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imagerteleconnotes20180807

Telecon Notes Aug 8, 2018

Attendance:

Regrets:

Agenda

Notes

PICO imager telecon - 8/8/2018

Participants: Kris, Qi, Roger, Tom, Jeff, Jacques, Toki

PICO Focal plane: Finalizing mechanical design (Qi)

On Indium conductivity

  • slide 6 Indium conductivity value between literature value and Bill's number are different by factor of x500
  • slide 6 For 1.8e-5 and 1.44 e-7, units are W/cm K
  • slide 7 Thermal conductivity goes as 1/t^2 at low temp. Extrapolated to 100 mK using data points from Sladek
  • slide 7 Assuming thermal conductivity from electron only - Phonon contribution will only add
  • slide 8 Using Sladek's value, 10 mW of loading will change temperature by 6 mK
  • slide 9 Indium bump bond has lower thermal conductivity. 9.9e-7 W/cm @ 100 mK - This means 20 uW of loading will increase FP temperature by 8mK
  • slide 9 Jacques asked “Where do you have cooling power requirement?”, Qi answered “requirement not stated in this slide”
  • slide 9 Toki asked: “what is expected optical load on focal plane?”, Qi answered “I don't know” Karl may know?
  • slide 9 Tom “~20 uW at focal plane is reasonable”
  • slide 9 Roger - This (indium bump bond) will work okay. We need to work on how we explain it. Talk about strategy to build proto-type and test
  • slide 9 Tom - We could also design focal plane with ribbon bond to further mitigate this issue
  • slide 9 Kris - If the bonding was not enough there is room to put gold wires
  • slide 9 Roger - Through wafer via is used in PIPER. Are there any thermal problem? PIPER did lab testing. So far no major problem. Paper on this is not out yet. Test was done @ 100 mK
  • slide 9 Roger - We should point to PIPER as existing proof of working focal plane with similar configuration.
  • slide 9 Jacques - Are there write up on estimates on mass on cold stage & requirement on cooling power for the focal plane?
  • slide 9 Toki - There is mass estimate at end of Qi's slide
  • slide 9 Roger - JPL have thermal engineer working on this
  • slide 9 Jacques - We should write down Write mass and cooling power requirement of the coldest stage

On back termination

  • slide 10 Qi - Cavity does not need to be stepped. Idea is to make non-resonant cavity
  • slide 10 Toki - There is a paper on pyramidal backshort for sinuous antenna.
  • slide 10 Roger - We put absorber in back before. About 10% of radiation goes in backlobe. This is not the biggest issue.
  • slide 10 Qi - lambda in the slide is for central band. Cavity is electrically quite small for lower frequency band
  • slide 10 Toki - Simons Observatory is trying similar reflective backshort idea. Their backshort is ~1 mm away from antenna for 90/150 GHz
  • slide 10 Toki - If we use absorber, we can then point to existing example. But this absorber has to be very thin.
  • slide 10 Qi - Via's height limit is 400 um~ 500um via conversation with Tom: Stack multiple layers with indium bump bond
  • slide 11 Qi - More indium bump bond can be added for heat sinking

On conical horn spacing

  • slide 15 Qi - Opening is larger than lenslet, but enough number of pixels fit with in focal plane area

On focal plane mass

  • slide 16 Roger: Mass seems low
  • slide 16 Roger: Scaling from SPIDER seems heavier
  • slide 16 Jeff: SPIDER weights 15~20 pounds with magnetic shielding
  • slide 16 Jeff: Cover plate weights a lot, cut back on B-field shielding
  • slide 16 Roger: We are not sure if we can get rid of B-field
  • slide 16 Jeff one to one comparison to see where delta is
    • Quick strawman number from Jeff's student - break down weight distribution into components
    • PICO does not have B-field shielding

Roger's update - Verbal update

  • Technology maturing schedule - How to mature technology up to TRL 5 by Oct 2023
  • 4 sections
    • LF detectors - multichroic
    • HF detectors - horn
    • Thermal design
    • Readout design
  • LF detectors
    • Focusing on this section
    • Pointing to existing experiments - for ex. SPT-3G's three color pixel
    • Talk about other approaches BICEP/ ACT, giving overview of technology in the field
  • Systematic effects are setting r at 1e-3.
    • Hope that over next decade we will push this down to 1e-4
    • Experiment will need to be supported to push down systematics through actual observation
    • List of experiments to mature this technology before 2023
  • HFT
    • People have made unpolarized absorbing detectors
    • SPTpol showed polarization versin at 90 GHz
  • Readout
    • Interested in having Hannes help Roger on this
    • Conservative TDM option. Does not mean FDM won't work, but TDM is close to what we need (x64)
    • PICO need x128, explain how we make this increase
  • Thermal design
    • Roger not involved as much - ask Amy on where this is
    • ADR system is being considered - They work, but some works to iron out for ex. B-field
    • Continuous dilution fridge version maybe interesting, but doesn't exist
    • Roughly 3~4 pages point
  • We can make detectors to work, but demonstrating systematics in actual experiment is necessary to convince reviewers
    • Balloon - NASA will support
    • R&D on detector NASA supported well
  • Schedule seems OK
  • IDS = Inflation and Dust Surveyer
imagerteleconnotes20180807.txt · Last modified: 2018/08/08 16:19 by wenxx181