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High-resolution passive video-rate imaging at 350 GHz. Halpern, Mark 2011

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High-Resolution Passive Video-Rate Imaging at 350 GHz∗ Daniel Beckera , Cale Gentryb , Peter Adec , James Bealla , Hsiao-Mei Choa , Simon Dickerd , William Duncana †, Mark Halperne , Gene Hiltona , Kent Irwina , Peter Lowella , Michael Niemacka , Nick Paultera , Carl Reintsemaa , Frank Schimaa , Robert Schwalla , Carole Tuckerc a NIST-Boulder b University c Cardiff d University e University  of Oklahoma University  of Pennsylvania  of British Columbia  ABSTRACT We are developing a 350 GHz cryogenic passive video imaging system for use in standoff security applications. This demonstration system uses 800 photon-noise-limited superconducting transition edge sensor bolometers, read out using a time-division multiplexed readout system. It will image a 1 m × 1 m field of view at a standoff distance of 16 m to a resolution of approximately 1 cm at video frame rates (20 frames per second). High spatial resolution is achieved by the use of an f/2.0 Cassegrain optical system with 1.3 m primary mirror. Preliminary dark and optical testing of prototype detectors indicates that we can achieve a noise equivalent temperature difference (NETD) below 100 mK for the fully sampled 1 m × 1 m image at 20 frames per second. We report on the current status of development of this system.  1. INTRODUCTION Millimeter-wavelength radiation penetrates clothing well and is non-ionizing, making it a good candidate for identifying threats held beneath clothing.1 For detection of threats at close distances in portal security scenarios, active millimeter-wave systems are commercially available and have been deployed at airports and other sites around the world. For identifying threats at larger “stand-off” distances of more than five meters, passive video imaging systems are available commercially2 but have poor spatial and temperature resolution at frame rates faster than 5 frames per second. To achieve good noise performance at faster frame rates, several groups are developing passive imaging systems using superconducting transition edge sensors. One system with 64 detectors produces video images with a noise equivalent temperature difference (NETD) of 0.5 K at 6 Hz with a resolution of 4 cm over a 2 m × 4 m area.3–6 Another video-imaging system has only 20 detectors but much lower noise on a per-detector basis.7 The millimeter and sub-millimeter astronomy community has spent the past several decades working on a similar problem: high-speed mapping of high-resolution images over a large field of view. One common solution has been the use of large-format arrays of over 1000 superconducting transition edge sensor (TES) bolometers, with multiplexed readout using superconducting quantum interference devices (SQUIDs).8–10 The development of this technology provides the opportunity to greatly increase temperature sensitivity of terrestrial passive imaging systems. We are developing a cryogenic passive video imaging system for operation at distances from 16 m to 28 m.11, 12 The system will contain 800 photon-noise-limited TES bolometers read out by superconducting quantum interference devices (SQUIDs) using a multiplexer developed at NIST. The system will be used as a test-bed to explore trade-offs between NETD, resolution and video frame rate, with the goal of understanding performance requirements for specific real-world stand-off imaging applications. ∗ †  US government contribution; not subject to copyright in the United States. Current Address: Intellectual Ventures, 11235 SE 6th St., Suite A 200, Bellevue, WA 98004  Send correspondence to Daniel Becker: E-mail: beckerd@boulder.nist.gov Passive Millimeter-Wave Imaging Technology XIV, edited by David A. Wikner, Arttu R. Luukanen, Proc. of SPIE Vol. 8022, 802206 · © 2011 SPIE · CCC code: 0277-786X/11/$18 · doi: 10.1117/12.884374  Proc. of SPIE Vol. 8022 802206-1 Downloaded from SPIE Digital Library on 12 Sep 2011 to Terms of Use: http://spiedl.org/terms  Atmospheric & Filter Transmission Transmission (Arbitrary Units)  1 0.8 0.6 0.4 0.2 0 300  Atmospheric Transmission Filter Transmission 320  340 360 Frequency [GHz]  380  400  Figure 1. Plot showing measured transmission of our bandpass filter (solid lines) and typical atmospheric transmission (dashed lines). The passband is centered at approximately 350 GHz (850 µm) and has a full width at half-maximum of about 11 %.  Figure 2. Schematic of optical system. Labels are (A) 1.3 m primary mirror, (B) secondary mirror with dithering mechanism, (C) cryostat window lens, (D) detector focal plane module, including bandpass filter. For clarity, the cryostat is not shown. Inset is a photograph of the primary and secondary mirror assembly.  