Laser cooling of C2- for ultra cold antiproton · 2019. 8. 7. · Laser cooling of C2 −for ultra...

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Laser cooling of C 2 for ultra cold antiprotons Narita Kanako Supervisor: Michael Doser 1

Transcript of Laser cooling of C2- for ultra cold antiproton · 2019. 8. 7. · Laser cooling of C2 −for ultra...

  • Laser cooling of C2− for

    ultra cold antiprotons

    Narita Kanako

    Supervisor: Michael Doser

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  • About me

    • At HomeMaster in Particle Physics

    Searching for hidden photons at

    The University of Tokyo

    • At CERNLock-in measurement for photo-electrons from anion molecules

    AEGIS,ES-SME

    My working place

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  • What is AEGIS experiment?

    • Goal: Study gravitational interaction of antimatter with matter, searching for violations of CPT theorem and weak equivalence principle

    •Antihydrogen production via resonant charge exchange

    Antihydrogen production:

    →Requires ultracold antiprotons

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  • How to cool antiprotons

    • Idea: Sympathetic cooling of ҧ𝑝 by laser cooling of anions

    • Use of C2− anions because of well known level scheme

    • Laser cooling of C2− in Penning trap cools ҧ𝑝 to 𝑻 ҧ𝒑 ≈100 mk

    • C2− has to be in the ground state for cooling

    I am studyingtrapping and cooling C2

    Experimental equipment for cooling

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  • What am I actually doing at AEGIS?

    My study:To make a program to check if there was a signal on the MCP cameraPurpose:To know that the laser was on the resonance with the C2

    photodetachment transitionTo verify whether C2

    − is in the ground state

    Trapping C2− 3MHz

    @ 120 V

    C2− flying to the trap

    Photo electronkicked out radially from the trap to the detectorMCP camera

    Detector/MCP camera

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  • What am I actually doing at AEGIS?

    Time [us] Time [us]

    Function generator’s signal MCP’s signal

    The trap radio frequency is driven by the function generator.When the function generator signal goes from 0 to 1, a recording is triggered, where the time is noted and the corresponding MCP signal in the same time is recorded for a period of 100ns.This MCP data is just the background data, without any lasers or C2

    −. The final MCP data will be recorded later.

    Voltage[V] Voltage[V]

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  • Result

    0.001547

    0.006187

    0.000885

    0.002431

    -0.001325

    0.003093

    0.00243

    -0.001325

    0.0030940.00265

    -0.002

    -0.001

    0

    0.001

    0.002

    0.003

    0.004

    0.005

    0.006

    0.007

    1 2 3 4 5 6 7 8 9 10

    The average value of background dataVoltage[V]

    Event number

    We picked up the MCP back ground signals corresponding to signals going up in function generator. The final MCP data will be recorded later. 7

  • Summary

    • We did Lock-in measurement for photo-electrons from anion molecules.

    • I made a program to select signals according to photo-electron signals.

    • The final MCP data will be recorded later.

    • I thank Drs. Michael Doser, Sebastian Gerber, Christian Zimmer and Emanuel Oswald for their support.

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  • Thank you for your attention. Questions?

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  • Back up

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  • What is AEGIS experiment?

    Studies:

    Gravitational Acceleration of Antihydrogen

    How it works:

    Observes the pattern produced by parallel beams of excited low-energy antihydrogen atoms as they pass through 3 gratings

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  • Why is the amplitude of function generatorlower ?

    • Shortly before the rf cable reaches the trap, the signal that goes to the oscilloscope is capacitive coupled out (using a 5nF capacity on the signal cable). So the measured rf signal on the oscilloscope has only ~5V peak to peak, but it follows the V_amp shape.

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