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A Universal Atomic and Molecular Detector for Atom Interferometry Maxwell Gregoire Cronin Lab University of Arizona

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Page 1: grad talk presentation 2

A Universal Atomic and Molecular Detector for Atom Interferometry

Maxwell Gregoire

Cronin LabUniversity of Arizona

Page 2: grad talk presentation 2

Polarizability

E

d

p = Qd = α E

p: dipole moment Q: electron charged: displacement

E: electric field

valence electron cloud

nucleus

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DiffractionP

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Mach-Zehnder Atom InterferometerP

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Mach-Zehnder Atom Interferometer

P

bars blocktransmission

P

bars allowtransmission

P

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Mach-Zehnder Atom Interferometer

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Mach-Zehnder Atom Interferometer

-

+

● Creates phase shift in atom waves:

Φ proportional to α

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The Problem: Current Detector

Langmuir-Taylor “hot wire” detector● Thermal/surface ionization: atoms

contacting a filament ionize as they boil off

● Efficient only if atom's ionization potential is comparable to filament's work function

atoms ionsDiscriminator

&Pulse

Counter

filament

CEM

ptable.com

ptable.com

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The Solution: Universal Detector

● We want to be able to detect atoms from the entire periodic table

● We want to be able to detect molecules

ptable.com

Page 10: grad talk presentation 2

Motivations: Test Atomic Theory

● Test atomic theory:

polarizability, van der Waals coeff's, state lifetime, branching ratio, and index of refraction calculations

all rely on knowing the

atomic dipole transition matrix elements

● Measuring one of those things tests the theory

ptable.com

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Motivations: Parity Non-Conservation

● PNC research tests for beyond-the-standard-model physics

● Observing the rate of parity-violating transitions requires knowing the atomic dipole transition matrix elements

ptable.com

Page 12: grad talk presentation 2

Motivations: Atomic Clocks

● Atomic clocks use trapped atoms to keep time● Limitation on accuracy is due to lack of knowledge

of blackbody radiation shift, which depends on polarizability

ptable.com

Page 13: grad talk presentation 2

Electron Impact Ionization Detector

IonizationRegionatoms ions

MassFilter filtered

ions

Discriminator&

PulseCounter

CEM

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Electron Impact Ionization Detector

IonizationRegionatoms

MassFilter filtered

ions

Discriminator&

PulseCounter

SRS RGA 200 contains

● Quadrupole Mass Analyzer

● Channel Electron Multiplier

CEM

Build our own Discriminator

● AMPTEK A111, variable level

Use LabJack as pulse counter

ions

http://www.thomasnet.com/articles/instruments-controls/analyzers-residual-gas

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Electron Impact Ionization Detector

IonizationRegionatoms

MassFilter filtered

ions

Discriminator&

PulseCounter

Design considerations:

● Ionization cross section

● Phase-space density

● Phase-space density limit/ beam divergence

● Filament heat/resulting noise

CEM

ions

Farland, Kinney, Phys. Rev. 137, A1058 (1964)

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Electron Impact Ionization Detector

IonizationRegionatoms

MassFilter filtered

ions

Discriminator&

PulseCounter

CEM

atom beam being ionized

electron beam

Ideas:

● 1) shaped beam ● 2) almost-tangential beam(s)

ions

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Electron Impact Ionization Detector

IonizationRegionatoms

MassFilter filtered

ions

Discriminator&

PulseCounter

CEM

Ideas:

● 3) pinching magnet along with beam or filament source

ions

DeKieviet et al, Rev. Sci. Instrum. 71, 2015 (2000)

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Acknowledgements

People

● Professor Alex Cronin

● PhD students: Will Holmgren (~2013) Ivan Hromada (~2014) Raisa Trubko (~2015), Me (~2016), You (?)

● Undergraduates: Adam deBolt (2013), James Greenberg (2014)

Organizations

● University of Arizona Dept. of Physics

● National Science Foundation

● National Institute of Standards and Technology

Questions?