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14
 Laser Cooling of a Nanomechanical Oscillator Jasper Chan et. al. Presented by: Clinton Potts

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  • Laser Cooling of a Nanomechanical

    Oscillator Jasper Chan et. al.

    Presented by: Clinton Potts

  • Overview

    Experimental Motivation

    Optomechanics

    Sideband Cooling

    Nanomechanical Oscillator

    Measurement Technique

    Results

    Future Work 2

  • Experimental Motivation

    Observe quantum mechanical behavior in a mesoscopic system

    Mesoscopic Billions of atoms

    Similar work performed using cryogenic cooling techniques

    25

    Solely cryogenic cooling not realizable for many devices

    ~ OConnell, Nature 464, 697-703 (2010)

    3

  • Optomechanics

    Crookes radiometer

    Photons carry momentum

    Radiation Pressure

    High finesse cavities increase momentum transfer

    Optical field couples to the mechanical motion

    Markus Aspelmeyer, Cavity Optomechanics (2013)

    www.envirogadget.com

    4

  • Optical Resonator

    High population of photons at resonant frequency Population quickly drops off

    Optical decay rate - Related to Finesse

    Markus Aspelmeyer, Cavity Optomechanics (2013)

    5

  • Optomechanical Resonator

    Optical Cavity consists two mirrors

    Fixed Mirror

    Movable mirror attached to Spring

    Movable mirror act as simple harmonic oscillator

    Motion described by phonons

    6

  • Sideband Cooling

    Non-Sideband Resolved

    >

    Sideband Resolved

    <

    7 Markus Aspelmeyer, Cavity Optomechanics (2013)

    =

  • Phonon-Photon Interactions

    Three processes possible

    Photon Absorption (Grey)

    Phonon Creation (Red, Stokes)

    Phonon Annihilation (Blue, Anti-Stokes)

    Markus Aspelmeyer, Cavity Optomechanics (2013)

    8

  • Ground State Cooling

    9

    To maximize Anti-Stokes scattering

    = High Density of States within cavity

    Low Density of States outside cavity

    =

    Markus Aspelmeyer, Cavity Optomechanics (2013)

  • Nano-Mechanical Device

    Silicon Nanobeam

    Device pre-cooled to 20K

    Laser coupled via tapered fiber

    10

  • Measurement and Results

    =

    (()2+(

    2 )2)

    Average number of phonons

    Total mechanical damping rate

    Measured from transmitted drive laser

    Phonon number determined via curve fitting

    11

  • Measurement and Results

    = . .

    Average number of Phonons

    Cooling limited by increased bath temperature

    Due to high intensity field

    12

  • Going Forward

    Not a true quantum mechanical measurement Classical measurement of quantum system

    Measured average number of phonons Detection of discrete phonon values more direct proof of quantum mechanics

    Markus Aspelmeyer, Cavity Optomechanics (2013)

    13

  • Questions

    14