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Advanced Resonators for Axion Searches Tia Martineau UMass Dartmouth University of Washington REU 8/29/2017 University of Washington REU Presentation 1
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Page 1: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Advanced Resonators for AxionSearches

Tia MartineauUMass Dartmouth

University of Washington REU

8/29/2017 University of Washington REU Presentation 1

Page 2: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Overview

• What is dark matter?

– The axion

• Resonators as low mass axion haloscopes

• “Pizza Cavity” resonator prototypes

– Model 1

– Model 2

• Future work/Conclusions

8/29/2017 University of Washington REU Presentation 2

Page 3: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

The Axion

• Well-motivated cold dark matter candidate

– Theorized to solve strong CP problem, characteristics match that of CDM candidates

8/29/2017 University of Washington REU Presentation 3

[1]Dark Matter and Background Light - J.M. Overduin & P.S. Wesson

Page 4: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

A bit of cosmology

8/29/2017 University of Washington REU Presentation 4

CDM (cold dark matter) is slow compared to the speed of light

Axions were created abundantly during Big Bang

Low mass axions prevented other decay modes, so the universe would be filled with cold Bose–Einstein condensate of primordial axions. Hence, axions explain the dark matter problem

Page 5: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Overview

• What is dark matter?

– The axion

• Resonators as low mass axion haloscopes

• “Pizza Cavity” resonator prototypes

– Model 1

– Model 2

• Conclusions/Future work

8/29/2017 University of Washington REU Presentation 5

Page 6: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Axion Haloscopes and Resonators

8/29/2017 University of Washington REU Presentation 6

Axions will convert to photons in a strong inhomogeneous magnetic

field B(x)Axion Haloscopes are typically closed microwave resonators

Axions moving through magnetic field will convert when EM resonance in cavity is tuned to frequency of the photons produced. Axions detected as excess power at this frequency

Ben T. McAllister et al., Phys. Rev. Lett. 116, 161804

Page 7: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

ADMX

8/29/2017 University of Washington REU Presentation 7

Field Cancellation Coil

SQUID Amplifier Package

Dilution Refrigerator

Antennas

8 Tesla Solenoid Magnet

Microwave Cavity

Page 8: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Motivation

8/29/2017 University of Washington REU Presentation 8

ADMX Projected Sensitivity up to date Jan 12 2017 source: Gray Rybka

Page 9: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Overview

• What is dark matter?

– The axion

• Resonators as low mass axion haloscopes

• “Pizza Cavity” resonator prototypes

– Model 1

– Model 2

• Future work/Conclusions

8/29/2017 University of Washington REU Presentation 9

Page 10: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Motivation

8/29/2017 University of Washington REU Presentation 10

ADMX Projected Sensitivity up to date Jan 12 2017 source: Gray Rybka

Page 11: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

The use of dielectrics

8/29/2017 University of Washington REU Presentation 11

Allow for higher frequency searches

Can use one tunable cavity instead of multiple smaller cavities

Manipulate waveforms so we can look at other TM modes

Page 12: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

“Pizza Cavity” Simulation

8/29/2017 University of Washington REU Presentation 12

Quasi-TM510 modeFrequency ~9.86 GHzQ-value ~2-3,000

R. Cervantes, cavity simulations, University of Washington (2017)

Page 13: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Potential Tuning Mechanisms

8/29/2017 University of Washington REU Presentation 13

Page 14: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Potential Tuning Mechanisms

8/29/2017 University of Washington REU Presentation 14

Page 15: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Model 1

8/29/2017 University of Washington REU Presentation 15

Page 16: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Model 1

8/29/2017 University of Washington REU Presentation 16

Page 17: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Empty Model 1 cavity reflection result

8/29/2017 University of Washington REU Presentation 17

Page 18: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

A mess

8/29/2017 University of Washington REU Presentation 18

Page 19: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Model 2

8/29/2017 University of Washington REU Presentation 19

Page 20: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Model 2

8/29/2017 University of Washington REU Presentation 20

Page 21: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Model 2 Transmission Data

8/29/2017 University of Washington REU Presentation 21

Page 22: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Model 2 – Tracking Modes

8/29/2017 University of Washington REU Presentation 22

Page 23: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Overview

• What is dark matter?

