Development of Kinetic Inductance Detectors in Grenoble Martino - - PowerPoint PPT Presentation

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Development of Kinetic Inductance Detectors in Grenoble Martino - - PowerPoint PPT Presentation

Development of Kinetic Inductance Detectors in Grenoble Martino Calvo Institut Nel, CNRS Grenoble Outline 1 A ground-based KID instrument: NIKA2 2 KID for higher frequencies (>300GHz) 3 KID for lower frequencies (<100GHz)


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Development of Kinetic Inductance Detectors in Grenoble

Martino Calvo Institut Néel, CNRS Grenoble

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2 – KID for higher frequencies (>300GHz)

Outline

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1 – A ground-based KID instrument: NIKA2 3 – KID for lower frequencies (<100GHz) 4 – Getting ready for space...

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30 m

Correct Field Of View up to 6.5 arcmin 30 m aperture 12 arcsec @ 1.25mm 17 arcsec @ 2mm Multi-bands measurements

A unique tool for mm-wave astronomy!

2mm 1.25mm

Sierra Nevada (Spain) @2900m a.s.l.

The IRAM 30m telescope

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One of the largest single-dish antennas worldwide for the millimetric band

Thousands of ultrasensitive detectors → KID!

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Correct FOV:

The NIKA2 camera

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NIKA: the first KID based camera open to external astronomers!

6.5 arcmin Total pixel count: ≈ 3000 Arrays count: 3 (2mm + 2 x 1.25mm)

The new generation photometric instrument for the 30m telescope

NIKA2: New IRAM KID Array 2

On site since last October! (…and for the coming 10 years…)

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1.3 ton 2.3m length Cryogen free Base T ≈ 150mK Full remote operation

A NON-space-like cryostat!

The cryostat :

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1.3 ton 2.3m length Cryogen free Base T ≈ 150mK Full remote operation

The cryostat : The optics :

Splitting achieved using quasi-optical elements

A NON-space-like cryostat!

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1.3 ton 2.3m length Cryogen free Splitting achieved using quasi-optical elements Base T ≈ 150mK Full remote operation 2 colours, + 2 polarizations at 1mm

2mm 2mm 1mm H 1mm H 1mm V 1mm V

Dichroic Polarizer

The cryostat : The optics :

A NON-space-like cryostat!

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NIKA2 KID arrays

2mm: 600÷1000 pixels 1.25mm: 1200÷2000 pixels 4 feedlines 8 feedlines

1000 pixels 2mm array

NIKELv1 boards: MUX factor 400 over 500MHz band Single 4'' wafer fabrication Current MUX factor: 250 (for safety + Qi on ground!)

  • O. Bourrion et al.,

2012 JINST 7 P07014

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The 'house specialty': Hilbert LEKID

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Hilbert LEKID design, 2-pol

  • M. Roesch et al., Proc ISSTT 2011

Hilbert LEKID: a modified version of the standard LEKID design Inductive line based on Hilbert fractal pattern Inductor = radiation absorber!

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The 'house specialty': Hilbert LEKID

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Hilbert LEKID design, 2-pol

  • M. Roesch et al., Proc ISSTT 2011

Hilbert LEKID: a modified version of the standard LEKID design Inductive line based on Hilbert fractal pattern Inductor = radiation absorber! Need to match Zeff of meander to Zwave

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The 'house specialty': Hilbert LEKID

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Hilbert LEKID design, 2-pol

  • M. Roesch et al., Proc ISSTT 2011

2mm

Hilbert LEKID: a modified version of the standard LEKID design Inductive line based on Hilbert fractal pattern Inductor = radiation absorber! Need to match Zeff of meander to Zwave Zeff = R□ ∙ (s+w)/w s w High absorption efficiency over large band NIKA2 pixels based on thin film Al (<20nm) Feedline: CPW or MS

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LEKID coupling to radiation

7 n=1 n=3.4 Zeff≈377W

Basic principle:

Backshort (2n+1)l/4 Zwave≈377W

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LEKID coupling to radiation

7 l/4 n=1 n=3.4 n=1 Zeff≈110W l/4 n=1 n=3.4 Zeff≈377W

CPW : back-illumination + l/4 backshort Microstrip : front illumination

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LEKID coupling to radiation

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CPW : back-illumination + l/4 backshort Microstrip : front illumination

l/4 n=1 n=3.4 n=1 Zeff≈110W l/4 n=1 n=3.4 neff nAR Zeff≈(377/nAR)W

AR coating: integrated AR coating: external BI: ideal for large band applications FI: ideal for narrower bandwidths

h > 60% over 100% band hmax ≈ 100% at center of 30% band

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Lab characterization testbench

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Sky simulator beam maps/responsivity Martin-Pupplet interferometer absorption spectra

Cold BB load → sky A planet !

Available tools allow to fully characterize the arrays: + radioactive sources & fast electronics CR impacts!

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Sample array: NIKA2 2mm

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NIKA2 'AR11' array:

1020 pixels, CPW feedline, AR layer by dicing

4 x 250 pixels, simultaneous readout

f shift (Hz)

Map of 'planet' (and wire..)

>80% good pixels!

After removal of doubles and bad KID

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NIKA2 arrays on the sky

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NIKA2 started observations last October For the time being, runs dedicated mainly to commissioning Full operation will start next January 2mm 1.25mm V 1.25mm H

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NIKA2 arrays on the sky

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NIKA2 started observations last October For the time being, runs dedicated mainly to commissioning Full operation will start next January

f shift (Hz)

A real planet! (Uranus) (and a real atmosphere...)

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NIKA2: first light!

