quantum micro-mechanics with ultracold atoms€¦ · quantum micro-mechanics with ultracold atoms...
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Quantum micro-mechanics with
ultracold atoms
Dan Stamper-Kurn
UC Berkeley, Physics
Lawrence Berkeley National Laboratory, Materials Sciences
Quantum measurement of a mechanical oscillator
Motivations
Force detection (Caves, Braginski, Milburn, others)
• Apply force resonantly. Measure Z or E.
Basics of quantum metrology: e.g. what detector to use?
• Direct vs. post-amplification
• quadrature specific/non-specific
• destructive vs. non-destructive (QND)
Quantum mechanics of macroscopic bodies.
coszF t
Z
Detection
Some experimental realizations
Nanofabricated cantilevers
Schwab [(Nature 443, 193 (2006)]
also Roukes, Cleland, Wineland
Bouwmeester [(Nature 444, 75 (2006)]
also Aspelmayer/Zeilinger, Rugar, Pinard/Heidman, Harris
Some experimental realizations
Micro-toroidal resonators Ultracold atoms in a cavity
Vahala, Kippenberg
[(PRL 97, 243905 (2006)]this talk
Optical (bosonic) detection
Z
Detection
f Z
/ osc cav in outH H H H f Z nforce per photon:
2 1
2
hf
cL
L
Detection limits:
2
2 1
ph
ZN f
position measurement is photon-shot-noise limited: want more photons
2
2
2
ph
fP N
quantum back-action = radiation pressure fluctuations from shot noise: want fewer
photons
Optical (bosonic) detection
Z
Detection
f Z
/ osc cav in outH H H H f Z nforce per photon:
2 1
2
hf
cL
L
Detection limits:
const. Z P Uncertainty limit for quadrature specific measurement
2
SQL
z
ZM
Uncertainty limit for quadrature non-specific measurement
Micro-mechanical state of the art
Cannot passively cool to ground state
freq. = kHz – MHz < 10 mK = 200 MHz
Cooling by active feedback or by dynamical back-action demonstrated, though not to ground state
closest approach: n = 59 quanta (Schwab, 2006)
requires resolved sidebands:detector bandwidth < oscillator freq.[PRL 99, 093901-2 (2007)]
Measurement sensitivity approaching quantum limit
ΔZ = 6 x SQL (Schwab, 2004)
Back-action observed, but above quantum level
(ΔZ)(ΔP) > 15 x SQL (Schwab, 2006)
Trapped ions
sympathetic cooling
quantum states
prepared and
detected
resolved-sideband
laser cooling
Ultracold atoms in cavity
evaporative cooling
back-action heating
measured at quantum
level
cavity cooling of
single/many atoms
ΔZ = 5 x SQL
MOT
7.5 cm
Cavity mounted
through here
Trap
home of ring-trap
experiments
~200 mStabilized to sub picometer!
