We have obtained a second-epoch observation of the Cassiopeia A supernova remnant (SNR) with the Chandra X-Ray Observatory to measure detailed X-ray proper motions for the first time. Both observations are 50 ks exposures of the ACIS-S3 chip, and they are separated by 2 years. Measurements of the thin X-ray continuum-dominated filaments located around the edge of the remnant (which are identified with the forward shock) show expansion rates from 0.02% to 0.33% yr -1 . Many of these filaments are therefore significantly decelerated. Their median value of 0.21% yr -1 is equal to the median expansion of the bright ring (0.21% yr -1 ) as measured with Einstein and ROSAT . This presents a conundrum if the motion of the bright ring is indicative of the reverse shock speed. We have also reevaluated the motion of the radio bright ring with emphasis on angle-averaged emissivity profiles. Our new measurement of the expansion of the angle-averaged radio bright ring is 0.07% ± 0.03% yr -1 , somewhat slower than the previous radio measurements of 0.11% yr -1 , which were sensitive to the motions of small-scale features. We propose that the expansion of the small-scale bright ring features in the optical, X-ray, and radio do not represent the expansion of the reverse shock, but rather represent a brightness-weighted average of ejecta passing through and being decelerated by the reverse shock. The motion of the reverse shock itself is then represented by the motion of the angle-averaged emissivity profile of the radio bright ring.
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DeLaney et al. (2003) studied this question.
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