Download presentation
Presentation is loading. Please wait.
Published byEloise Addison Modified over 9 years ago
1
Diamond Sensors Laboratory 3D micro-structuring of diamond for radiation detector applications B.Caylar, M.Pomorski, P.Bergonzo Diamond Sensors Laboratory CEA-LIST, Gif-Sur-Yvette, France José Alvarez Laboratoire de génie électrique de Paris (LGEP), Gif-sur-Yvette, France Alexander Oh University of Manchester, School of Physics and Astronomy, Manchester, United Kingdom Thorsten Wengler CERN, Geneva, Switzerland
2
Diamond Sensors Laboratory Advantages 1 : Higher electric field for a given applied bias voltage Shorter drift path thus drift time Lower probability of trapping 2 Context – Why using 3D electrodes? [1] J.Morse, C.J. Kenney, E.M. Westbrook et al. / Nuclear Instruments and Methods in Physics Research Section A, 524 (2004) 236. 2D Electrodes 3D Electrodes Ionizing particle
3
Diamond Sensors Laboratory 3 Context – Why using 3D electrodes? Planar 3D Analytically calculated currents generated by a MIP
4
Diamond Sensors Laboratory 4 NIEL induces bulk defects When flux increases : Defects number increases Carrier lifetime reduction CCE decreases [2] Michal Pomorski – PhD debate, Frankfurt University 07/08/2008 before irradiation after 1.2 x 10 14 20MeV n.cm -2 after 1.97 x 10 14 20MeV n.cm -2 Signal decrease Context – Why using 3D electrodes?
5
Diamond Sensors Laboratory 5 3D geometry is faster : 8ns vs 208ps. 3D geometry makes the detector more radiation hard Context – Why using 3D electrodes? Planar 3D
6
Diamond Sensors Laboratory Burried electrodes Laser setup & Fabrication Structural characterization Electrical characterization pc-CVD Detector (e6 detector grade) Electrical characterization Characterization under alpha particles sc-CVD Detector (e6 electronic grade) Optical characterization Electrical characterization Transient current measurements Conclusion 6 Outline
7
Diamond Sensors Laboratory BURRIED ELECTRODES LASER SETUP & FRABRICATION 7
8
Diamond Sensors Laboratory 8 Burried electrodes – Laser setup Tunable parameters Scan velocity 1-1000 µm/s Laser power 0-160µJ/pulse Repetition rate 1-30 Hz Sample holder Nitrogen laser λ = 337nm τ = 3ns XYZ Motorized stage Webcam 20x Lens
9
Diamond Sensors Laboratory 9 Burried electrodes – Fabrication XYZ Motorized stage Photoluminescence during laser processing Translation Graphitization
10
Diamond Sensors Laboratory 10 BURRIED ELECTRODES STRUCTURAL CHARACTERIZATION
11
Diamond Sensors Laboratory 11 Clean surface (Where graphitization starts) Cracked Surface (Where graphitization ends) Tilted sample 150 µm Optical grade sc-CVD sample Structural characterization – Optical microscopy 10µm diameter 20-100 µm diameter 700µm depth
12
Diamond Sensors Laboratory 12 Structural characterization – 2D Raman mapping 2D Raman depth mapping obtained by integrating diamond peak No micro-channel Micro-channel with cracks 1000 CCD cts 0 CCD cts 1000 CCD cts 0 CCD cts 10µm Depth
13
Diamond Sensors Laboratory 13 Structural characterization – SEM imaging Channel’s clean side after laser processing Channel’s clean side after H 2 plasma H 2 Plasma
14
Diamond Sensors Laboratory 14 BURRIED ELECTRODES ELECTRICAL CHARACTERIZATION
15
Diamond Sensors Laboratory 15 Electrical characterization – I(V) measurements Graphite’s channel resitivity [3] T.Ohana, T.Nakamura, A.Goto et al. / Diamond and Related Materials, 12 (2003) 2011 ρ (average) = 5.7x10 -1 Ω.cm R (500µm) ~ 2kΩ Match with nanocrystalline graphite given in literature 3 A
16
Diamond Sensors Laboratory 16 PC-CVD DETECTOR ELECTRICAL CHARACTERIZATION E6 detector grade 10 x 10 x 0.7 mm 3 Sample courtesy Alexander Oh
17
Diamond Sensors Laboratory 17 Electrical characterization – Device leakage current A Comparison between planar and 3D geometry Planar 3D
18
Diamond Sensors Laboratory 18 PC-CVD DETECTOR CHARACTERIZATION UNDER ALPHA PARTICLES
19
Diamond Sensors Laboratory 19 α Al front contact Al back contact Am-241 Source 5.486MeV R V bias = ±500V Characterization under alpha particles – Experimental setup FCSA Fast Charge Sensitive Amplifier M.Ciobanu, GSI, Germany Signal Scope Collimator
20
Diamond Sensors Laboratory 20 Characterization under alpha particles - Results Polarization study – Holes drift (pc-CVD sample) Planar 3D
21
Diamond Sensors Laboratory 21 Characterization under alpha particles - Results Polarization study – Electrons drift (pc-CVD sample) Planar 3D
22
Diamond Sensors Laboratory 22 Characterization under alpha particles - Results Holes drift (pc-CVD sample) α α Amplitude has been normalized with the signal of a sc-CVD « e6 electronic grade » diamond
23
Diamond Sensors Laboratory 23 Characterization under alpha particles - Results Electrons drift (pc-CVD sample) α α Amplitude has been normalized with the signal of a sc-CVD « e6 electronic grade » diamond
24
Diamond Sensors Laboratory 24 Characterization under alpha particles - Analysis α α Low CCE High CCE Electric field simulation 3D Geometry but pseudo–3D detector 700µm 200µm HV +500V V/µm 5 4.5 4 3.5 3 2.5 2 1.5 1 0.5 0
25
Diamond Sensors Laboratory 25 SC-CVD DETECTOR E6 electronic grade - oriented 3 x 3 x 0.3 mm 3 Sample courtesy Eleni Berdermann
26
Diamond Sensors Laboratory 26 SC-CVD DETECTOR OPTICAL CHARACTERIZATION
27
Diamond Sensors Laboratory 27 Bulk strain mapping after graphitization Micro structured sc-CVD diamond observed with crossed polarizers Test areas Detector area Detector’s optical characterization – Optical microscopy
28
Diamond Sensors Laboratory 28 Detector’s optical characterization – Optical microscopy Detector after metallization
29
Diamond Sensors Laboratory 29 SC-CVD DETECTOR ELECTRICAL CHARACTERIZATION
30
Diamond Sensors Laboratory 30 Electrical characterization – Device leakage current sc-CVD sample after plasma O2 etching HV on cracked surface HV on clean surface
31
Diamond Sensors Laboratory 31 SC-CVD DETECTOR TRANSIENT CURRENT MEASUREMENTS
32
Diamond Sensors Laboratory 32 2D Zone HV +100V Electrical characterization – Setup and methods 2D Zone Signal Scope Ampli Transient current measurements 300µm Ultra-Fast 40 dB, 2 GHz Broadband Amplifier
33
Diamond Sensors Laboratory Signal 3D ~500mV Electrons drift Mixed e/h drift Signal 2D ~100mV Signal 2D ~80mV Holes drift 33 Transient current measurements - Results Without collimator Alphas’ injection on cracked side Alphas’ injection on clean side 1 ns
34
Diamond Sensors Laboratory 34 Transient current measurements - Results With collimator 1 ns Mixed e/h drift Alphas’ injection on cracked side
35
Diamond Sensors Laboratory V/µm 35 Transient current measurements - Analysis Electric field simulation 3 2.5 2 1.5 1 0.5 0 300µm +100 V α α Planar+3D signal Planar signal only
36
Diamond Sensors Laboratory 36 Transient current measurements - Results Experimental results Selection of relevant events Amplitude ratio = 6
37
Diamond Sensors Laboratory Amplitude ratio = 23.8 2GHz low pass filter 37 Transient current measurements - Results Analytically calculated signals Theoritical response Amplitude ratio = 22
38
Diamond Sensors Laboratory Amplitude’s ratio = 6.2 38 Transient current measurements - Results Analytically calculated signals 350 MHz low pass filter Ampli + device bandwith ~350MHz R device ~ 520 Ω 12 channels connected R channel ~ 6 kΩ
39
Diamond Sensors Laboratory 39 Conclusion Conductive graphitic structures has been achieved on both pc- and sc-CVD sample These structures are suitable for detectors applications Two dectetors using 3D-geometry electrodes has been produced A real improvement between planar and 3D geometry has ben observed Higher signal Faster response « Polarization effect » decrease on pc-CVD detector But real 3D detector hasn’t been achieved yet…
40
Diamond Sensors Laboratory 40 Thanks for your attention !
Similar presentations
© 2024 SlidePlayer.com Inc.
All rights reserved.