PICO 60 Results and PICO 40L Status Carsten B. Krauss for the PICO - - PowerPoint PPT Presentation

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PICO 60 Results and PICO 40L Status Carsten B. Krauss for the PICO - - PowerPoint PPT Presentation

PICO 60 Results and PICO 40L Status Carsten B. Krauss for the PICO Collaboration TAUP 2019, Sept 09 2019 1 Outline PICO 60 Results Electron Recoil Rejection PICO 40L Summary 2 PICO 60 PICO 60 was initially


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SLIDE 1

PICO 60 Results and PICO 40L Status

Carsten B. Krauss 
 for the PICO Collaboration TAUP 2019, Sept 09 2019

  • 1
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SLIDE 2

Outline

  • PICO 60
  • Results
  • Electron Recoil Rejection
  • PICO 40L
  • Summary

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SLIDE 3

PICO 60

  • PICO 60 was initially filled with 26.8kg of CF3I

(PRD93, 052014, 2016)

  • This fill was successful, but limited by

anomalous backgrounds

  • The chamber was subsequently filled with

52.2kg of C3F8 (run 1: 3.3keV threshold, run 2: 2.45keV, blind analysis)

  • Particulate contamination and the water buffer

liquid ultimately limited this chamber design

  • Later, we also learned that neutron

backgrounds prevented background free

  • peration for exposures larger than ~1000kg

days

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SLIDE 4

Bubble Chambers for Dark Matter

  • Use moderately superheated liquid with

large fluorine content to boost the spin dependent WIMP sensitivity

  • The bubble chambers stays expanded

until the cameras detect a bubble in an image (or a timeout occurs)

  • Piezoelectric acoustic sensors pick up

waveforms that allow to distinguish louder alpha background events from nuclear recoil events

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SLIDE 5

Bubble Chambers for Dark Matter

  • Use moderately superheated liquid with

large fluorine content to boost the spin dependent WIMP sensitivity

  • The bubble chambers stays expanded

until the cameras detect a bubble in an image (or a timeout occurs)

  • Piezoelectric acoustic sensors pick up

waveforms that allow to distinguish louder alpha background events from nuclear recoil events

  • Phys. Rev. D 100, (2019) no.5, 052001

4

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SLIDE 6

Bubble Chambers for Dark Matter

  • Use moderately superheated liquid with

large fluorine content to boost the spin dependent WIMP sensitivity

  • The bubble chambers stays expanded

until the cameras detect a bubble in an image (or a timeout occurs)

  • Piezoelectric acoustic sensors pick up

waveforms that allow to distinguish louder alpha background events from nuclear recoil events

  • Phys. Rev. D 100, (2019) no.5, 052001

4

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SLIDE 7

C3F8 Run 1 Result (SD)

The 90% C.L. limit on the SD WIMP-proton cross section from PICO-60 C3F8 plotted in blue, along with limits from PICO-60 CF3I (red), PICO-2L (purple), PICASSO (green), SIMPLE (orange), PandaX-II (cyan), IceCube (dashed and dotted pink), and SuperK (dashed and dotted black). The indirect limits from IceCube and SuperK assume annihilation to τ leptons (dashed) and b quarks (dotted).

Phys.Rev.Lett. 118 (2017) no.25, 251301

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SLIDE 8

C3F8 Run 2 Result (SD)

90% C. L. limit on the SD WIMP proton cross section from the profile likelihood analysis of the PICO-60 C3F8 combined blind exposure plotted in thick maroon, along with limits from the first blind exposure of PICO-60 C3F8 (thick blue), as well as limits from PICO-60 CF3I (thick red), PICO-2L (thick purple), PICASSO (green band), SIMPLE (orange), XENON1T (gray), PandaX-II (cyan), IceCube (dashed and dotted pink), and SuperK (dashed and dotted black). The indirect limits from IceCube and SuperK assume annihilation to τ leptons (dashed) and b quarks (dotted).

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Phys.Rev. D100 (2019) no.2, 022001

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SLIDE 9

PICO 60 Complete Exposure

  • The new results is improved by
  • Lower threshold (3.3 keV ➝ 2.45 keV)
  • Better understanding of the threshold by careful analysis of years of calibration data
  • The PICO 60 detector was ultimately limited by backgrounds and made space for PICO 40L

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SLIDE 10

ame device, beg

PICO 60 PICO 40L

8

  • PICO 60 was limited by “small” pressure vessel that allowed

backgrounds to enter the chamber

  • The buffer liquid and particulate contamination also created

hard to reject recoil like events

  • To address this, PICO 40L is turned “right-side-up” to eliminate

the buffer liquid and collect possible dust contaminants in the inactive region. PICO 40L also has a much larger pressure vessel to reduce the impact of external backgrounds

  • This design requires extra cooling systems in the lower part
  • f the detector
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SLIDE 11

ame device, beg

PICO 60 PICO 40L

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SLIDE 12

ame device, beg

PICO 60 PICO 40L

Superheat Cold

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SLIDE 13

PICO 40L

  • The detector is filled with active

liquid and fully instrumented

  • Currently in commissioning
  • Regular data taking will start in Fall

2019

ame device, beg

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SLIDE 14

PICO 40L construction

  • Jan - April 2019

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SLIDE 15

First Bubble!

  • The detector was brought to

temperature and the first bubbles were recorded

  • Temperature control trigger

systems still need to be fully commissioned in the coming weeks/months

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SLIDE 16

Expected PICO40L sensitivity

  • Exploring parameter space below the Xe CEνNS cross

section (grey area)

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SLIDE 17

Post PICO 40L Plans

  • With a hydrogenated liquid for PICO 40L (after the C3F8

program is complete) we can extend the range of bubble chambers to much lower masses

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SLIDE 18

Summary

  • PICO has operated 3 generations of bubble chambers

since 2012

  • We have been able to constantly improve the sensitivity

towards spin depended dark matter with C3F8 as target

  • PICO 40L will improve the reach once again
  • PICO 500 is starting to be constructed in 2020 


➞ see A. Noble’s talk tomorrow

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