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TES Bolometer Array. For the APEX-SZ Camera. Jared Mehl University of California, Berkeley LTD 12, Paris, 2007. Collaborators. U. C. Berkeley Bill Holzapfel Zigmund Kermish Adrian Lee Martin Lueker Jared Mehl Tom Plagge Paul Richards Dan Schwan Martin White. McGill University - PowerPoint PPT Presentation
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TES Bolometer ArrayFor the APEX-SZ Camera
Jared MehlUniversity of California, Berkeley
LTD 12, Paris, 2007
CollaboratorsU. C. BerkeleyBill HolzapfelZigmund KermishAdrian LeeMartin LuekerJared MehlTom PlaggePaul RichardsDan SchwanMartin White
MPIfRRolf GuestenRuediger KneisslErnst KreysaKarl MentenDirk MudersPeter SchilkeAxel Weiss
McGill UniversityMatt DobbsTrevor LantingJames Kennedy
University of ColoradoNils HalversonDan BeckerAmy Bender
LBNLHelmuth Spieler
NISTHsiao-Mei Cho
Cardiff UniversityPeter Ade
University of BonnKaustuv BasuFrank Bertoldi Martin Nord Florian Pacaud
MPEHans Boehringer
APEX-SZ• 12 m antenna, ALMA prototype
• 5100 m Atacama Plateau, Chile
• 320 element TES bolometer array
• Frequency domain SQUID
multiplexer readout
• Pulse-Tube Cooler (PTC)
• Use Sunyaev-Zel’dovich effect to
study galaxy clusters
• Operating and taking data
TES Array
• Horn-coupled
• 55 Pixels Per Wedge
• 6 Wedges Per Array
TES Array
• Horn-coupled
• 55 Pixels Per Wedge
• 6 Wedges Per Array
TES Bolometer
• Al/Ti Bilayer TES
R ~ 1.2 normal
T ~ 450 mKC
• Au Thermal Link
G ~ 200 pW / K
• low-stress Si N substrate, released with XeF etch3 4 2
• Au spiderweb absorber
R ~ 200 / sq
~ 9 msoptical
Bolometer Cavity Design
Invar Backshort
SiliconWafer
Spiderweb Absorber
Airgap
WaveguideFeed Horn
TES
Band-defining filters
Bolometer Cavity Simulation150 GHz Simulation, 200 Ohm/sq Abs, λ/4 Backshort
Absorbed Power
Reflected Power
Radiated Power
• Optimize bolometer cavity• HFSS - Ansoft Corporation - 3D finite-element electromagnetic sims
Frequency Domain Multiplexer
AC bias bolometers from 200 kHz – 1 MHz
Frequency Domain Multiplexer
• Zero power dissipation
at sub-Kelvin stage
• Strong rejection of time- varying B-fields
• Simple shielding requirements
• Reduced vibration sensitivity
AC bias bolometers from 200 kHz – 1 MHz
Frequency Domain Multiplexer
SQUID arraymade by NIST
= / (Loopgain + 1) > 300 μs
Bolometer Stability
bias
sensor[ Irwin, JAP,1998 ]
5.8Conservative Stability Criterion:
bias = 2L
R~ 50 μs
For current fMUX (AC bias) at 50% bolometer superconducting transition:
With conservative stability criterion we can tolerate:
sensor 0
Early bolometers:
= ~ 100 μs C
G
Too fast for stable operation0
MUX
Increasing Heat Capacity
Current Bolometers:
0 ~ 30 ms
• Add 3 μm thick gold ring
• Slow down detectors
• Critical for heat capacity to be strongly coupled to TES
• Allows operation deep into transition
Noise Performance
120 aW / Hz1/2
Cluster MapAbell 2163 ~1 hour integration
Courtesy T. Lanting
South Pole TelescopeSub-millimeter Wavelength Telescope:• 10 meter telescope (1’ FWHM beam at
150 GHz)1st Generation Camera:• 1 sq. deg FOV• ~1000 pixels• Observe in 3+ bands between 95-220
GHz simultaneously with a modular focal plane
Funded by NSF
220 GHz 150 GH
z
150
GH
z150 GH
z
95 G
Hz
95 GHz
The End.