3D Detector Activities: Difference between revisions
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== 3D | = Introduction to 3D detectors = | ||
3D detectors have three dimensional electrods going through the silicon substrate. The depletion thickness depends on p+ and n+ electrode distance. The advantages with 3D technology is: | |||
* It can operate at very low voltages | |||
* One can achieve very high radiation hardness | |||
* Very fast | |||
* Active almost to the edge | |||
Schematic drawings of the 3D detector: | |||
More information | |||
* Testbeam talk by Erlend and Ole | |||
* 3D workshop in Barcelona | |||
* 3D-state of the art | |||
* 3D proposal by S.I. Parker C.J. Kenneyand and J. Segal (NIMA395(1997)328) | |||
Our Activities | |||
* TestBeam Analysis | |||
* 3DSensor Characteristics | |||
* 3DMeasurement System | |||
Who are we? | |||
* In Bergen: Bjarne, Heidi, Kristine, Ahmed ... | |||
Revision as of 13:32, 18 February 2009
Introduction to 3D detectors
3D detectors have three dimensional electrods going through the silicon substrate. The depletion thickness depends on p+ and n+ electrode distance. The advantages with 3D technology is:
* It can operate at very low voltages * One can achieve very high radiation hardness * Very fast * Active almost to the edge
Schematic drawings of the 3D detector:
More information
* Testbeam talk by Erlend and Ole * 3D workshop in Barcelona * 3D-state of the art * 3D proposal by S.I. Parker C.J. Kenneyand and J. Segal (NIMA395(1997)328)
Our Activities
* TestBeam Analysis * 3DSensor Characteristics * 3DMeasurement System
Who are we?
* In Bergen: Bjarne, Heidi, Kristine, Ahmed ...