The system will operate at a frequency of 350 GHz (850 μm) with 11 % fractional bandwidth. Spatial resolution will be 1 cm over a 1 m × 1 m field of view at a distance of 16 m, with a video rate of 20 frames per second. Measurements of prototype detectors and the system’s optical efficiency indicate that the fully populated focal plane with 800 detectors should achieve NETD below 100 mK at 20 frames per second once we have optimized the optical efficiency. This paper describes the optics, detectors, readout, cryogenics and current status of this system.  2. DESIGN OVERVIEW 2.1 Optical Frequency Choice The choice of frequency for a passive imaging system is a tradeoff between the ability to penetrate clothing (favoring low frequencies) and spatial resolution (favoring high frequencies). The 3 dB point for attenuation through clothing ranges from 350 GHz to 1 THz (high frequencies for thin materials such as Nylon, lower for thicker materials such as wool).13 We chose 350 GHz to keep clothing attenuation at or below 3 dB and provide good spatial resolution. This frequency is also the center of an atmospheric transmission band (see Fig. 1).  2.2 Optics Our optical system is an f/2.0 Cassegrain design. The 1.3 m elliptical primary mirror focuses light onto the hyperbolic secondary, which directs the light back through the central hole in the primary; the light then enters an ultra-high-molecular-weight (UHMW) polyethylene lens at the mouth of the cryostat. The lens makes the system telecentric, allowing use of a flat focal plane. The lens/cryostat combination can be moved relative to the primary mirror to focus the system at distances between 16 m and 28 m. The optics were simulated with ray-tracing software and shown to be diffraction-limited across the entire focal plane and at all focusing distances between 16 m and 28 m. See Fig. 2 for an annotated picture of the optical system. A detailed description of the optics has been published elsewhere.11, 12 The observation band is defined by a metal mesh filter14 cooled to 900 mK, defining an optical bandwidth of 40 GHz (11 % FWHM fractional bandwidth); the measured passband of this filter is shown in Fig. 1. Additional filters for thermal blocking are located at the 4 K, 50 K, and 300 K stages.15 Total transmittance of the filter stack plus lens is predicted to be 62 %.  Proc. of SPIE Vol. 8022 802206-2 Downloaded from SPIE Digital Library on 12 Sep 2011 to Terms of Use: http://spiedl.org/terms  Op cal	absorber 1.2	K TES Weak thermal link  Voltage bias  SQUID  900	mK Figure 3. Illustrative plot of resistance vs temperature for a superconductor. The transition is typically very narrow, allowing the use of a superconductor as a sensitive thermometer. A TES detector is voltage-biased into the transition, with the bias point changing based on changes in optical power.  Figure 4. Schematic depiction of the operation of a TES. Optical power is absorbed onto the TES. Increases in absorbed optical power raises the temperature of the TES, raising its resistance. The dissipated V 2 /R Joule power in the TES drops, compensating for the increase in optical power, leaving as constant the total dissipated power flowing out of the TES through the weak thermal link. This negative electro-thermal feedback allows the detector to operate stably. Changes in current passing through the TES are detected by a SQUID.  At the focal plane, light is captured by smooth-walled conical feedhorns that were chosen for their simplicity and ease of manufacture. To optimize coupling of the feedhorns to the rest of the optical system, we use feedhorns with a diameter of 3.2 mm, or approximately 2F λ, where F = 2.0 is the f-number of the optics and λ = 850 μm is the optical wavelength. The taper half-angle is 9.4◦ , tapering to a 3.5 mm length of 0.6 mm diameter circular waveguide that leads to the detectors. The feedhorn design was modeled with finite-element electromagnetic simulations, predicting a spillover efficiency of 54 %. Conductive loss in the 3.5 mm length of 0.6 mm waveguide behind the feedhorn is calculated to be about 10 %. At the back of the 0.6 mm circular waveguide, in front of a quarter-wave backshort, the light is absorbed by a thin-film PdAu mesh patterned on a relieved membrane, as described in section 2.4. Finite-element electromagnetic models predict that the PdAu mesh will absorb 82 % of the optical power coming down the waveguide. The mesh absorbs both polarizations. The feedhorns will cover only a portion of the diffraction-limited area of the focal plane. Additionally, the spacing between the feedhorns is larger than the point-spread-function of the optics, so the image projected on the focal plane at any given instant will not be Nyquist sampled. Therefore, in order to use the entire diffractionlimited extent of the optics, and to generate fully sampled images, the image will be moved across the focal plane in a “dithering” pattern. This is done by moving the secondary mirror with a pair of linear actuators.  2.3 Transition Edge Sensors Optical power is detected by voltage-biased superconducting transition edge sensor (TES) bolometers.16, 17 Below a critical temperature, Tc , a superconductor loses all resistance to DC electrical current (see Fig. 3). The sharp transition from the normal state to superconducting state allows a superconductor that has been biased into its transition to serve as a sensitive thermometer. Any signal that can be turned into a temperature change can then be detected as a change in the resistance of the superconductor. Reference 18 contains a detailed description of the behavior of TES devices. Fig. 4 schematically depicts the operation of a voltage-biased TES bolometer. A superconducting film is thermally sunk to an optical absorber. Increased optical power raises the temperature of the film, increasing the  Proc. of SPIE Vol. 8022 802206-3 Downloaded from SPIE Digital Library on 12 Sep 2011 to Terms of Use: http://spiedl.org/terms  E C  Total Power (TES + heater) [pW]  Saturation Power vs Bath Temp  D  A  B  2000  1500  1000  500  0 800  200 um  Figure 5. A picture of a prototype detector. The relieved area is 800 µm in diameter. The different components are: (A) PdAu absorbing mesh, lines 2 µm wide spaced 85 µm apart, (B) thin-film Al TES, (C) silicon nitride legs connecting relieved membrane to the bulk Si substrate that serves as low-temperature bath, (D) Au ring providing additional heat capacity to slow the thermal response time of the device for optimal readout, (E) PdAu heater resistor used for testing.  4309 Data 4309 Fit 4311 Data 4311 Fit 4307 Data 4307 Fit  900 1000 1100 1200 Bath Temperature [mK]  1300  Figure 6. Plot showing saturation power Psat vs bath temperature for three of our prototype devices. Fitting all three parameters n, K, and Tc implies n ≈ 3.6. The fit constrains n is weakly, so for this paper we assume n = 4.0 everywhere; this increases our predicted detector noise by a few percent. Detector 4307 was measured in a different cryostat with different thermometry, which could explain the temperature offset from detectors 4309 and 4311.  resistance of the TES, which decreases the current passing through the circuit. A SQUID detects the drop in current. The device operates in a negative-feedback loop, with increasing optical power leading to lower V 2 /R Joule heating, allowing the device to operate stably. A weak thermal link connects the absorber and superconducting film to a low-temperature heat bath. The n ), thermal conductance of this link determines the saturation power Psat according to Psat = K(Tcn − Tbath where K and n depend on the geometry of the thermal link and the dominant heat transport mechanism in the temperature regime of interest; for our detectors we expect n ≈ 4.0. The dominant source of intrinsic noise in a TES bolometer is thermal fluctuations of the temperature of the TES itself. This noise is N EPG = F 4kB GTc2 , where kB is Boltzmann’s constant and the differential thermal conductance G is defined as G = dP/dTc = nKTcn−1 . The prefactor F is unity in equilibrium, and in the range 0.5–1.0 under operating conditions. Photon noise is also a significant source of noise in our system. The expression for photon noise, including the effect of photon bunching, is19 N EPopt =  2hνPopt (1 + η¯ n),  (1)  where h is Planck’s constant, ν is the central frequency, Popt is the total optical loading, η is the optical efficiency (excluding feedhorn spillover efficiency, because the feedhorn spillover is terminated at 300 K), and n ¯ = [exp(hν/kB T ) − 1]−1 is the average photon occupation number per mode. For our system observing 300 K radiation, n ¯ = 17.5, so the bunching term is important. Total optical power per √ detector when observing a 300 K target will be 2ηkB T Δν = 165 pW. Use of (1) then gives N EPopt = 0.8 fW/ Hz.  2.4 Design of Prototype Detectors Fig. 5 shows a picture of a prototype detector. The device is fabricated on a relieved silicon-nitride membrane approximately 800 μm in diameter. A PdAu mesh absorbs the light, with mesh dimensions (2 μm wide lines spaced 85 μm apart) chosen to match the wave impedance of the waveguide. The Al TES is at the lower edge of  Proc. of SPIE Vol. 8022 802206-4 Downloaded from SPIE Digital Library on 12 Sep 2011 to Terms of Use: http://spiedl.org/terms  the membrane and has dimensions 64 μm × 64 μm. A 15 μm × 16 μm PdAu heater resistor sits near the center of the relieved membrane for use in testing. We designed our detectors to have Psat = 1 nW at a bath temperature of 900 mK, for a safety factor of 6 times the predicted optical loading of 165 pW. Given this saturation power, an Al TES with Tc = 1.2 K, a bath at 900 mK, and a target G of 4.5 nW/K should meet our NETD requirements. The dimensions of the eight silicon-nitride legs (11 μm wide × 40 μm long, 0.5 μm thick) were chosen to achieve this G. This large thermal conductance requires a large heat capacity C to keep the thermal time constant near the 1 ms that is optimal for our readout system. We have achieved this by adding a 2 μm thick gold ring around the outer diameter of the relieved membrane.  2.5 Readout The array is read out by the SQUID-based time-division multiplexing (TDM) system developed at NIST.20 At room temperature a single Multi-Channel Electronics (MCE) crate will read out all 800 detectors.21 The combination of NIST SQUID TDM with the MCE is used daily to collect data at three different millimeter-wave telescopes.8, 10, 22 All hardware for the full 800 detector array, including cryogenic wiring, is already installed in our cryostat.  2.6 Cryogenics To cool our focal plane to an operating bath temperature of 900 mK, we use a two-stage refrigeration system. The first stage is a commercially available cryogen-free cooler that reaches 3 K. The second stage is a custom-built 4 He sorption fridge that cools to below 1 K, and is based on a design that has been proven in the field.23 The system reaches a base temperature of approximately 900 mK with a hold time of 13.5 hours when open optically. Operation of the cryogenics will be fully automated.  3. CURRENT STATUS We have installed four prototype detectors into our cryostat. Individual modules with feedhorns integrated into their cover hold each detector. All data discussed in this section were taken with the complete multiplexed readout chain configured in a 2 row × 2 column format.  3.1 Dark Testing The prototype devices have a transition temperature of approximately 1.23 K, with a normal-state resistance of about 3.5 mΩ. Fig. 6 shows measured saturation power vs. bath temperature for three √ tested devices; √ the measured G values are 5.0 nW/K to 5.4 nW/K. These values of G imply N EPG of 0.64 fW/ Hz to 0.69 fW/ Hz, assuming a prefactor F of 1.0. The measured NEP under no optical load for a prototype detector is shown in Fig. 7. The measured noise level matches the prediction well. √ Adding the measured detector noise and predicted photon noise in quadrature gives N EPtot = 1.1 fW/ Hz. This total NEP can be converted to an NETD through the use of the radiometer equation,24 N ET D =  N EPtot √ , 2kB Δνη 2τ  (2)  where τ is the total integration time per pixel in the processed video frame, Δν = 40 GHz is the pre-detection optical bandwidth, and η = 0.25 is the total optical efficiency (0.82 absorber efficiency, 0.62 filter stack efficiency, 0.54 feedhorn spillover efficiency and 0.90 feedhorn insertion loss). Creating a 1 m2 image with 1 cm resolution requires 2002 pixels per video frame. With an 800 detector system, this leads to a “dithering factor” of 2002/800 = 50, meaning that each detector will image 50 image pixels per video frame, and τ = 1/(50)(20 Hz). Equation 2 thus predicts that our system will have N ET D = 85 mK across the full field of view at 20 FPS.  Proc. of SPIE Vol. 8022 802206-5 Downloaded from SPIE Digital Library on 12 Sep 2011 to Terms of Use: http://spiedl.org/terms  Detector NEP (40% Rn)  −14  NEP (W/rt−Hz)  10  Measured Predicted TFN Noise  −15  10  −16  10  0  10  1  10  Frequency (GHz)  2  10  Figure 7. Plot showing measured noise equivalent power (NEP) spectral density for a prototype detector, under no optical √ load. The white noise level is about 0.65 fW/ Hz. The low-frequency increase in noise is due to a drift in bath temperature that we are fixing. The 120 Hz rolloff is due to a filter in the readout electronics that was turned on while acquiring this spectrum.  3.2 Optical Testing Our optical testing has focused on two areas: measuring optical efficiency and taking still images. To measure total optical efficiency we measure the difference in detected optical power between when the imager is observing 295 K and 77 K blackbodies. If this difference in detected optical power is ΔP295/77 , then the total optical efficiency of the system is defined as ΔP295/77 / (2kB ΔT Δν). The 295 K blackbody is a sheet of room-temperature Eccosorb AN-72 attached to an aluminum backing sheet. The 77 K blackbody is a sheet of Eccosorb AN-72 submerged in liquid nitrogen held in a styrofoam cooler with walls approximately 2.5 cm thick. We apply a correction to account for the imperfect transmission of the styrofoam cooler’s walls, which we measured by moving the cooler’s lid back and forth in front of the cooler. This measurement approach resulted in an average optical efficiency of 11.5 % for the four detectors, about half of the predicted value of 26 %. We have not yet identified the source of the lost efficiency, but it is likely that some of the loss is due to poor alignment of the cryostat with the primary and secondary mirrors. We do not yet have enough detectors installed to take video images. But we can take still images by using the secondary mirror to raster scan over the target. Fig. 8 shows an image of a person with a ceramic knife concealed beneath his shirt. This image includes data from three detectors, with