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Showing papers by "Edward J. Wollack published in 2005"


Proceedings ArticleDOI
04 Feb 2005
TL;DR: In this article, the authors proposed an analytical design for a microstrip broadband spurious-suppression filter, which uses each section of the transmission line as both a coupling and a spurious suppression element.
Abstract: We propose an analytical design for a microstrip broadband spurious-suppression filter. The proposed design uses each section of the transmission line as both a coupling and a spurious suppression element. Every two sections of the transmission line are combined to create a quarter-wavelength stepped impedance resonator (/spl lambda//4 SIR). The optimal resonator length is proven to be the shortest, while delivering the broadest spurious-free bandwidth. The experimental result shows that the size of the 4th order bandpass filter with a stepped impedance ratio (R) of 0.2 is 0.33/spl lambda/, long and 0.18/spl lambda/ wide, which is less than half of the size of the filter designed using the in-line coupling approach. The out-of-band attenuation of the developed filter is greater than 50 dB; and the first spurious mode is shifted to approximately 5.4 times the fundamental frequency.

17 citations


Journal ArticleDOI
TL;DR: In this article, the authors report on the design of corrugated feed horn microwave antennas at 3.3, 5.6, 7.8, and 10.2 GHz for cosmology, astrophysics, and diffuse emission experiment.
Abstract: We report on the design of corrugated feed horn microwave antennas at 3.3, 5.6, 7.8, and 10.2 GHz for the absolute radiometer for cosmology, astrophysics, and diffuse emission experiment. These horns have low sidelobe symmetrical beams with 12° full width at half power, and three noteworthy features: a 30° slice at the aperture, a profiled rather than a linear taper, and a slowly varying groove depth along the length of the horn. The profiled taper and varying groove depth provided a narrow beam given the existing physical spatial constraints of the instrument in which the horns are used. The 30° slice was necessary for instrumental considerations and has a minimal effect on the symmetry of the beam. The slice reduces the effective aperture radius and overall length to that corresponding to an unsliced horn with an aperture at roughly the middle of the slice and does not introduce any undesirable effects.

9 citations


01 Dec 2005
Abstract: We are building a bolometer camera (the Goddard-Iram Superconducting 2-Millimeter Observer, GISMO) for operation in the 2 mm atmospheric window to be used at the IRAM 30 m telescope. The instrument uses a 8x16 planar array of multiplexed TES bolometers which incorporates our newly designed Backshort Under Grid (BUG) architecture. Due to the size and sensitivity of the detector array (the NEP of the detectors is 4×10-17 W/√Hz), this instrument will be unique in that it will be capable of providing significantly greater imaging sensitivity and mapping speed at this wavelength than has previously been possible. The major scientific driver for this instrument is to provide the IRAM 30 m telescope with the capability to rapidly observe galactic and extragalactic dust emission, in particular from high-z ULIRGs and quasars, even in the summer season. The 2 mm spectral range provides a unique window to observe the earliest active dusty galaxies in the universe and is well suited to better confine the star formation rate in these objects. The instrument will fill in the SEDs of high redshift galaxies at the Rayleigh-Jeans part of the dust emission spectrum, even at the highest redshifts. The observational efficiency of a 2 mm camera with respect to bolometer cameras operating at shorter wavelengths increases for objects at redshifts beyond z ~ 1 and is most efficient at the highest redshifts, at the time when the first stars were re-ionizing the universe. Our models predict that at this wavelength one out of four serendipitously detected galaxies will be at a redshift of z > 6.5.

3 citations


Patent
23 May 2005
TL;DR: A charge-dissipative electrical interconnect comprises at least one first conductive element, a first lossy dielectric layer surrounding the first conductivity element and a first shielding element.
Abstract: A charge-dissipative electrical interconnect comprises at least one first conductive element, a first lossy dielectric layer surrounding the at least one first conductive element, a first shielding element surrounding the first lossy dielectric layer, at least one grounding conductive element electrically contacting the first shielding element, and a second lossy dielectric layer surrounding the first shielding element.

2 citations


01 Jan 2005
TL;DR: In this paper, the authors present a mathematical description of a quasioptical vector interference (QVI) which maps an input polarization state to an output polarization state by introducing a phase delay between two linear orthogonal components of the input polarization.
Abstract: We present a mathematical description of a Quasioptical Vector Interferometer (QVI), a device that maps an input polarization state to an output polarization state by introducing a phase delay between two linear orthogonal components of the input polarization. The advantages of such a device over a spinning wave-plate modulator for measuring astronomical polarization in the far-infrared through millimeter are: 1. The use of small, linear motions eliminates the need for cryogenic rotational bearings, 2. The phase flexibility allows measurement of Stokes V as well as Q and U, and 3. The QVI allows for both multi-wavelength and broadband modulation. We suggest two implementations of this device as an astronomical polarization modulator. The first involves two such modulators placed in series. By adjusting the two phase delays, it is possible to use such a modulator to measure Stokes Q, U, and V for passbands that are not too large. Conversely, a single QVI may be used to measure Q and V independent of frequency. In this implementation, Stokes U must be measured by rotating the instrument. We conclude this paper by presenting initial laboratory results.

1 citations


01 Jan 2005
TL;DR: In this article, the authors measured electrical and optical properties of implanted silicon resistor layers designed to be suitable for these absorbers, demonstrating frequency regimes in which different recipes will be applicable for absorbers.
Abstract: Broadband absorption structures are an essential component of large format bolometer arrays for imaging GHz and THz radiation. We have measured electrical and optical properties of implanted silicon resistor layers designed to be suitable for these absorbers. Implanted resistors offer a low-film-stress, buried absorber that is robust to longterm aging, temperature, and subsequent metals processing. Such an absorber layer is readily integrated with superconducting integrated circuits and standard micromachining as demonstrated by the SCUBA II array built by ROE/NIST (1). We present a complete characterization of these layers, demonstrating frequency regimes in which different recipes will be suitable for absorbers. Single layer thin film coatings have been demonstrated as effective absorbers at certain wavelengths including semimetal (2,3), thin metal (4), and patterned metal films (5,6). Astronomical instrument examples include the SHARC II instrument is imaging the submillimeter band using passivated Bi semimetal films and the HAWC instrument for SOFIA, which employs ultrathin metal films to span 1-3 THz. Patterned metal films on spiderweb bolometers have also been proposed for broadband detection. In each case, the absorber structure matches the impedance of free space for optimal absorption in the detector configuration (typically 157 Ohms per square for high absorption with a single or 377 Ohms per square in a resonant cavity or quarter wave backshort). Resonant structures with -20% bandwidth coupled to bolometers are also under development; stacks of such structures may take advantage of instruments imaging over a wide band. Each technique may enable effective absorbers in imagers. However, thin films tend to age, degrade or change during further processing, can be difficult to reproduce, and often exhibit an intrinsic granularity that creates complicated frequency dependence at THz frequencies. Thick metal films are more robust but the requirement for patterning can limit their absorption at THz frequencies and their heat capacity can be high. patterned absorber structures that offer low heat capacity, absence of aging, and uniform, predictable behavior at THz frequencies. We have correlated DC electrical and THz optical measurements of a series of implanted layers and studied their frequency dependence of optical absorption from .3 to 10 THz at cryogenic temperatures. We have modeled the optical response to determine the suitability of the implanted silicon resistor as a function of resistance in the range 10 Ohms/sq to 300 Ohms/sq.