The RIMO

Overview

The RIMO, or Reduced Instrument Model is a FITS file containing selected instrument characteristics that are needed by users who work with the released data products. It is described in detail in The HFI and LFI RIMO ICD (ref). There will be two RIMOs, one for each instrument, which will follow the same overall structure, but will differ in the details. The type of data in the RIMO can be:

Parameter 

namely scalars to give properties such as a noise level or a representative beam FWHM

Table 

to give, e.g., filter transmission profiles or noise power spectra

Image 

namely 2-D "flat" array, to give, e.g., the beam correlation matrices

The FITS file begins with primary header that contains some keywords that mainly for internal use and no data. The different types of data are written into different BINTABLE (for parameters and tables) or IMAGE (for 2-D arrays) extensions, as described below.

File Names

HFI

HFI_RIMO_R1.10.fits

LFI

LFI_RIMO_R1.12.fits

Detector-level parameter data

The detector parameter data are given in the form of a table giving the parameter values for each detector. The table columns (whose names are in BOLD ITALICS) are:

Bolometer name - DETECTOR 

These are the detector names. For HFI these will be of the form 217-3 for SWBs or 100-3b for PSBs, and for LFI they will have the form 27M or 18S. There are 52 HFI detectors and 22 LFI detectors.

Focal plane geometry parameters - PHI_UV, THETA_UV, and PSI_UV 

These parameters give the geometry of the focal plane, or the positions of the detectors in the focal plane in the Dxx reference frame. The angles that give the rotation of the beam pattern from a fiducial orientation (forward beam direction (z-axis) pointing along the telescope line of sight, with y-axis aligned with the nominal scan direction) to their positions in the focal plane. The fiducial position is that given by the Star Tracker. All angles are in radians. These parameters are derived from observations of bright planets; see Detector pointing for details.

Polarization parameters - PSI_POL, EPSILON 

These are the direction of maximum polarization, defined with the beam in the fiducial orientation described above, that is, before rotation onto the detector position, and the cross-polarization contamination (or leakage). These values are determined from ground-based measurements.

Beam parameters - FWHM, ELLIPTICITY, POSANG 

These are the mean FWHM of the scanning beam (in arcmin, the beam ellipticity (no units), and the position angle of the beam major axis. The scanning beam is that recovered from the observation of bright planets; details in Beams section.

Noise parameters - NET_TOT, NET_WHT, NET_OOF, F_KNEE, ALPHA 

Three NETs are given: one determined from the total noise (rms of the noise timeline, excluding glitched data and other non-valid data), one determined from the white noise level of the noise amplitude spectrum, and one determined from fitting a 1/f noise spectrum, described by the function [math]\sigma^2(1+(f_{knee}/f)^\alpha)[/math] to the noise Power spectrum. In the latter, the F_KNEE and ALPHA parameters are the frequency where the 1/f component meets the white noise level, and the slope of the former. so that the slope is is about twice the slope of the amplitude spectrum. The NETs are in units of Kcmb or MJy/sr * sqrt(s).

Detector sampling frequency - F_SAMP, which is self-explanatory.

In the HFI RIMO, this table includes entries for the RTS bolometers (143-8 and 545-3), which are approximate or 0.00 when not evaluated.

Map-level parameter data

The map-level data table contains the effective beam solid angle (total and out to different multiples of the beamFWHM) and noise information. It is written into a BINTABLE extension named MAP_PARAMS whose structure is different for HFI and LFI and is as follows. The noise description below is very simplified; a more accurate rendition can be obtained from the half-ring maps. Regarding the characterization of systematics, the user should use the survey differences.

HFI

FREQUENCY (String) 

a 3-digit string giving the reference frequency in GHz, i.e., of the form 217

OMEGA_F, OMEGA_F_ERR (Real*4) 

the full beam solid angle and its uncertainty, in armin²

OMEGA_1, OMEGA_1_DISP (Real*4) 

the beam solid angle out to 1FWHM, and its dispersion, in arcmin²

OMEGA_2, OMEGA_2_DISP (Real*4) 

the beam solid angle out to 2FWHM, and its dispersion, in arcmin²

FWHM (Real*4) 

FWHM of a Gaussian beam having the same (total) solid angle, in armin². This is the best value for source flux determination

FWHMGAUS (Real*4) 

FWHM derived from best Gaussian fit to beam maps, in armin². This is the best value for source identification

NOISE (Real*4) 

This is the typical noise/valid observation sample as derived from the high-l spectra of the half-ring maps, in the units of the corresponding map

For the Omega columns, the 'DISP' (for dispersion) column gives an estimate of the spatial variation as a function of position on the sky. This is the variation induced by combining the scanning beam determined from the planet observations with the scanning strategy, as described in Beams.

LFI

FREQUENCY (String) 

a 3-digit string giving the reference frequency in GHz, i.e., of the form 030, 044, 070

FWHM (Real*8) 

FWHM of a Gaussian beam having the same (total) solid angle, in arcmin

NOISE (Real*8) 

This is the average noise in T[math]\cdot[/math]s^1/2

CENTRALFREQ (Real*4) 

This is the average central frequency in GHz

FWHM_EFF, FWHM_EFF_SIGMA (Real*4) 

This is the average FWHM of the effective beam, in arcmin, and its dispersion

ELLIPTICITY_EFF, ELLIPTICITY_EFF_SIGMA (Real*4) 

This is the average ellipticity and its dispersion

SOLID_ANGLE_EFF, SOLID_ANGLE_EFF_SIGMA (Real*4) 

This is the average full beam solid angle, in arcmin², and its dispersion

Effective band transmission profiles

The effective filter bandpasses are given in different BINTABLE extensions. The extension is named BANDPASS_{name}, where name specified the frequency channel. In the case of the maps, the bandpasses are a weighted average of the bandpasses of the detectors that are used to build the map. For details see Planck-2013-IX. The bandpasses are given as 4-column tables containing:

HFI

WAVENUMBER (Real*4) 

the wavenumber in cm-1, conversion to GHz is accomplished by multiplying by [math]10^{-7}c[/math] [mks].