a large area of overlap near the image center. The knife is visible on the left side. Also visible is the outline of a pocket, the shirt collar, and the strip of extra cloth backing the shirt’s buttons. To produce this image, we combined data simultaneously acquired by three detectors. First, data from each detector were used to create three sub-images. Second, an edge taper was applied to each sub-image, and all three sub-images were combined. Third, the full image was Weiner deconvolved by use of the measured pointspread-function of the system, which has the effect of both (a) reducing noise on spatial scales smaller than the system’s resolution, and (b) improving apparent resolution. The temperature scale was calibrated by use of the heaters and the measured optical efficiency. The expected contrast in the image is 12 K (skin temperature of 310 K with emissivity of 0.80, lab background temperature of 295 K). The total contrast in the image is 14 K, indicating that the calibration is reasonable. We estimate the image NETD by taking the standard deviation of pixel temperature values in a flat area of each sub-image. This yields an NETD of 85 mK, which is about what we expect, given the integration time per sub-image pixel of 5.5 ms and the measured optical efficiency. The integration time per pixel for video images will be 1 ms, so  Proc. of SPIE Vol. 8022 802206-6 Downloaded from SPIE Digital Library on 12 Sep 2011 to Terms of Use: http://spiedl.org/terms  Figure 8. Two representations of a still image taken with our system. The image was taken by raster scanning across a person with a ceramic knife concealed beneath his shirt. The knife is visible on the left side of each image. Also visible is the outline of a pocket, the shirt collar, and the strip of extra cloth backing the shirt’s buttons. The total time to acquire the image was 50 s, with an average of 5.5 ms integration time per image pixel. Left False-color temperature mapping. The video-rate NETD implied by this image is 200 mK, which can be reduced to below 100 mK through optimization of the optical system. The total contrast in the image is 14 K, and the contrast between the knife and the warm part of the body next to it is 3.9 K. Right “Topographic” mapping of the same image data. The data is plotted as a 3-D image, lit from directly above by a light source, and viewed from directly above. This 3-D representation is routinely used with range data in active radar imaging systems.25  √ the implied NETD for video rate images is 85 mK × 5.5 = 200 mK. This is approximately two times higher than predicted in section 3.1, which is expected because of our poor measured optical efficiency. Optimization of the optics should allows us to reach the predicted 85 mK NETD.  4. NEXT-GENERATION SYSTEM The current system features high sensitivity and low noise to facilitate the investigation of the tradeoffs inherent in an operational system. Adapting this system for field deployment will require reduction in cost, weight, and complexity. In addition to modifications such as molded composite optical elements and simplified cryogenics, we are planning to read out a next-generation system with gigahertz micro-resonators that can read out focal planes of either TESs or Microwave Kinetic Inductance Devices (MKIDs).26 This technology can read out hundreds of detectors with a single coaxial cable, greatly reducing the cost and complexity of cryogenic wiring, and allowing focal planes with larger numbers of detectors.  Proc. of SPIE Vol. 8022 802206-7 Downloaded from SPIE Digital Library on 12 Sep 2011 to Terms of Use: http://spiedl.org/terms  5. CONCLUSION We have designed a 350 GHz cryogenic terrestrial passive video imaging system by leveraging technology proven in the millimeter and sub-millimeter astronomy fields. The video imager will use 800 TES bolometers to image a 1 m × 1 m field to a resolution of 1 cm at a distance of 16 m at video frame rates. Measurements of our prototype detectors indicate that they are close to being photon-noise-limited. Initial optical testing indicates that the fully populated system will take video-rate images with 200 mK NETD. Improving NETD to the predicted 85 mK requires optimizing our optical efficiency, but requires no changes to the detector design. Our next steps are to design, fabricate, and install the full 800-detector focal plane.  REFERENCES [1] R. Appleby, “Passive millimetre–wave imaging and how it differs from terahertz imaging,” Philosophical Transactions A 362(1815), p. 379, 2004. [2] C. Mann, “First demonstration of a vehicle mounted 250GHz real time passive imager,” in Proceedings of SPIE, 7311, p. 73110Q, 2009. [3] A. Luukanen and J. Pekola, “A superconducting antenna-coupled hot-spot microbolometer,” Applied Physics Letters 82, p. 3970, 2003. [4] E. Grossman, C. Dietlein, J. Bjarnason, A. Luukanen, M. Leivo, and J. 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