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mg Molecular collisions in the (ultra-)cold Matthias W Gempel RTG - Goslar 3013-02-11

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Page 1: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

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Molecular collisions in the (ultra-)cold

Matthias W Gempel

RTG - Goslar 3013-02-11

Page 2: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

Molecules

Vdd=d2

R31−3cos2𝜃

long-range anisotropic

+ can tune (effective) interactions

+ can handle them (might not be easy)

Page 3: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

To give you an idea…

AB (n) + AB (m) AB (p=n) + AB (q=m)

AB (n) + AB (m) AB (p≠n) + AB (q≠m)

AB (n) + AB (m) A2 (p) + B2 (q)

AB (n) + AB (m) A2B + B

AB + A …

or…

etc.

or…

What happens in a trap filled with molecules?

elastic

inelastic

chemical

Page 4: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

Theory v.s. Experiment

Theory Experiment

T→0 T≈1

Some single quantum state

Some quantum states

Page 5: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

What makes Experiment so difficult ?

… vastly different energy scales.

and same reason why theory is difficult…

room: 300 K

0.1 μK

chemical: 1000 K

vibration: 100 K

rotation: 0.1 K

resonance spacings: 1 nK

no direct (laser)cooling to uc

Page 6: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

Theory

Chem Rev 112,4949 (2012)

long-range

r

p r’

• Coupled channel • Internal vibrational relaxation • Unimolecular dissociation • Statistical

• Coupled channel • Quantum defect theory • Quantum Langevin • Born

Page 7: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

Theory: ‚Simple‘ model of elastic collisions

NJP 11,055039

−ℏ2

2𝜇Δ + 𝑑1𝑑2

1−3cos2𝜃

𝑅3 + 𝑉𝑠𝑟 Ψ = 𝐸 Ψ

aligned dipoles short range: hard core (interested in long range → ‘ignore’ it)

Natural scales:

𝑎𝑑𝑑 =𝜇𝑑1𝑑2

ℏ2

𝑈𝑑𝑑 = ℏ6

𝜇3𝑑12𝑑2

2 𝐸

12

𝐸0

Page 8: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

Theory: ‚Simple‘ model of elastic collisions

NJP 11,055039

s-wave scattering

phase shifts at short range potential average out over multiple partial waves

𝜎𝑒𝑣𝑒𝑛 = 1.117 𝑎𝑑𝑑2 + 4𝜋𝑎2

𝜎𝑜𝑑𝑑 = 3.351 𝑎𝑑𝑑2

𝜎𝑒𝑖𝑘 = 8𝜋3 𝑎𝑑𝑑

𝜇

2𝐸

Page 9: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

Theory: Statistical approach

PRA 87,012709

𝑅 < 𝑅0 : is hard →

look for sth. ‚simple‘

many (dense) scattering resonances

mean decay width: Γ𝑅𝑅𝐾𝑀 =𝑁𝑜

2𝜋𝜚

average obervables

𝑎 𝑖

Random Matrix Theory Multichannel

Quantum Defect Theory

Page 10: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

Theory: Statistical approach

PRA 87,012709

𝐽 = 𝐿𝑖𝑛 𝐽 = 𝐿 + 𝑁1 + 𝑁2

many (dense) scattering resonances: rotational – vibrational - chemical

𝑁𝑂 = 1 𝜚 ≫ 1

𝑁𝑂 > 1 𝜚 ≫ 1

RbCs

KRb

long complex lifetimes:

broad resonances

𝜏~102ms

Compute short range K-Matrix match MQDT at R0

compute scattering matrix

Page 11: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

Theory: Statistical approach

PRA 87,012709

RbCs:

Page 12: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

The group

Thanks!

Prof. Silke Ospelkaus

Torben Schulze

Matthias Gempel

Torsten Hartmann

Maurice Petzold

Janis Wöhler Dr. Alessandro Zenesini

Page 13: Molecular collisions in the (ultra-)cold€¦ · Theory: ‚Simple‘ model of elastic collisions NJP 11,055039 s-wave scattering phase shifts at short range potential average out

Theory: Statistical approach

PRA 87,012709

KRb: