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One of the activities of the spatial team of the CNRS/CRTBT Samuel Leclercq, CNRS/CRTBT (Grenoble, France) European Network on Applied Cryodetectors Munich, Germany, 7th November 2003
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Projects Bolometric Camera for Millimetre wavelengths Diabolo Archeops Planck Edelweiss II Team Alain Benoit Philippe Camus François-Xavier Désert Samuel Leclercq One of the activities of the spatial team of the CNRS/CRTBT
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Goals for the bolometric camera 64x64 pixels @ =1.2 mm (250 GHz), 1.5x1.5 mm 2 /pixel (FWHM 8.5") 32x32 pixels @ =2.1 mm (143 GHz), 2.6x2.6 mm 2 /pixel (FWHM 15") Shannon sampling of the unvignetted 260" field of view at the IRAM 30m telescope. 1 hour for the detection of a 3mJy source (F galaxy ≈ 10 12 L ) (10 hours with best actual instruments) Reach optimum abilities of the IRAM 30 m telescope : angular resolution and photon noise. SZ effect and high z galaxy mapping. For one pixel with 1 mm water vapour in atmosphere, and instrument NEP = 50% of total photon NEP : 1 Jy = 10 -26 W/m 2 /Hz
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Exemple of electro- thermal tests. 80mK 150mK 200mK 300mK NbSi single bolometer Bolometer on thin Si 3 N 4 membrane L=300 m S=60 m 2 NbSi : Anderson insulator, variable range hopping. Goal : reach the metal-insulator transition at the dilution temperature (100 mK). Efros and Shklovskii law : NbSi Au/Cr Au/Cr (thermal link) Bi (absorber) NEP : 5.10 -17 W/ Optimisation : A ≈ 10 and R fit to the electronic read out. Controlled by the shape of the NbSi thin layer + Nb composition
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#1 à #8 #10 #13 #11 Lithography : <0 resist and 365nm UV exposure Au ≈ 1500 Å Ti ≈ 50 ÅNb ≈ 500 Å Ir ≈ 50 Å NbSi ≈ 1000 Å SiO ≈ 250 Å Only wafers #11 and #13 have Nb electrodes deposited with mechanical mask. 4 kinds of arrays tested Resist / Lithography Shadow mask NbSi arrays Smooth edges no contact problems No resist no pollution problems
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Fits : R 0 = 1,1 k 16 < T 0 (K) < 18,8 R(V) = V/I still too high at low V. Films not as homogenous as expected. Yet, shapes fits with electron-phonon decoupling : g e–ph = 100 W/K 5 /cm 3. Better results on #13 (data processing in progress). NbSi arrays Tests on wafer #11
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Electronic multiplexing Necessity for a cold multiplexing system with low current and low noise electronic Without multiplexing system Matrix NxN N 2 +2 wires between dilution and 300K too much. Ex matrix 32x32 1026 wires. input polarisation NxN output signals bolometer matrix only R load R bolo Matrix NxN 2N+2 wires. Advantages : volume occupied and conductive heat loads by wires, dissipation from cold JFET amplifiers. Ex matrix 32x32 66 wires. With multiplexing system Commutation transistor : HEMTs Capacity filtering transient effects : C 1 nF bolometer and transistors matrixes N commutation lines N output signals
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Electronic time multiplexing for high Z LTD FREQUENCY REQUIREMENTS Bolometer Signal bandwidthB = 10 Hz Bolometer Sampling frequencyF sampling > 2 B ELECTRICAL NOISE ANALYSIS Bolo Johnson noise e N,bolo = (W/ ) Read time/pixel t mes = 1/F samping Amplifier HF noise e N,ampl (W/ ) Sample RMS noise TYPICAL DESIGN Rb = 10M ; C INT = 1.6 nF ; T=100mK ; e N,bolo =7.4 nV/ CAPACITIVE POLARISATION No power dissipation at low temperature Cold capacity (C POL ~ 5pF) to avoid any leakage current Minimisation of transient effects when commutation occurs
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In progress : conception and test of a complete bolometer matrix with bow tie absorber antennas 1) nitruration 2) RIE (SF 6 ) 3) KOH thermal membrane 4) Nb electrodes with shadow mask 5) NbSi thermometer with shadow mask 6) Au track lithography 7) SiO 2 isolation 8) Nb antennas lithography 9) Bi shunt lithography 10) KOH opening membranes
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In progress : conception and test of a complete bolometer matrix with bow tie absorber antennas Test of antennas absorption on a Fourier Transform Interferometer (Martin Pupplet)
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Very low capacity Cgs~1fF R ON 10 7 Array of 13 HEMTs with common source in PLCC-28 supports Ig<0.1pA Small voltage variation for switching Conduction noise = Johnson [PRL] In progress : development of Quantum Point Contacts HEMTs too improve the multiplexing system
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Coming next NbSi : - Electric tests on a bolometer matrix with field effect and electron-phonon decoupling fittings. - Fourier Transform on V(I) curves Phonon, Johnson, 1/F and "pop corn" noises. Antennas : - Numerical analysis of electromagnetic absorption by antennas with a fourth wave cavity (in progress). - Conception of a Martin Pupplet interferometer. - Studies on different shapes and tests with the Martin Pupplet. Bolometers : - Finishing the electronic and instrument control program. - Heat transfers in membranes. - Photon noise recording and calibration with a black body (in progress) Around the matrix : - radiation filters - dilution fridge for the camera - lenses and mirrors for adaptation on the IRAM 30 m telescope Optical axe of the telescope (F/D=10) Field mirror Focal plane of the field mirror on the cold lens Image of the sky < 1 m
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