Open Cavity Resonators The Orpheus Experiment Gray Rybka, - - PowerPoint PPT Presentation

open cavity resonators the orpheus experiment
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Open Cavity Resonators The Orpheus Experiment Gray Rybka, - - PowerPoint PPT Presentation

Open Cavity Resonators The Orpheus Experiment Gray Rybka, University of Washington Workshop on Microwave Cavity Design for Axion Detection LLNL - 2015 Source: K. Van Bibber, Vistas in Axion Physics 2012 Beyond Current Axion Experiments


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Open Cavity Resonators The Orpheus Experiment

Source: K. Van Bibber, Vistas in Axion Physics 2012

Gray Rybka, University of Washington Workshop on Microwave Cavity Design for Axion Detection – LLNL - 2015

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 2

Beyond Current Axion Experiments

Gen 2 ADMX Targets

Reaching the highest masses is challenging:

  • Smaller Volumes
  • Lower Qs

We have programs underway at UW (and elsewhere) to mitigate these challenges

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 3

Axion Haloscope

You Want:

  • Large Cavity Volume
  • High Magnetic Field
  • High Cavity Q

You Don't Want:

  • High Thermal Noise
  • High Amplifier Noise

See: Sikivie, Phys. Rev. Lett. 1983

a γ γ

Dark matter axions will convert to photons in a magnetic field. A high-Q cavity can enhance the conversion rate.

To make an axion haloscope as sensitive as possible -

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 4

Power From Axion Conversion

Axion-Photon Coupling Axion Frequency Resonator Quality

P=1.5×10

−21W (

B 7.6T )

2 gγ

0.97 ρa 0.45GeV /cc f a 750 MHz Q 70,000 Vf 220l

Magnetic Field Dark Matter Density

(∫ ⃗ E⋅⃗ BdV )

2

B

2∫ ⃗

E⋅⃗ E dV

Overlap of integral of electric field of resonance and magnetic fields

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 5

Maximizing Power at High Frequencies

This mode couples to axions. (Form Factor 0.8) This mode does not. (Form Factor 0)

Q decreases with increasing frequency, and volume decreases with wavelength in a constant magnetic field

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 6

Ari Brill (Yale REU Student) Kunal Patel UW Katleiah Ramos UW Robert Percival UW Not Pictured: Gray Rybka, Andrew Wagner (postdoc)

“Orpheus” An experiment to look for higher-mass dark matter axions

Built at operated primarily by undergraduates

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 7

This is at optimal overlap

Key Concept: Spatially varying magnetic field matches E&M mode structure

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 8

Orpheus Design

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 9

Open Resonator Prototype

Network Analyzer (Measures Q) Reflector Wire Planes Reflector Spectrum Analyzer (Measures Power Out) Amplification Wire Plane Power Supply ADMX R&D: Orpheus

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 10/45

Orpheus Data Analysis

Raw Power Spectrum Corrected Power Spectrum Axion Search

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 11

Orpheus Results

Many orders of magnitude improvement possible with improved B-Field, volume, Q, noise temperature Orpheus was operated for two weeks. Results published in Rybka et al. Phys. Rev. D 91, 011701(R) (2015) Simple benchtop sensitivity competitive with large-scale national lab laser experiments

Mass Prediction*

*prediction from Visinelli et al. PRL 11, 011802 (2014)

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 12

The Next Open Resonator Experiment

  • Operate at liquid helium temperatures
  • Operate at tesla scale fields
  • Explore new axion-like particle couplings

Support from Heising-Simons Foundation

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 13

Design Change: Loaded Resonators

Strategically placed dielectrics modify resonant mode electric field instead of changing magnetic field direction Conceptually similar to multiple wire planes, but easier to implement with high fields

Shorter wavelength in dielectric Longer wavelength in vacuum

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 14

Loaded Resonators: Implementation

Using dielectric blocks placed periodically in a waveguide placed in a dipole field, TE Modes can couple to dark matter axions

To tune, blocks are moved inside waveguide in a “breathing” motion B

Tuning mechanism prototype

Demonstrated here with waveguide, but we'll still use

  • pen resonators to reach

maximum Q and volume

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 15

Experiment Design

In-house wound 1.5 T superconducting coil fits into cryostat Reflectors Plate/reflector position control rods Alumina plates Magnetic Field Direction Resonant mode electric field profile (estimated shape)

(This is lowered into a LHe cryostat)

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 16

Sensitivity Estimate

Mass Prediction*

*prediction from Visinelli et al. PRL 11, 011802 (2014)

Cryogenic Design Target

We anticipate sensitivity to unexplored axion-like-particle couplings in a theoretically interesting mass range. This is over an order of magnitude better than the best limits so far. Previous Prototype Exclusion

(best limit so far)

A more accurate prediction will be available once RF simulations are complete

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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 17

Next Steps

  • RF Simulation & Engineering to start soon
  • Fabrication early next year
  • Assembly, testing, data taking in 2016
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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 18

Far Future

Current design target Potential Reach With

  • mK temperatures
  • 2+ T fields
  • Qs of 105 or more
  • Larger Volumes
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Workshop on Microwave Cavity Design for Axion Detection - LLNL 2015 - Gray Rybka 19

Conclusions

  • Benchtop open resonator prototype demonstrated

technique is feasibly and powerful

  • Cryogenic experiment being built to explore new

ALP parameters and pave way for larger experiments

  • This is a promising technique: ultimate sensitivity

should be able to probe realistic axions up to 100 of μeV.