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![Page 1: The pure Inversion-Tunneling Transition of Ammonia in Helium Droplets Rudi Lehnig and Wolfgang Jäger Department of Chemistry, University of Alberta, Edmonton,](https://reader035.fdocuments.net/reader035/viewer/2022070403/56649f2b5503460f94c4568d/html5/thumbnails/1.jpg)
The pure Inversion-Tunneling Transition The pure Inversion-Tunneling Transition of Ammonia in Helium Dropletsof Ammonia in Helium Droplets
Rudi Lehnig and Wolfgang Jäger
Department of Chemistry, University of Alberta, Edmonton, AB Canada
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• Gas-phase like (that means rotationally resolved) spectra of dopant molecules.
• Increased moment of inertia (dopant drags normal fluid helium density with it).
• Line widths range from 75 MHz to several GHz.
• Microwave spectroscopy may help to understand the line-broadening mechanisms(low-pass filter for droplet excitations).
Helium Nanodroplet SpectroscopyHelium Nanodroplet Spectroscopy
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pure MW spectroscopy:• J = 4 – 3, J = 5 – 4 of HCCCN (10.5 – 14.5 GHz)
Reinhard et al., PRL 82, 5036 (1999). • Callegari et al., JCP 113, 4636 (2000).• J = 1 – 0 of HCN and DCN (58 – 74 GHz)
Conjusteau et al., JCP 113, 4840 (2000).
MW-IR double resonance:• 1 of HCCCN
Callegari et al., JCP 113, 4636 (2000).• 3 of OCS
Grebenev et al., JCP 113, 9060 (2000). Kunze et al., JCP 116, 7473 (2002).
Previous Microwave StudiesPrevious Microwave Studies
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diffusion pump8000 L / min
turbo pump700 L / min
turbo pump700 L / min
turbo pump700 L / min
turbo pump340 L / min
cryostatca. 14 K
skimmer500 μm
doping cell
microwave resonator
quadrupolemass-spec
nozzle5 μm
Helium Nanodroplet SpectrometerHelium Nanodroplet Spectrometer
ℓHe-cooledbolometer, 1.5 K
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radiation
2060 cm-1: 1 photon for 400 helium atoms8 GHz: 18 photons for 1 helium atom
Depletion SpectroscopyDepletion Spectroscopy
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Implementation of Microwave ResonatorImplementation of Microwave ResonatorCavity mirrorsHelium droplet beam
Use of TWT microwave amplifier; output power: 10 Wreflectivity R ~ 0.98; total stored power: ~ 50 * Pin
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Inversion Motion of AmmoniaInversion Motion of Ammonia
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Microwave Inversion Transition of NHMicrowave Inversion Transition of NH33@He@HeNN10
-5 d
eple
tion
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diffusion pump8000 L / min
turbo pump700 L / min
turbo pump700 L / min
turbo pump700 L / min
turbo pump340 L / min
cryostatca. 14 K
skimmer500 μm
doping cell
microwave resonator
quadrupolemass-spec
nozzle5 μm
Helium Nanodroplet SpectrometerHelium Nanodroplet Spectrometer
ℓHe-cooledbolometer, 1.5 K
flag
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Microwave Inversion Transition of NHMicrowave Inversion Transition of NH33@He@HeNN10
-5 d
eple
tion
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single ammonia molecule
sharp feature is saturated
Pick-up Pressure; Saturation BehaviourPick-up Pressure; Saturation Behaviour
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Microwave Inversion Transition of Microwave Inversion Transition of 1515NHNH33@He@HeNN
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Possible Causes for the Sharp PeakPossible Causes for the Sharp Peak
• Effect of Bose-Einstein Condensate fraction?
• Two different relaxation channels?
• Saturation effect, Lamb Dip?
• Maser action of ammonia molecule?
• The overall feature looks like the P-, Q-, R-branches of a vibrational band.
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Energy level splitting through coupling of ammonia rotation with center-of-mass motion of ammonia in the droplet (particle in a box model).
Rotational wavefunction is identical and inversion wavefunction nearly identical Splitting is similar for both states.
Line-Broadening MechanismLine-Broadening Mechanism
K. K. Lehmann, Mol. Phys. 97, 645 (1999).I. Reinhard, C. Callegari, A. Conjusteau, K. K. Lehmann, and G. Scoles, PRL 82, 5036 (1999).K. K. Lehmann, JCP 126, 024108 (2007).
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20.0 20.5 21.0 21.5 22.0 22.5 23.0 23.5Frequency / GHz
m’13121110
98
641
13121110
98
641
m”
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Frequency / MHz
Inte
nsity
Simulated Line-ShapeSimulated Line-Shape
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E = f1 m2 E = h (m+1/2) E = B m(m+1)
Results of SimulationsResults of Simulations
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$$$
AcknowledgementsAcknowledgements
• Chemistry Design and Manufacturing Facility
• Canada Foundation for Innovation• ASRA, ISRIP• NSERC• University of Alberta