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DR21OH star forming region:

P r e l i m i n a r y !

Integration time: 12 min

Credit: N. Ponthieu and NIKA2 collaboration

P r e l i m i n a r y !

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NIKA2: first light!

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SZ effect in cluster CLJ1227

P r e l i m i n a r y !

Integration time: 1h06min

Credit: F. Ruppin and NIKA2 collaboration

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What's next?

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Plenty of good news NIKA2 is up and running...

  • it works very well! Results (& papers…) on their way.
  • experience for detectors in the 100-300GHz range
  • time to explore something new!
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What's next?

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Plenty of good news NIKA2 is up and running...

  • it works very well! Results (& papers…) on their way.
  • experience for detectors in the 100-300GHz range
  • time to explore something new!

100GHz 300GHz 50GHz 700GHz

(luckily enough, choosing ramen is much harder!)

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14 100GHz 50GHz 700GHz

Going to higher frequencies...

300GHz

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Going to higher frequencies...

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Can keep same technology (eg, materials!) Relatively easy to modify LEKID to cover the 300→600GHz range In theory, just need to change the geometry a bit: w, s << l

2mm

s w

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First test mask for high n LEKID

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3.2mm 3.2mm First test mask already made Teaser: pixel size and meander type are not chosen at random! Goal is just a first iteration of the loop design/fabrication/test/feedback! 4 different sub-arrays of 60 pixels each

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First results

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Df0 Df0 ≈ 400kHz DP ≈ 100pW Note #1: must increase stray-light rejection (as of now likely the limiting factor to our sensitivity!) Note #2: optical path not yet in final configuration so power per pixel is a rough estimate

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First results

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Note #1: must increase stray-light rejection (as of now likely the limiting factor to our sensitivity!) Note #2: optical path not yet in final configuration so power per pixel is a rough estimate Qi = Df/f0 ≈ 6000!! Df f0

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First results

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Current design is not yet optimized to maximize absorption... ...but already achieved a very large band! More data needed for an 'absolute' value of absorption efficiency (need to consider HDPE lenses, BB power, atmosphere...)

LP optical filter Al cutoff

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New mask design

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Already designed a second generation pixel (denser meander) Increase absorption by a factor ≈3 (if we believe in simulations!) Improve baffling and optics of dedicated test cryostat Resonances are at very low frequencies (a pro?) Denser meander means longer lines → need to check yield! Show sensitivity under representative background load

Next steps:

Test new materials (eg lower eeff wafer)

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18 50GHz 700GHz

Going to lower frequencies...

300GHz 100GHz

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Going to lower frequencies...

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Ecp = 3.5kbT

c

Not as straightforward… KID are pair-breaking detectors! Thin Aluminum ok only above ≈ 100GHz!

Al cutoff

Eg = hn ngap ≈ T

c∙ 73 GHz

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Going to lower frequencies...

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Not as straightforward… KID are pair-breaking detectors! Thin Aluminum ok only above ≈100GHz! Plenty of other materials available, but beware of their properties! Example: TixN1-x, NbxSi1-x... Maybe Ti/TiN?

!!

TixN1-x: NEP worse under lower background! ngap ≈ T

c∙ 73 GHz

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Bi-layer LEKID for low n applications

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Bi-layers have been widely used (for example for TES!) Proximity effect gived Tc intermediate between 2 materials Example : Ti/Al! Different tests made, best results for Ti10nm/Al25nm

T

c ≈ 0.9K

ncutoff ≈ 65GHz

  • A. Catalano et al.,

A&A, 580 (2015) A15

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Bi-layer LEKID for low n applications

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Bi-layers have been widely used (for example for TES!) Proximity effect gived Tc intermediate between 2 materials Example : Ti/Al! Different tests made, best results for Ti10nm/Al25nm

  • A. Catalano et al.,

A&A, 580 (2015) A15

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Getting ready for space!

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So far so good… But are KID really ready for space? Try to ask ESA! (And I guess JAXA/NASA...) Basically, no technology can be flown if it didn't fly before (??)

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Getting ready for space!

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So far so good… But are KID really ready for space? Try to ask ESA! (And I guess JAXA/NASA...) Basically, no technology can be flown if it didn't fly before (??) Is there a workaround? Demonstrate the technology using a balloon!

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The PlanB / B-SIDE project

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PlanB: a French KID-based balloon experiment Follow-up of the PILOT project Main goal is to measure the polarized emission of foregrounds

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PlanB / B-SIDE overview

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Field of view : 3° Dual-polarization (cold 45° polarizer) Rotating HWP at 4K

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PlanB / B-SIDE overview

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Field of view : 3° Dual-polarization (cold 45° polarizer) Rotating HWP at 4K Resolution @ 550GHz: between 3' and 6' 2x 500-1000 pixels MUX ratio of 250 Flight: 24hrs in April 2018 from Australia BICEP2 field

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PlanB / B-SIDE goals

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Accurate measurements of foreground polarization Allow clean-up of existing datasets Demonstrate performance of KID in space-like conditions!

  • KID NEP in-flight under low optical load
  • Effect of CR (glitches!)
  • Low-consumption readout electronics
  • Any unexpected surprises?
  • and a bonus: Closed Cycle Dilution Refrigerator!
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Conclusions

Lots of experience gained thanks to the NIKA2 project Work has already started to widen the band of operation of

  • ur detectors

The situation looks promising for both high (>300GHz) and low (<100GHz) frequencies

Thank you!

The PlanB/B-SIDE balloon project can be a key step to demonstrate the suitability (and 'readiness'!) of KID arrays for space-based missions Happy to collaborate!