| 308 | |
| 309 | [[Image(rnovalmc_4668_image.png)]] |
| 310 | |
| 311 | Above is an image of the field with central frequency 4668 MHz. The ToO target is at RA = 05h40m44.2s Dec = -66d40m11.6. |
| 312 | So it seems that we have not detected the target, but there are two other sources apparent in the image. Using |
| 313 | NED we can identify these sources as SUMSS J054003-663939 (RA = 05h40m03.7s Dec = -66d39m40s, top right source) and |
| 314 | SUMSS J054125-664307 (RA = 05h41m25.2s Dec = -66d43m07s, bottom left source). Let's look at all the images together |
| 315 | in the image below. |
| 316 | |
| 317 | [[Image(rnovalmc_montage.png)]] |
| 318 | |
| 319 | In this image, the central frequency is increasing in each successive plot to the right and down. We can see here another |
| 320 | effect of the increasing central frequency. The two sources are seen to "move" towards the edge of the field in successive |
| 321 | images, and this is because the primary beam of the antenna gets smaller with increasing frequency. |
| 322 | |