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Royal Holloway University of London
Towards passive terahertz imaging using a semiconductor quantum dot sensor Vladimir Antonov Royal Holloway University of London
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Acknowledgments Royal Holloway, UK : H Hashiba
Tokyo University&JST, Japan: Prof. S Komiyama, Drs. J Chen, O Astafiev (NEC) ISSP RAN, Russia: Dr. L Kulik NPL, UK: Dr A Tzalenchuk, Dr S Gibling and P Kleinschmidt Chalmers University, Sweden: Prof. P Delsing, Dr S Kubatkin Optisense LTD: M Andreo
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Passive Imaging with superconducting bolometer by VTT-NIST
Nb superconducting bolometer Detection of hidden weapon Courtesy of VTT-NIST
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Some numbers for consideration
Noise Equivalent Temperature Difference (NETD) imposed by the temperature contrast, or variation of spectral intensity (spectral fingertips) < 0.1K Background limited noise BLIP~ T(F/n)1/2 , where F - frame rate (10Hz), n - number of detected photons (108), ~0.05K Detector should have NETD better than 0.1K and counting rate around 108 photons/sec
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Some numbers for consideration
Plank’s law There is a difference in ~1010 photons/sec (~10-23J) for black body radiation at 300K and 305K in bandwidth from 0.5 to 0.7 THz. Passive imaging U, J /(Hz m3) f , THz T=305K U, J /(Hz m3) T=300K f , THz
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Finger prints of explosives
Complex materials has a unique fingerprints in spectrum T=300K JF Federici et all ’05
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QD as a spectral sensitive detector
Layout of the QD in 2DEG SEM images of the QD Resonance curve APL ’02 B (Tesla) 1 2 3 4 5 20 40 60 Frequency (/cm) c 0 QD in magnetic field Zero filed Plasma resonance in QD
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Log-periodic circular antenna (0.2-3Thz)
QD-SET detector Log-periodic circular antenna (0.2-3Thz) coupled with QD sensor Energy diagram Dark switches and photo-response original peaks shifted DVg SET response to QD excitation
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Modeling of QD-SET SET SG1 CG Offset charge at SET SG2 QD QSET -Vc
NSET NSET+1 -Vc
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Formation of QD Individual SET trace 2D map of SET current
Charging of the QD
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Photosignal at 0.3K T=0.3K T=0.05K
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Photo response and dark counts
Noise Equivalent Power~ Watt/Hz1/2 NETD = NEP/(2hkBDnt1/2) ~0.01K Quantum Efficiency ~1% Spectral bandwidth ~ 1% Operation temperature is limited by SET (up to 4K) APL, JAP, PRB, IEEE ’04-07
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Photosignal at K
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2D maps of QD-SET VS, V VS, V VC, V VC, V Emitter is OFF Emitter is ON
Physica E ’06 PRB’06
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Detector of different designs
A lateral sensor with QD crossing the channel A lateral sensor with QD outside channel A lateral sensor with QD inside channel A vertical sensor
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QD outside of 2DEG channel
Gate QD-SET
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QD inside the 2DEG channel
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QD in high magnetic field
LL0 LL1 SEM picture of the QD 1m NATURE, 2000
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QD in high B QD under illumination Time traces of QD conductance
Spectral sensitivity of the detector
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QD in high B LL1 I II QD has three levels: LL0,LL0¯,
Lifetime of excitations PRB, 2002
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LT THZ microscope of Tokyo University
Ikushima, Komiyama APL, 2006
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LT THZ microscope of Tokyo University
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Future plans: Quantum Dot in DQW heterostructure
Schematic view Inter-well excitation in asymmetric DQW ~1 THz
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Near-field antennae Simulation of near-field antennae
Simulation of E-field
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Near-field antenna
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Challenges Room Temperature Imaging
QD detector: which type? Room Temperature Imaging Source of THz radiation for in-situ calibration Physics of isolated QD in DW heterostructures
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Vertical sensor in DQW heterostructure
An et all, PRB’07
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