strongly-correlated fermions in optical lattices - apparatus · 2020. 7. 15. · pc pid setpoint pd...

Post on 19-Jan-2021

5 Views

Category:

Documents

0 Downloads

Preview:

Click to see full reader

TRANSCRIPT

Apparatus and sequence overview

Interferometer setup for superlattice

Ultracold 40K and 87Rb Optical lattice with tuneable geometry

Team members 2001-2016

AOM

+ c,X+ ref

Coherent Mephisto MOPA 36 NE

Nd:YAG 1064 nm

optical isolator

beam dump

thin filmpolarizer

AOM AOM AOM

+ c,Z + c,X

double AR plate

interference phase PD

AOM

+ c,Y

30:70 plate

mirror

50:50 plate

fiberx axis

fiber y axis

fiber z axis

/2 plate

x and y axis

/4

lattice y

imaging x imaging y

achromatf=400 mm

f=400 mm

Gradiumf=100 mm

f=100 mm

intensity Y

intensity

intensity

anamorphicprism pair

fiberoutcoupler

lattice x

deconf. x

intensityX and X

x

yz

XYX

f=400 mm

FORT x

f=400 mm

f=400 mm

f=400 mm

CC

D

CCD

cleaning plate

RF source p,XPhaseTag X

RF source c,XCarrier X

RF source r,XReference X

AOM driver

AOM X

RF source p,YPhaseTag Y

RF source c,YCarrier Y

RF source r,YReference Y

>> +90dB

FM in

Y monitor DC

Y monitor RF

feedback signal

AOM driver

AOM Y

<< +30dB

c,Y

c,Y

p,Y

p,Y

PC

<< +30dB

>> +90dB

FM in

X monitor DC

X monitor RF

RF source mixMixing down

feed

back

si

gnal

GPS 10 MHz

c,X

c,X

p,X

p,X

PD

Phase stabilization X Phase stabilization Y

PC

delayline

Lase

r In

tens

ity

fixed intensityvariable intensity

Laser frequency

c,X

p,X

p,X

c,Y

p,Y

p,Y

beat X

beat Y

ref

a bX beam

Y beam110 112 114 116 118

PD beat frequency (MHz)

-90-80-70-60-50-40-30-20-10

0

sign

alpow

er(d

Bm

)

beat X

beat Y

RF source i,XIntensityTag X

RF source c,XCarrier X

AOM driver

AOM X

AM in

0 1 2 3 4 5

beat frequency (MHz)

-80

-60

-40

-20

0

20

sign

alpow

er(d

Bm

)

<< +30dB

DC

PIDPCsetpoint

PD>>

a b

beat X intensitybeat X intensity

Intensity stabilisation

Beat notes on photodiodePhase lock: RF electronicsSuperlattice: optical setup on laser table Optical setup on experiment table

(old naming convention)

(old naming convention)

Experiment Theory

~ 0

~ /2

1.20

1.05

0.90

0.75

0.60

0.45

0.30

0.15

0.00

Density (a.u.)

2 k�

Superlattice phase calibration

Raman-Nath/Kapitza-Dirac diffraction on 87Rb BEC

Bx

x y

MOT QUIC FORT

Sympathetic cooling of 40K with 87Rb in QUIC

0 9 19 23time (s)

40K

N 4 106

N 1 109

N 2 106

N=0

87Rb

2 mm

Magnetic coils setup

3

Cloud position

Quadrupole coils

Ioffe

coi

l

Gra

dien

t coi

l

Transportcoils

Glasscell

Scale 1:2

4

18

52.5 59.5

4.1

x

z

y

Fesh

bach

coi

ls

0 50 100 150Position x (px)

0.0

0.5

1.0

OD

(a.u

.)

0.0 0.5 1.0OD (a.u.)

0

50

100

150

Posi

tion

z(p

x)

100 m

xz

400k 40K

0.078 T/TF

21 nK

6.5 6.6 6.7 6.8rf endpoint (MHz)

1.0

1.2

1.4

1.6

1.8

2.0N

K(1

06)

0

1

2

3

NRb

(106

)6.5 6.6 6.7 6.8

rf endpoint (MHz)

0.3

0.4

0.5

T K(T

F)

100

150

200

250

T Rb

(nK)

(a) (b)

Degenerate Fermi gas

Magnetic gradient for K-Rb mixture in FORT

(Quadrupole-Ioffe configuration) (Far-offresonant trap = dipole trap)

θ =

ϕ =

x

z

x

z

x

z

X

ZX

Cubic Hexagonal

Checkerboard Dimers

a

b

c

xy

z

BA

BA

Optical lattice: 1D bandstructure

-1 0 10

5

10

15

-1 0 1 -1 0 1 -1 0 1Quasimomentum q/klat

Ener

gy/E

rec

V0 = 0Erec 2 Erec 20 Erec6 Erec

kx

ky

x

y

Brillouin zone kL=4unit cell

kLA Ba

a1

2D unit cell and Brillouin zone

Potential symmetry phase

superlattice phase

Thilo Stöferle, Henning Moritz, Michael Köhl, Christian Schori, Kenneth Günter, Niels Strohmaier, Robert Jördens, Leticia Tarruell, Daniel Greif, Thomas Uehlinger, Gregor Jotzu, Michael Messer, Rémi Desbuquois, Frederik Görg

Rb source

Differential pumping tube

K source

Ion pump

Titanium sublimationpump

MOTchamber

Glass cell20 cm

Mag

netic

tran

spor

t

Mag

neto

-opt

ical

trap

(MO

T)

Mic

rowa

ve e

vapo

ratio

nin

mag

netic

trap

(QU

IC)

Stat

e pr

epar

atio

n

Imag

ing

Read

out

Opt

ical

latti

ce e

xper

imen

t

Coo

ling

in d

ipol

e tra

pPr

epar

atio

n of

spi

n m

ixtu

re

Opt

ical

mol

asse

sO

ptic

al p

umpi

ng

time (s)

0 20 3010 40 50

Ion pump

MOT chamber Glass cell

x

z

y

Lattice team: Kilian Sandholzer, Joaquín Minguzzi, Anne-Sophie Walter, Konrad Viebahn, and Tilman EsslingerInstitute for Quantum Electronics, ETH Zurich

Strongly-correlated fermions in optical lattices - apparatus

top related