SSC Home Page

IRS Long-High Time-Dependent Dark


SPITZER HOME || SPITZER SCIENCE || INSTRUMENTS || SCIENCE USER SUPPORT || SEARCH

+ - General Information
- Spitzer News
- Research Categories
- Science Schedules
- Advisory Groups
- Observing Rules
- Legacy Program
- First-Look Survey
+ - Observatory & Instruments
- Overview
- PCS
- IRAC
- IRS
- MIPS
- AOTs
+ - Science User Support
- Proposal Kit
- Documents
- Tools
+ - Approved Programs
- Observing Schedules
+ - Data Archives / Analysis
- Science Archive Access
- Post-BCD Tools
+ - Data Analysis Funding
- Information
+ - FAQ
- Search site
During observations with the Long-High (LH) module, the dark current may have anomalously high values in the first 100-200 seconds of a series of exposures. Depending on the integration time and the number of cycles selected, data in the first exposure (or first nod position) may be affected. The "excess flux" is not evenly distributed over the LH array, being brightest on the blue end of each echelle order. In Figure 1 we show the difference between LH nod 1 and nod 2 spectra of a faint point source. The faint excess flux is seen as a bright band stretching across the bottom of the array, both on and between the orders. This phenomenon manifests itself in extracted spectra of relatively faint sources as a "scalloping" or order tilting, wherein the slopes of affected orders are made bluer (flatter), inducing order-to-order discontinuities. The order-to-order discontinuities are typically 30-50 mJy. The magnitude of the effect does not seem to be related to source brightness. In Figure 2 we show two extracted LH spectra of a faint point source. The top spectrum has the source at the nod 1 position, while the bottom spectrum has the source at the nod 2 position. A background sky spectrum has not been subtracted in either case, but the edges of the (color-coded) orders have been trimmed. The order mismatches are obvious in the nod 1 data, but vanish in the nod 2 data. If you have observations of faint point sources with LH, and you are seeing these order tilts in your spectra, we recommend that you check your LH BCDs in the first nod position (or during the first few hundred seconds of a series of exposures), to see if this effect is more apparent. If order discontinuities such as described above are evident in the first few exposures or the first nod position, observers should consider not including these data during co-addition. If your LH data do not show this effect, you can include all the data in your final co-added spectrum. We are currently exploring ways to remove or reduce these effects in the way we take and process the data.

Figure 1

Figure 1

Figure 2

Figure 2


Go back to IRS page


SPITZER HOME || SPITZER SCIENCE || INSTRUMENTS || SCIENCE USER SUPPORT || SEARCH

help@spitzer.caltech.edu
http://ssc.spitzer.caltech.edu/irs/timedepdark.html
This file was last modified on Fri Sep 29 08:42:38 2006.

California Institute of Technology Jet Propulsion Laboratory NASA