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Predicting Herschel

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Measuring Fluctuations & Counts Mattia Vaccari & Alberto Franceschini & Giulia Rodighiero & Stefano Berta Department of Astronomy - University of Padova – PowerPoint PPT presentation

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Title: Predicting Herschel


1
Predicting Herschel SCUBA2 ConfusionMeasuring
Fluctuations Counts Mattia Vaccari
Alberto Franceschini Giulia Rodighiero
Stefano BertaDepartment of Astronomy -
University of Padova
  • A) Summary
  • Confusion in Herschel SCUBA2 bands is
    estimated using two complementary criteria
  • ISO, Spitzer SCUBA counts are used to
    constrain models of extragalactic populations
  • Based on such models the two approaches
    respectively measure fluctuations due to
    unresolved sources and set a maximum number
    density for resolved sources
  • These two methods provide results which are in
    good agreement for all bands
  • Recommendations for planning Herschel SCUBA2
    extragalactic surveys are outlined

Mattia Vaccari mattia_at_mattiavaccari.net www.mattia
vaccari.net
  • B) Confusion at Long Wavelengths with Herschel
    SCUBA2
  • Confusion sets a major limit to the sensitivity
    of long-? extragalactic surveys
  • As IRAS first dramatically showed, the
    FIR/sub-mm sky is very densely populated
  • ISO Spitzer SCUBA confirmed this view
    providing a wealth of additional data
  • Great care must be taken in taking stock of
    current knowledge in order to predict Herschel
    SCUBA2 confusion limits and thus allow a timely
    planning of observations
  • C) Modelling ISO, Spitzer SCUBA Observations
  • Models by Franceschini et al. 2001 (AA, 378)
    were updated to account for intervened reanalyses
    of ISO 15 ?m data and results from Spitzer MIPS
    and SCUBA observations
  • Models describe available observables in terms
    of four populations
  • slowly or non-evolving disk galaxies blue
    dotted lines
  • type-1 AGNs evolving as shown by UV and X-ray
    selected quasars Seyferts green long-short
    dashed lines
  • moderate-luminosity starbursts with peak
    emission at z 1 cyan dot-dashed lines
  • ultra-luminous starbursts with peak evolution
    between z 2 and z 4 red long dashed
    lines
  • D) Measuring Confusion with Fluctuations
    Counts
  • Fluctuations measure fluctuations in the
    background due to unresolved sources
    Franceschini et al. 1989 (ApJ, 344) and set
    confusion at the 3 ? fluctuation level
  • Counts measure source counts and set
    confusion where a maximum number of sources per
    beam, or rather a minimum number of beams per
    source (bps), is reached Franceschini et al.
    2001 (AA, 378)
  • Roughly speaking, while Fluctuations follow
    the trend of counts fainter than the confusion
    limit, Counts follow the trend at brighter
    fluxes than that. The degree of consistency
    between the two depends on the slope of counts at
    and near this flux limit

MIPS 70 ?m
MIPS 24 ?m
  • E) Fluctuations vs. Counts Confusion Limits
  • 3 ? Fluctuations are very similar to Counts
    10 bps for PACS but nearer to 20 bps for SPIRE
  • This is due to the different slopes of PACS and
    SPIRE counts at and fainter than their 10 bps
    levels
  • The availability of multi-? (notably MIPS 24/70
    ?m and/or PACS) data will be invaluable in
    accurately pin-pointing SPIRE SCUBA2 sources in
    order to reach down to 10 bps fluxes in all
    Herschel bands

Channel PACS1 PACS2 PACS3 SPIRE1 SPIRE2 SPIRE3 SC2-S SC2-B
?m 70 110 170 250 350 500 450 850
Beam FWHM 4 .74 6.96 10.76 17.1 24.4 34.6 7.4 13.7
3 ? mJy 0.07047 1.002 7.484 18.12 22.55 20.19 1.967 1.383
10 bps mJy 0.1100 1.263 7.090 14.00 15.23 13.23 1.917 1.302
20 bps mJy 0.3029 2.746 11.82 20.49 21.65 18.31 3.426 2.125
30 bps mJy 0.4887 4.034 15.23 25.40 26.34 21.49 4.604 2.755
40 bps mJy 0.6656 5.110 18.12 29.18 29.93 24.09 5.630 3.253
50 bps mJy 0.8350 6.107 20.45 32.47 33.05 26.18 6.467 3.701
(See C) for Legenda)
Confusion sets in at a flux level determined by
the Beam FWHM line (left below) and the 10 beams
per source line (right below) respectively
Integral Counts
SCUBA2 850
SCUBA2 450
SPIRE 350
PACS 170
PACS 70
(See C) for Legenda)
Differential Counts
  • F) Recommendations for Herschel SCUBA2 Survey
    Planning
  • Target sensitivities envisaged in Herschel
    SCUBA2 surveys appear to be realistic from a
    confusion stand-point when modelling ISO
    Spitzer SCUBA results
  • In particular, reaching the 10 mJy level in all
    SPIRE bands appears to be feasible and thus
    somehow mandatory in order to fulfill Herschels
    potential for extragalactic surveys. Such deep
    SPIRE surveys should be undertaken over sky areas
    where deep Spitzer MIPS 24/70 ?m and/or PACS
    coverage is or will be available, e.g. within the
    most popular Cosmic Windows
  • Survey-like exploratory efforts should be
    undertaken at a relatively early time during
    Herschel SCUBA2 operations in order to measure
    actual confusion levels and thus ensure to make
    the most of Herschels 3-year life span and of
    SCUBA2s 2-year 5-year plans.

Herschel Extragalactic GT Survey Wedding Cake
Time (hr) PACS (659) SPIRE (850) Harwit
(10) (Spitzer Depths)
Name Area Field PACSTime SPIRE Time 70 110 170 250 350 500
- deg2 - hr hr mJy mJy mJy mJy mJy mJy
Clusters - - 80 100 - - - - - -
Level 1 0.04 GOODS-S 230 1030 1.0 1.0 1.0 3.3 4.0 4.6
Level 2 0.04 GOODS-N 27 10 2.0 2.8 3.0 6.7 8.1 9.2
Level 3 0.25 GOODS-S 34 25 2.2 6.2 6.7 10.5 12.7 14.5
0.25 Groth Strip 34 25 2.2 6.2 6.7 10.5 12.7 14.5
0.25 Lockman 34 25 2.2 6.2 6.7 10.5 12.7 14.5
Level 4 2 COSMOS 110 50 6.0 9.8 10.5 21.1 25.5 29.1
2 XMM-LSS 110 50 18 9.8 10.5 21.1 25.5 29.1
Level 5 10 Spitzer 185 200 18 16.9 18.0 23.6 28.5 32.5
Level 6 50 Spitzer - 150 18 - 120 61 74 84
  • G) Ongoing Work
  • Fitting additional observables (e.g. redshift
    distributions) into refined modelling picture
  • Comparing our estimates with results obtained
    using other confusion estimators
  • Providing a consensus confusion model suitable
    for survey planning
  • Applying techniques to other projects, e.g.
    Akari SPICA FIRM
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