Difference between revisions of "Map-making LFI"
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==Noise Monte Carlo Simulation== | ==Noise Monte Carlo Simulation== | ||
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===Overview=== | ===Overview=== | ||
Calculating and handling full pixel-to-pixel noise covariances in Planck maps if feasible only at low resolution. | Calculating and handling full pixel-to-pixel noise covariances in Planck maps if feasible only at low resolution. | ||
To support the analysis of high-resolution maps, a Monte Carlo set of noise maps were produced. | To support the analysis of high-resolution maps, a Monte Carlo set of noise maps were produced. | ||
These noise Monte Carlos were produced at two levels of the analysis: 1) LFI Monte Carlo (MC) as part of the LFI data processing, and 2) Full Focal Plane (FFP) Monte Carlo as part of the joint HFI/LFI data processing. This page describes the LFI noise MC. For the FFP MC, see [[HL-sims]]. | These noise Monte Carlos were produced at two levels of the analysis: 1) LFI Monte Carlo (MC) as part of the LFI data processing, and 2) Full Focal Plane (FFP) Monte Carlo as part of the joint HFI/LFI data processing. This page describes the LFI noise MC. For the FFP MC, see [[HL-sims]]. | ||
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===Inputs=== | ===Inputs=== | ||
The noise MC assumes a three-parameter noise model: white noise level ($\sigma$), slope, and knee frequency ($f_\mathrm{knee}$), so that the noise power spectrum is assumed to have the form | The noise MC assumes a three-parameter noise model: white noise level ($\sigma$), slope, and knee frequency ($f_\mathrm{knee}$), so that the noise power spectrum is assumed to have the form | ||
− | :$ P(f) = \frac{2\sigma^2}{f_\mathrm{sample}}\left(\frac{f}{f_\mathrm{knee}}\right)^\mathrm{slope} $. | + | :$ P(f) = \frac{2\sigma^2}{f_\mathrm{sample}}\left[1+\left(\frac{f}{f_\mathrm{knee}}\right)^\mathrm{slope}\right] $. |
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+ | Here $f_\mathrm{sample}$ is the sampling frequency of the instrument. The first term corresponds to white noise and the second term to correlated ($1/f$) noise. The noise parameters were determined separately for each radiometer as described in [[TOI-Noise LFI]], assuming they stayed constant over the mission. | ||
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+ | The detector pointing was reconstructed from satellite pointing, focal-plane geometry, and | ||
+ | |||
+ | The noise was generated internally in the Madam map-making code using a Stochastic Differential Equation (SDE) method, to avoid time-consuming writing and reading noise timelines to/from disk. Noise for each pointing period was generated separately, using a double-precision random number seed constructed from the realization number, radiometer number, and the pointing period number; to allow regeneration of the same noise realization when needed. White noise and $1/f$ noise were generated separately. | ||
− | + | The |
Revision as of 10:30, 19 October 2012
Noise Monte Carlo Simulation[edit]
Overview[edit]
Calculating and handling full pixel-to-pixel noise covariances in Planck maps if feasible only at low resolution. To support the analysis of high-resolution maps, a Monte Carlo set of noise maps were produced. These noise Monte Carlos were produced at two levels of the analysis: 1) LFI Monte Carlo (MC) as part of the LFI data processing, and 2) Full Focal Plane (FFP) Monte Carlo as part of the joint HFI/LFI data processing. This page describes the LFI noise MC. For the FFP MC, see HL-sims.
Inputs[edit]
The noise MC assumes a three-parameter noise model: white noise level ($\sigma$), slope, and knee frequency ($f_\mathrm{knee}$), so that the noise power spectrum is assumed to have the form
- $ P(f) = \frac{2\sigma^2}{f_\mathrm{sample}}\left[1+\left(\frac{f}{f_\mathrm{knee}}\right)^\mathrm{slope}\right] $.
Here $f_\mathrm{sample}$ is the sampling frequency of the instrument. The first term corresponds to white noise and the second term to correlated ($1/f$) noise. The noise parameters were determined separately for each radiometer as described in TOI-Noise LFI, assuming they stayed constant over the mission.
The detector pointing was reconstructed from satellite pointing, focal-plane geometry, and
The noise was generated internally in the Madam map-making code using a Stochastic Differential Equation (SDE) method, to avoid time-consuming writing and reading noise timelines to/from disk. Noise for each pointing period was generated separately, using a double-precision random number seed constructed from the realization number, radiometer number, and the pointing period number; to allow regeneration of the same noise realization when needed. White noise and $1/f$ noise were generated separately.
The
(Planck) Low Frequency Instrument
(Planck) High Frequency Instrument