. Gerlovin ◽  
Yu. K. Dolgikh ◽  
Yu. P. Efimov ◽  
...  

Author(s):  
Noha Shaaban ◽  
Wael El Gammal ◽  
Hesham Nasif

The use of modeling programs to predict the response of HPGe detectors is increasing in importance due to the extensive laboratory work, both in term of source preparations and measuring time. MCNP code is a powerful and useful tool for the simulation of Ge-detector efficiency calibration. The experimental efficiency data and MCNP calculations based only on the known physical measurements of the HPGe crystal do not agree well in some detectors. Detector construction materials and surface dead layers must be well specified. The dead layer of Ge detector is one of the most important factors that affect the calculations. In addition, and if provided by the manufacturer, the dead layer may changes with time. Consequently, it is necessary to optimize the thickness of the detector’s dead layer in order to obtain more accurate results for the efficiency of the detector using Monte Carlo calculations. Our approach consists of employing hybrid UCODE-MCNP codes to optimize the dead layer of the Ge-crystal aiming at decreasing discrepancies between experimental and simulated data of the Ge detector efficiency. UCODE has two attributes that are not jointly available in other inverse models: (1) the ability to work with any mathematically based model or pre- or post processor with ASCII or text only input and output files, and (2) the inclusion of more informative statistics.


2004 ◽  
Vol 51 (6) ◽  
pp. 3090-3093 ◽  
Author(s):  
W. Dusi ◽  
A. Donati ◽  
G. Landini ◽  
E. Perillo ◽  
A. Raulo ◽  
...  

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