Ultracold molecules - Vrije Universiteit...
Transcript of Ultracold molecules - Vrije Universiteit...
Ultracold Molecules
Introductory course onUltracold quantum gases
July 10-12, Innsbruck
Steven Knoop
Why ultracold molecules ?• Ultracold chemistry
– Control with external fields
• High resolution spectroscopy– Example: time variation me/mp
• Molecular BEC– “Superchemistry”– Dipolar quantum gases
• Quantum processing
F+H2(ν=0,j=0)->HF(ν’)+H
1 mK 1 K
s
p
Atoms: simple level structure
S1/2
2P1/2
2P3/2
Atoms: simple level structure
S1/2
2P1/2
2P3/2
Closed opticaltransitionmakes lasercooling work !
alkali, earth-alkali,metastable noble gases,few exotic species
Atoms: simple level structure
From atoms to molecules
rU(r)
+ rot. structure+ hyperfine structure
many vib.levels
many vib.levels
rU(r)
many decay channels:laser cooling fails
From atoms to molecules
slowing and cooling of molecules
Buffer gas coolingJ. Doyle et al.
molecules withlarge magnetic dipole moment
Stark decelerationG. Meijer et al.
polar molecules
slowing and cooling of molecules
Buffer gas coolingJ. Doyle et al.
molecules withlarge magnetic dipole moment
Stark decelerationG. Meijer et al.
polar molecules
mK…K
Starting from ultracold atoms:
free atoms
laser 1
laser 2
s+s
s+p
controlled photo-associationtwo-color
photo-associationone-color
laser
s+s
s+p
low molecule numbers, low densities
photo-association
molecules @ few nKmolecular quantum gas
atomic quantum gas
Herbig et al., Science 301, 1510 (2003)
Feshbach molecules
Starting from ultracold atoms:Feshbach association
Ultracold Feshbach molecules
• Ultracold atomic gases • Feshbach resonances
• Very basic two-body physics, molecular structure• Feshbach resonance (molecular view)• Feshbach association• Properties of Feshbach molecules• Fermion composed Feshbach molecules• Towards ultracold ground-state molecules NEW
Two-body potential
r
U(r)incident or scattering channel
r
Attractive potential: van der Waals force ~ -1/r6
Repulsive potential: Coulomb force
some molecular physics
Vibrational states
Rotational states
1+11+22+2
Hyperfine states
~ 100 THz
~ 3300 cm-1 (wavenumbers) / ~ 0.4 eV
1+11+22+2
~ 1 GHz
Zeeman effect
F=2
F=1
Magnetic field
Energy
Hyperfine splitting
mF
2
1
0
-1
-2
-1
0
1
7Li, 23Na, 39K, 41K, 87Rb
(2,1)+(2,1)
mF210-1
-2
-10
1(1,1)+(1,1)
B
E
B
E
(magnetically induced)Feshbach resonance
Feshbach resonance
F=2
F=1
Feshbach resonance
two atoms
B
E
molecule
binding energy
Feshbach resonance: a closer look
avoided crossing
scat
terin
g le
ngth
B0
entrance doors into the ultracold molecular world
Adiabatic magnetic field ramp
two atoms
B
E
molecule
• Imaging: fast magnetic field backramp
• Separation: e.g. magnetic field gradient
dissociation
Adiabatic magnetic field ramp
two atoms
B
E
molecule
• Imaging: fast magnetic field backramp
• Separation: e.g. magnetic field gradient
Purification
B
E
• resonant laser light / microwave pulse
making Feshbach molecules from BECs
CsCs22
Innsbruck, Science 301, 1510 (2003)
NaNa22
MIT, PRL 91, 210402 (2003)
MPQ, PRL 92, 020406 (2004)
8787RbRb22
Properties Feshbach molecules
• single rovibrational quantum state
- highly excited vibrational state (ν=-1)
- rotationally cold s-wave (ℓ=0) even ℓ (BB)odd ℓ (FF)all ℓ (BB’,BF,FF’)
• weakly bound (kHz-MHz-GHz)
Properties Feshbach molecules• atom-molecule, molecule-molecule collisions
relaxation to lower vibrational states
Properties Feshbach molecules
MIT, PRL 92, 180402 (2003)
• atom-molecule, molecule-molecule collisions
relaxation to lower vibrational states
atom-molecule
molecule-molecule
Adiabatic magnetic field ramp
two atoms
B
E
molecule
Properties Feshbach molecules
MIT, PRL 92, 180402 (2003)
• atom-molecule, molecule-molecule collisions
relaxation to lower vibrational stateslimited lifetime
atom-molecule
molecule-molecule
Properties Feshbach molecules
MIT, PRL 92, 180402 (2003)
• atom-molecule, molecule-molecule collisions
relaxation to lower vibrational stateslimited lifetime
optical lattice
(one molecule per lattice site)
atom-molecule
molecule-molecule
E/(∆µ∆B)
a/a bg
(B-B0)/∆B
∆B
Εb
Scattering length
Binding energy
Properties Feshbach molecules
a/2Quantum halo state
66LiLi22
Halo dimers out of fermions• Pauli blocking
• atom-dimer and dimer-dimer relaxation suppressed for large a
trap depth
• forming Feshbach molecules by three-body recombination
molecular BEC gallery (2003-2004)
MIT, Ketterle et al.66LiLi22
ENS Paris, Salomon et al.
