Fig 4 - uploaded by Jonas Zmuidzinas
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Mask layout of the QMMIC substrate. Actual size is approximately 2.5x3.8 mm. The InP HEMTs are bonded to the three pads spaced horizontally across the center of the chip. The input is coplanar waveguide on the left, and the output is on the right. There are three bond pads at the top for gate bias, and three across the bottom for drain bias. 

Mask layout of the QMMIC substrate. Actual size is approximately 2.5x3.8 mm. The InP HEMTs are bonded to the three pads spaced horizontally across the center of the chip. The input is coplanar waveguide on the left, and the output is on the right. There are three bond pads at the top for gate bias, and three across the bottom for drain bias. 

Context in source publication

Context 1
... results of these simulations are plotted in Figure 3. The final mask layout is show in Figure 4. The input and output of the QMMIC chip are coplanar waveguide (CPW), both to avoid via holes and to allow the devices to be tested on a probe station. ...

Citations

Article
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We present a 12CO J ¼ 6-5 map of the nuclear regions of the starburst galaxy M82 at a resolution of 1400 taken at the Caltech Submillimeter Observatory (CSO). Hot spots were found on either side of the dynamical center. We compare our results with a high-resolution 12CO J ¼ 2-1 interferometer map, and present a 12CO J ¼ 6-5/12CO J ¼ 2-1 line ratio map obtained using a novel deconvolution technique. This line ratio is highest at the two J ¼ 6-5 integrated intensity peaks, reaching 0.4 and 0.5 in the northeast and southwest peaks, respectively, and is typically 0.2 elsewhere in the nuclear region. We also present measurements of 12CO J ¼ 4-3, 12CO J ¼ 3-2, and 13CO J ¼ 3-2, and an upper limit for 13CO J ¼ 6-5. We analyze these observations in the context of a two-component large velocity gradient (LVG) excitation model. Likelihood density curves were calculated for each of the model parameters and a variety of related physical quantities for the northeast and southwest peaks based on the measured line intensities and their associated uncertainties. This approach reveals in an unbiased way how well various quantities can be constrained by the CO observa- tions. We find that the beam-averaged 12CO and 13CO column densities, the isotopomer abundance ratio, and the area filling factors are among the best constrained quantities, while the cool component H2 density and pressure are less well constrained. The results of this analysis suggest that the warm gas is less dense than the cool gas, and that over half of the total molecular gas mass in these nuclear regions is warmer than 50 K. Subject headings: galaxies: individual (M82) — galaxies: ISM — galaxies: starburst — submillimeter
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