Max coupling strength g/2p 16 MHz
Cavity half-linewidth /2p 0.66 MHz
Atomic half-linewidth /2p 3 MHz
Finesse/Q 5.8x105/3x108
Beam waist 23 m
Critical atom number 0.02
Critical photon number 0.02
absorption image
through side of cavity
Cavity loading procedure
200m
Optical lattice
Magnetic trapping outside cavity (TOP trap)
Evaporative cooling
Translation of the magnetic trap to within the cavity mode
Transfer to 1D optical lattice inside cavity + turn off magnetic trap
Result: ~50,000 atoms trapped in ~200 sites of the in-cavity standing wave trap, at T ~ 1 μK (20 kHz)
Note: Following the lead of Vuletic, Chapman, Zimmermann, Hemmerich, Esslinger, Reichel; Walther, Blatt
initial TOP trap
Light-atom interactions in a cavity
0( ) sin( ) pg z g k z
p
c
cavity resonance
probe frequency
light-atom coupling
a
atomic resonance
atomic coherence decay rate
cavity coherence decay rate
Consider dispersive case of large cavity-atom detuning:
2
/
ˆˆ ˆ
i
c atoms in out
atoms ca
g zH n n H H
AC Stark shift per photon per atom Cavity resonance shift per atom
2
N
ca
gN
-100
-50
0
50
100
No
rma
l m
od
e (
GH
z)
-100 -50 0 50 100
Atom-cavity detuning (GHz)
-10
0
10
-10 0 10
Many-atom cavity QED
Normal mode spectrum:
100
99
10099
2
2
2 2
ca cac ca NN g
N = 60,000 atoms
2 2 10MHzg p
5 GHz
60 MHz
Dispersive regime:
Atom = index of refraction
Cavity frequency shift
expand to first order in atomic displacement from trap center
defines collective operators relevant to the cavity probe:
850 nmtrap
780 nmprobe
single photon counter
2
2
0
( )ig z
g 1 1/2 0 1/2 1
†
0 /ˆˆ ˆ ˆ ˆ c N eff z else in outH n N f Zn a a H H
2
/
ˆˆ ˆ
i
c atoms in out
atoms ca
g zH n n H H
1sin(2 ) i i
atomseff
Z k z zN
sin(2 )i i
atoms
P k z p 2sin (2 ) ieff
atoms
N k z
f f
Optomechanical bistability
“Coherent” effect: Optical forces in the cavity will displace the trapped atoms
Probing the cavity shifts the cavity resonance nonlinear cavity optics
0( ) sin( ) pg z g k z
“Cavity nonlinear optics at low photon numbers from collective atomic motion,”PRL 99, 213601 (2007)
probe probe
Transmission spectrum of nonlinear cavity
bare cavity
cavity shift for undriven cavity
probeprobe probe
Cavity t
ransm
issi
on
frequency
0 ca
probe light repels atoms
Nonlinear optics with n<1 photons
Requirements for nonlinear optics at n ≤ 1
medium whose optical properties are altered by single photons
many atoms held in loose trap; displaced by single photon optical force
medium for which this alteration persists longer than photon lifetime
cold atoms with long motional coherence times
11ms 100ns
obs ph
triggered sweep, Δa/2p = -30 GHz
n
- - - -
10
5
075 70 65 60
n
- - - -
0.4
0.2
0.0155 150 145 140
0.2
0.1
0.0-10 -5 0 5 10
probe freq (MHz) probe freq (MHz)
back+forth sweep, Δa/2p = -100 GHz
Optomechanical potential
†
0 /ˆˆ ˆ ˆ ˆ c N eff z else in outH n N f Zn a a H H
Consider force on collective variable: 2
0 Z eff zF N f n Z M Z
“Optical spring”Lorenzian vs. position
some effects:
Optomechanical frequency shift
Optomechanical bistability
Dynamical back-action (non-adiabatic) – heating, cooling, amplification
Bistability and atomic motion
bare cavity
Cavity t
ransm
issi
on
drive frequency
0 ca
2
1
3
45
Spectrum of driven cavity Potential seen by atoms
1
2
34
5
position Z
~ nm
Exciting collective motion from bistable switching
Direct observation of collective atomic motion
wait for cavity to come into resonance
excite collective motion diabatically and observe single-shot detection
(measured, rms) 1.1nm Z ( , rms) 0.22 nm
Z SQLNm
“Incoherent” effect: (quantum) fluctuations of the intracavity intensity cause momentum diffusion / diffusive heating
Atoms serve as “spectators,” i.e. non-destructive detectors, of quantum fluctuations of an intracavity field
Force fluctuations (-> momentum diffusion) represent backaction of position measurement
Quantum optomechanical fluctuations
0 †( )( ) 2 ( ) (0) ( ) (0) ( )
eff SQL
IN z z
N f ZLb b i a b a b
Atom-cavity dynamics and “granularity”
Equations of motion
0
0( ) (0)exp( ) ( )exp ( )
teff SQL
z z
N f Za t a i t i dt n t i t t
Look for small parameters (weak optomechanical coupling):
transient driven by “force history”
bare-cavity responsemodulations (mixing) due to
atomic motion
0
eff SQLN f Z
Generally: a hard problem! Some insights from Ritsch, Vuletic, Rempe, etc.