66LiLi22
Rice, Hulet et al.
66LiLi22
Innsbruck, Grimm et al.
66LiLi22
JILA, Jin et al.4040KK22
Overview Feshbach molecules
23Na2 (s-wave)
85Rb2 (s-wave)
87Rb2 (s-, d-wave)
133Cs2 (s-, d-, g-, l-wave)
85Rb87Rb (s-wave)
6Li2 (s-wave)40K2 (s-wave)
6Li2 (p-wave)40K2 (p-wave)
Fuchs et al, PRA 2008
Gaebler et al, PRL 2007
Thompson et al, PRL 2005
Dürr et al, PRL 2004Volz et al, PRA 2005
Xu et al, PRL 2003
Herbig et al, Science 2003Mark et al, PRA 2007
Regal et al, Nature 2003
Strecker et al, PRL 2003Jochim et al, PRL 2003Cubizolles et al, PRL 2003Zwierlein et al, PRL 2003
Ospelkaus et al, PRL 2006Papp & Wieman, PRL 2006
hom
onuc
lear
hete
ronu
clea
r
bosons fermions
40K87Rb (s-wave)
boson+boson boson+fermion fermion+fermion
6Li40K 7Li87Rb 6Li87Rb
In the (near) future ?
6Li23Na 87Rb133Cs41K87Rb39K87Rb
52Cr2
Recent development
Recipe
make Feshbach moleculescoherent two-photon transfer
(STIRAP)
S+P
Towards ultracold dense gas of ground-state molecules
r
S+S
X1Σg+: singlet
a3Σu-: triplet
~ 100 THz
~10 THz
ν=0, J=0
ν=-1
ν=-2
Innsbruck, Cs2, ν=155 -> ν=73 (32 THz) Danzl et al, Science (published online: 10 July 2008)
ν=155
ν=73
JILA, KRb, ν=-1 -> ν=-3 (10 GHz)Ospelkaus et al, Nature Physics (published online: 22 June 2008)
Heteronuclear molecules: towards dipolar quantum gas !
Innsbruck, Rb2, ν=-1 -> ν=-2 (0.6 GHz)Winkler et al, PRL 98, 043201 (2007)
Quantum gas of chemically bound molecules !
ν=-1
ν=-2
Innsbruck, Cs2, ν=155 -> ν=73 (32 THz) Danzl et al, Science (published online: 10 July 2008)
ν=155
ν=73
JILA, KRb, ν=-1 -> ν=-3 (10 GHz)Ospelkaus et al, Nature Physics (published online: 22 June 2008)
Heteronuclear molecules: towards dipolar quantum gas !
Innsbruck, Rb2, ν=-1 -> ν=-2 (0.6 GHz)Winkler et al, PRL 98, 043201 (2007)
triplet ν=0 ground state(6 THz)
STAY TUNED !!!triplet ν=0 ground state
(7 THz)
Quantum gas of chemically bound molecules !