TRANSMISSION (Real*4) 

the transmission (normalized to 1 at the max for HFI)

ERROR (Real*4) 

the statistical [math]1\sigma[/math] uncertainty for the transmission profile.

FLAG (Integer) 

a flag indicating if the data point is an independent frequency data point (nominally the case), or an FTS instrument line shape (ILS)-interpolated data point. The frequency data has been over-sampled by a factor of ~10 to assist in CO component separation efforts Planck-2013-IXPlanck-2013-XIII.

The number of rows will differ among the different extensions, but are the same, by construction, within each extension. Tables with the unit conversion coefficients and color correction factors for the HFI detectors (and LFI in some instances), including uncertainty estimates based on the uncertainty of the HFI detector spectral response are given in this appendix.

LFI

there was some talk of changing wn to freq ... TBD

WAVENUMBER (Real*8) 

the wavenumber in GHz.  ???

TRANSMISSION (Real*8) 

the transmission (normalized to have an integral of 1 for LFI)

UNCERTAINITY (Real*4) 

the statistical [math]1\sigma[/math] uncertainty for the transmission profile (not provided for LFI)

FLAG (Character) 

a flag, not used by now by the LFI

The number of rows will differ among the different extensions, but are the same, by construction, within each extension.

Detector noise spectra

HFI

these are the ring noise amplitude spectra averaged over about 5000 rings in order to give a representative spectrum. The spectra of all 50 valid bolometers are given in a single table. The spectra have a maximum frequency (Nyquist) of 90.18685Hz, also given the the F_NYQ keyword, and are built over 32768 points, giving a lower frequency of 2.75 mHz.

LFI 

TBW

The keyword F_NYQ gives the Nyquist frequency, and can be used together with the number of points in the spectrum to reconstruct the frequency scale. The BINTABLE has Ndetector columns by Npoints rows.

Beam Window Functions

Beam window functions and associated error descriptions are written into a BINTABLE for each detection unit, where detection unit consists of an auto or a cross product (for HFI only) of one (or two) frequency maps or detset maps used in the likelihood. Here they are:

For the HFI

• the 6 HFI frequency channels, producing 21 extensions
  • 100, 143, 217, 353, 545, 857
• 26 detsets, producing 351 extensions; the detsets used are, by frequency channel:
  • 100-DS1, 100-DS2,
  • 143-DS1, 143-DS2, 143-5, 143-6, 143-7,
  • 217-DS1, 217-DS2, 217-1, 217-2, 217-3, 217-4,
  • 353-DS1, 353-DS2, 353-1, 353-2, 353-7, 353-8,
  • 545-1, 545-2, 545-4,
  • 857-1, 857-2, 857-3, 857-4

For the LFI

• the 3 LFI frequency channels, producing 3 extensions
  • 30, 44, 70

and the extension names are of the form BEAMWF_U1XU2 where U1 and U2 are one (possibly the same) detection unit from one of the main groups above (i.e. there are no cross products between detsets and frequency channels, or between HFI and LFI). Each extension contains the columns:

NOMINAL (Real*4) 

the beam window function proper,

EIGEN_n (Real*4, n=1-5 for the HFI, n=1-4 for the LFI)

the five/four corresponding error modes.

and the following keywords give further information, only for the HFI:

NMODES (Integer) 

the number of EIGEN_* modes,

LMIN and LMAX (Integer) 

the starting and ending (both included) multipoles of the vectors NOMINAL and EIGEN_*

LMIN_EM and LMAX_EM (Integer) 

that give the range of the valid samples of the EIGEN_* vectors. Here LMAX_EM is always less than or equal to LMAX. On the range LMAX_EM+1 to LMAX the values of EIGEN_* are set to NaN, while the values of NOMINAL only are a Gaussian extrapolation of the lower multipole window function, only provided for convenience.

CORRMAT (string) 

the name of the extension containing the corresponding beam correlation matrix

Beam Correlation Matrix

Two beam correlation matrices are given for the HFI, in two IMAGE extensions:

CORRBEAM_FREQ (Real*8) 

for the frequency channels (21 units), 105x015 pixel matrix,

CORRBEAM_DSET (Real*8) 

for the detsets (351 units), 1755x1755 pixel matrix

Each is a symmetric matrix with 1-valued diagonal, made of NBEAMS*NBEAMS blocks, each block being NMODES*NMODES in size. The n$^{th}$ row- (and column-) block entry relates to the B(l) model whose name is indicated in ROWn = BEAMWF_U1XU2 keywords, and the corresponding eigenmodes are stored in a HDU of the same name.

Each extension contains also the following keywords:

NDETS (Integer) 

the number of detector units

NBEAMS (Integer) 

the number of beams = NSETS * (NSETS+1) / 2

NMODES (Integer) 

here 5

L_PLUS (Integer) 

Eigenmode > 0 to break degeneracies

BLOCKn (string) 

for n=1-NBEAMS, gives the name of the extension containing the beam WF and error eigenmodes for the nth block

and some other ones for internal data checking and traceability

No beam correlation matrices are produced by the LFI by now.

Appendices

• Unit correction and color correction tables