|
|
|
|
LEADER |
01000caa a22002652 4500 |
001 |
NLM375980660 |
003 |
DE-627 |
005 |
20240905233010.0 |
007 |
cr uuu---uuuuu |
008 |
240808s2024 xx |||||o 00| ||eng c |
024 |
7 |
|
|a 10.1107/S160057752400643X
|2 doi
|
028 |
5 |
2 |
|a pubmed24n1524.xml
|
035 |
|
|
|a (DE-627)NLM375980660
|
035 |
|
|
|a (NLM)39110677
|
040 |
|
|
|a DE-627
|b ger
|c DE-627
|e rakwb
|
041 |
|
|
|a eng
|
100 |
1 |
|
|a Franklin, Lena A
|e verfasserin
|4 aut
|
245 |
1 |
0 |
|a Characterizing electron-collecting CdTe for use in a 77 ns burst-rate imager
|
264 |
|
1 |
|c 2024
|
336 |
|
|
|a Text
|b txt
|2 rdacontent
|
337 |
|
|
|a ƒaComputermedien
|b c
|2 rdamedia
|
338 |
|
|
|a ƒa Online-Ressource
|b cr
|2 rdacarrier
|
500 |
|
|
|a Date Revised 05.09.2024
|
500 |
|
|
|a published: Print-Electronic
|
500 |
|
|
|a Citation Status PubMed-not-MEDLINE
|
520 |
|
|
|a open access.
|
520 |
|
|
|a The Keck-PAD (pixel array detector) was developed at Cornell as a burst-rate imager capable of recording images from successive electron bunches (153 ns period) from the Advanced Photon Source (APS). Both Si and hole-collecting Schottky CdTe have been successfully bonded to this ASIC (application-specific integrated circuit) and used with this frame rate. The facility upgrades at the APS will lower the bunch period to 77 ns, which will require modifications to the Keck-PAD electronics to image properly at this reduced period. In addition, operation at high X-ray energies will require a different sensor material having a shorter charge collection time. For the target energy of 40 keV for this project, simulations have shown that electron-collecting CdTe should allow >90% charge collection within 35 ns. This collection time will be sufficient to sample the signal from one frame and prepare for the next. 750 µm-thick electron-collecting Schottky CdTe has been obtained from Acrorad and bonded to two different charge-integrating ASICs developed at Cornell, the Keck-PAD and the CU-APS-PAD. Carrier mobility has been investigated using the detector response to single X-ray bunches at the Cornell High Energy Synchrotron Source and to a pulsed optical laser. The tests indicate that the collection time will meet the requirements for 77 ns imaging
|
650 |
|
4 |
|a Journal Article
|
650 |
|
4 |
|a X-ray detector
|
650 |
|
4 |
|a cadmium telluride
|
650 |
|
4 |
|a high-Z sensor
|
650 |
|
4 |
|a pixel array detector
|
700 |
1 |
|
|a Brown, Nicholas J
|e verfasserin
|4 aut
|
700 |
1 |
|
|a Gruner, Sol M
|e verfasserin
|4 aut
|
700 |
1 |
|
|a Met-Hoxha, Elida
|e verfasserin
|4 aut
|
700 |
1 |
|
|a Tate, Mark W
|e verfasserin
|4 aut
|
700 |
1 |
|
|a Thom-Levy, Julia
|e verfasserin
|4 aut
|
773 |
0 |
8 |
|i Enthalten in
|t Journal of synchrotron radiation
|d 1994
|g 31(2024), Pt 5 vom: 01. Sept., Seite 1217-1223
|w (DE-627)NLM09824129X
|x 1600-5775
|7 nnns
|
773 |
1 |
8 |
|g volume:31
|g year:2024
|g number:Pt 5
|g day:01
|g month:09
|g pages:1217-1223
|
856 |
4 |
0 |
|u http://dx.doi.org/10.1107/S160057752400643X
|3 Volltext
|
912 |
|
|
|a GBV_USEFLAG_A
|
912 |
|
|
|a SYSFLAG_A
|
912 |
|
|
|a GBV_NLM
|
912 |
|
|
|a GBV_ILN_40
|
912 |
|
|
|a GBV_ILN_350
|
912 |
|
|
|a GBV_ILN_2005
|
951 |
|
|
|a AR
|
952 |
|
|
|d 31
|j 2024
|e Pt 5
|b 01
|c 09
|h 1217-1223
|