CO and NH3 sensor properties and paramagnetic centers of nanocrystalline SnO2 modified by Pd and Ru

2011 ◽  
Vol 520 (3) ◽  
pp. 904-908 ◽  
Author(s):  
A.V. Marikutsa ◽  
M.N. Rumyantseva ◽  
A.M. Gaskov ◽  
E.A. Konstantinova ◽  
D.A. Grishina ◽  
...  
2013 ◽  
Vol 182 ◽  
pp. 555-564 ◽  
Author(s):  
Nataliya Vorobyeva ◽  
Marina Rumyantseva ◽  
Darya Filatova ◽  
Elizaveta Konstantinova ◽  
Diana Grishina ◽  
...  

2011 ◽  
Vol 25 ◽  
pp. 296-299 ◽  
Author(s):  
N. Vorobyeva ◽  
M. Rumyantseva ◽  
E. Konstantinova ◽  
D. Grishina ◽  
A. Gaskov

Sensors ◽  
2021 ◽  
Vol 21 (4) ◽  
pp. 1550
Author(s):  
Dominic Greiffenberg ◽  
Marie Andrä ◽  
Rebecca Barten ◽  
Anna Bergamaschi ◽  
Martin Brückner ◽  
...  

Chromium compensated GaAs or GaAs:Cr sensors provided by the Tomsk State University (Russia) were characterized using the low noise, charge integrating readout chip JUNGFRAU with a pixel pitch of 75 × 75 µm2 regarding its application as an X-ray detector at synchrotrons sources or FELs. Sensor properties such as dark current, resistivity, noise performance, spectral resolution capability and charge transport properties were measured and compared with results from a previous batch of GaAs:Cr sensors which were produced from wafers obtained from a different supplier. The properties of the sample from the later batch of sensors from 2017 show a resistivity of 1.69 × 109 Ω/cm, which is 47% higher compared to the previous batch from 2016. Moreover, its noise performance is 14% lower with a value of (101.65 ± 0.04) e− ENC and the resolution of a monochromatic 60 keV photo peak is significantly improved by 38% to a FWHM of 4.3%. Likely, this is due to improvements in charge collection, lower noise, and more homogeneous effective pixel size. In a previous work, a hole lifetime of 1.4 ns for GaAs:Cr sensors was determined for the sensors of the 2016 sensor batch, explaining the so-called “crater effect” which describes the occurrence of negative signals in the pixels around a pixel with a photon hit due to the missing hole contribution to the overall signal causing an incomplete signal induction. In this publication, the “crater effect” is further elaborated by measuring GaAs:Cr sensors using the sensors from 2017. The hole lifetime of these sensors was 2.5 ns. A focused photon beam was used to illuminate well defined positions along the pixels in order to corroborate the findings from the previous work and to further characterize the consequences of the “crater effect” on the detector operation.


2021 ◽  
Vol 726 ◽  
pp. 138662
Author(s):  
Alp Kılıç ◽  
Onur Alev ◽  
Okan Özdemir ◽  
Leyla Çolakerol Arslan ◽  
Serkan Büyükköse ◽  
...  

2021 ◽  
Vol 125 (12) ◽  
pp. 6773-6786
Author(s):  
Claudio José Magon ◽  
Harold Lozano Zarto ◽  
José Pedro Donoso ◽  
Hellmut Eckert ◽  
Sindy Devis ◽  
...  

2021 ◽  
Vol 0 (0) ◽  
Author(s):  
Alexander Ulyanov ◽  
Dmitrii Stolbov ◽  
Serguei Savilov

Abstract Jellyfish-like graphene nanoflakes (GNF), prepared by hydrocarbon pyrolysis, are studied with electron paramagnetic resonance (EPR) method. The results are supported by X-ray photoelectron spectroscopy (XPS) data. Oxidized (GNFox) and N-doped oxidized (N-GNFox) flakes exhibit an extremely high EPR response associated with a large interlayer interaction which is caused by the structure of nanoflakes and layer edges reached by oxygen. The GNFox and N-GNFox provide the localized and mobile paramagnetic centers which are silent in the pristine (GNF p ) and N-doped (N-GNF) samples. The change in the relative intensity of the line corresponding to delocalized electrons is parallel with the number of radicals in the quaternary N-group. The environment of localized and mobile electrons is different. The results can be important in GNF synthesis and for explanation of their features in applications, especially, in devices with high sensitivity to weak electromagnetic field.


Sign in / Sign up

Export Citation Format

Share Document