– The axion

• Resonators as low mass axion haloscopes

• “Pizza Cavity” resonator prototype

– Model 1

– Model 2

• Future work/Conclusions

8/29/2017 University of Washington REU Presentation 23

Page 24: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Future work:

8/29/2017 University of Washington REU Presentation 24

Look into other more complex modes: whispering galleries with

more exotic materials

Focus on cavity optimization, Q value, etc.

Confirm tuning methods are workable

Page 25: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

We still don’t have a catchy name..

PRNCESS - Pizza ResoNant Cavity Experiment using SapphireS

POP TART - PeriOdically-Placed Teflon Axion/Aluminum ResonaTor

DARTH VADER - Dark matter Axion Resonating Tube Haloscope with Vacuum And DiElectric R?

DARK - Dark matter Axion Resonating Kavity??

GRAY (Rybka) - GHz Range Axion cavitY

PENTAGRAM – Periodic rEsoNaTor for Acquiring GHz-Range Axionic Matter

ALAKAZAM - ALuminum Axion Cavity, AZimuthally A Mess

PANDeMiC - Pizza AxioN Dark Matter deteCtor

PARADOX - PizzA Resonator cAvity DetectOr Xperiment

PROTOCOl - Pizza ResOnaTOr Cavity detectOr

DANC Experiment - Dielectric AxioN Cavity Experiment

8/29/2017 University of Washington REU Presentation 25

Page 26: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Conclusions

8/29/2017 University of Washington REU Presentation 26

Dielectrics are beneficial in achieving high-frequencies

Similar R&D projects proven necessary to scan larger areas for axion

Page 27: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Funding provided in part by:

8/29/2017 University of Washington REU Presentation 27

High Energy Physics DE-SC0011665 & DE-SC0010280 & DE-AC52-07NA27344

Page 28: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Special thanks to:

8/29/2017 University of Washington REU Presentation 28

Dr. Gray Rybka, for (putting up with me all summer long and for) being the best mentor a girl could have,

Raphael Cervantes, for being an awesome office mate,

All of ADMX, for providing me an incredibly warm and welcoming environment to be a part of,

Jenny Smith, for being an amazing friend, and

Nick Du, because he asked to be in my acknowledgements.

Page 29: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

8/29/2017 University of Washington REU Presentation 29

Backup Slides

Page 30: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Form Factor (E B)

8/29/2017 University of Washington REU Presentation 30

Will couple to the axion, form factor (E B) is positive

Will NOT couple to the axion, form factor is 0 due to cancellations

G. Carosi – ADMX, UCLA Dark Matter Symposium (2016)

Page 31: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Dielectrics and form factor

8/29/2017 University of Washington REU Presentation 31

Page 32: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Q Factor of Resonators

• The Q factor (quality factor) of a resonator is a measure of the strength of the damping of its oscillations, or for the relative linewidth.

8/29/2017 University of Washington REU Presentation 32

Page 33: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Model 1 (top)

8/29/2017 University of Washington REU Presentation 33

Page 34: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Basic geometric solution for slice size

8/29/2017 University of Washington REU Presentation 34

Page 35: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Method for solving for resonant frequencies

8/29/2017 University of Washington REU Presentation 35

Page 36: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Size comparison

8/29/2017 University of Washington REU Presentation 36

Page 37: Advanced Resonators for Axion Searches · Special thanks to: 8/29/2017 University of Washington REU Presentation 28 Dr. Gray Rybka, for (putting up with me all summer long and for)

Axion Haloscopes (cont’d)

8/29/2017 University of Washington REU Presentation 37

Multiplying the cross section by the axionflux of the Milky Way dark matter halo, one obtains rate of detection

P. Sikivie, Phys. Rev. Lett. 51, 1415 – Published 17 October 1983


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