Granularity parameter
Scaled temperature†
z a a
collective atomic field
cavity optical field
Atom-cavity dynamics and “granularity”
Granularity parameter:
Scaled temperature:
Does a single photon’s kick significantly affect the cavity?
0
0
2
1
eff
eff
z
N fN f
Mline shift from atomic displacement
cavity linewidth
0
1
eff
SQL
N f
Z
(single-photon force) x (residence time of photon)
zero-point momentum spread
Does a single photon’s kick significantly perturb the trapped atom?
atom temperature
cavity-cooling equilibrium temperature
†
z a a
Is cavity cooling/anti-cooling significant compared to diffusive heating
Fluctuation and dissipation
… one obtains a general result
† 2 2 †ˆ ˆ ˆ ˆ nn nn nn
da a S S S a a
dt
with spectral density of photon number fluctuations
( ) ˆ ˆ ˆ ˆ( ) (0) ( ) (0)
zi t
nnS dt e n t n n t n
Diffusive heating + coherent amplification/cooling:
heating by red-detuned noise (promotes oscillator)
amplification/cooling = cavity anti-cooling/cooling (Ritsch, Vuletic, Rempe)
Resolved sidebands:
blue-detuned cavity: cooling to ground state (Zwerger/Kippenberg, Girvin/Harris)
red-detuned cavity: quantum-limited quadrature-non-specific amplifier
Quantum fluctuations of light within a cavity
For our system (non-granular, low temperature):
2 2
1
1 /
freespace
z
DdEC
dt m
Proportional to intensity
Note: At constant intensity, shot noise fluctuations of photon number in a resonant cavity are enhanced w.r.t. those in free space!
spectrum analyzer
monochromatic laser beam
vacuum in all other modes
2
0
2
gC
single-atomcooperativity
Cavity-induced heating: measured by atom loss
1
10Bk T U
( )B
dE dNN U k T
dt dt
wait and see
bare cavity
N
probe
Prepares atoms in well defined initial state
Cavity-induced heating: measured by atom loss
What this means:
Quantum metrology: back-action heating of macroscopic object at level prescribed by quantum measurement limits
Quantum optics: Shot-noise spectrum is enhanced/colored by a cavity
Cavity-light+atom interactions: “theory” looks good
Quantum measurement of atom number or spin: spells trouble for some non-destructive measurements
Micro-mechanics summary
Cavity mode structure selects a single collective mode in a large N gas of atoms.
Evaporative cooling cools this mode to the ground state
Detection: Atomic motion affects cavity properties
Actuation: Cavity light exerts concerted forces on trapped ultracold atoms
Back-action: Probe-light fluctuations cause momentum diffusion
Ahead:
Measurement: optimal method? fundamental limit?
Bistability: Quantum effects? Use as quadrature-specific amplifier?(cf Josephson bistability amplifier)
Amplification/cooling: Observe directly and test theories. Quantum amplifier?
Granular regime: quantum optics. Can we detect a single photon by radiation pressure?
E1: Spinor BECJennie GuzmanSabrina Leslie
Christopher SmallwoodMukund Vengalattore
(James Higbie)(Lorraine Sadler)
E2,E3: Cavity QEDThierry BotterDaniel Brooks
Joseph LowneyZhao-Yuan MaKater MurchTom Purdy
(Kevin Moore)(Subhadeep Gupta)
E4: Ring-trap interferometryJoanne Daniels
Ed MartiRyan Olf
Tony OettlEnrico VogtTiger Wu