www.tugraz.at w i s s e n t e c h n i k l e i d e n s c h a f t 17. januar 13 name und oe, eingabe...
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W I S S E N T E C H N I K L E I D E N S C H A F T
u www.tugraz.at
17. Januar 13
Name und OE, Eingabe über > Kopf- und Fußzeile
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Thursday, 2014-06-19Florian Lackner
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Helium droplet assisted preparation of…
Molecules[1,2,3]
0.1 nm 1 nm 10 nm 100 nm
Clusters Nanowires
[1]…Science 273, 629-631 (1996)[2]…Phys. Rev. Lett. 100, 063001, (2008) [3]…J. Phys. Chem. A 117, 13719 (2013)
Volk et al. J. Phys. Chem. 138, 214312 (2013)
Thaler et al., submitted manuscript (2014)
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RbSr molecules
X2Σ+ ground state: electric and magnetic dipole moment
Thursday, 2014-06-19Florian Lackner
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interesting for ultracold molecular physics[8]
RbSr has not been characterized experimentally…
… but extensively by theory because of increasing interest in RbSr [9,10,11,12,13]
[9]…Ẑuchowski et al. arXiv:1402.0702 (2014)[10]…Phys. Rev. Lett. 105, 153201 (2010)
[11]…Phys. Rev. A 88, 023601 (2013)[12]…Phys. Rev. A 82, 042508 (2010)[13]…Lackner et al. submitted manuscript (2014)
[8]…Phys. Rev. A 88, 023601 (2013)
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Production of RbSr Molecules on HeN
Thursday, 2014-06-19Florian Lackner
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HeN
Pickup
Rb Sr
Source conditions: 15 K / 60 bard ~ 8 nm
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Spectroscopic Methods
Thursday, 2014-06-19Florian Lackner
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Resonant two-photon ionization (R2PI) spectroscopy
Laser induced fluorescence (LIF) spectroscopy
Dispersed fluorescence (DF) spectroscopy
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Thursday, 2014-06-19Florian Lackner
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RbSr on HeNTime-of-flight mass spectra
Monomers Dimers and RbSr
mass [amu]mass [amu]
ion
sig
na
l [a
rb.
u.]
ion
sig
na
l [a
rb.
u.]
Krois et al. in preparation
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RbSr Potential Energy CurvesMRCI calculations
Thursday, 2014-06-19Florian Lackner
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For details see: talk FC07Friday 10:07 AMJohann Pototschnig
X2Σ+
RbSr-HeN:only X2Σ+ (ν" = 0) is populated (0.37 K)
Lackner et al. submitted manuscript (2014)
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RbSr-HeN Excitation SpectrumTheory vs. experiment
Thursday, 2014-06-19Florian Lackner
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R2PI spectroscopy
Lackner et al. submitted manuscript (2014)
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42Σ+ state: Te = 14006(4) cm-1
ωe = 86(3) cm-1 ωexe = 1.2(0.7) cm-1
42Σ+←X2Σ+ Transition Vibrationally resolved
Thursday, 2014-06-19Florian Lackner
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R2PI
LIF
Information onfree RbSr molecules
Insight intoRbSr-HeN
Krois et al. in preparation
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…desorb from the droplet upon laser excitation (42Σ+←X2Σ+ )
Thursday, 2014-06-19Florian Lackner
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RbSr molecules…
Access to free RbSr molecules
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Dispersed Fluorescence SpectraFree 42Σ+ RbSr molecules
Thursday, 2014-06-19Florian Lackner
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X2Σ+ ground state: ωe ~ 42 cm-1 Theory[9,10]: 38-42 cm-1
[9]…Ẑuchowski et al. arXiv:1402.0702 (2014)[10]…Lackner et al. submitted manuscript (2014)
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Thursday, 2014-06-19Florian Lackner
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Dispersed Fluorescence SpectraFree RbSr molecules
relaxation
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Thursday, 2014-06-19Florian Lackner
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Dispersed Fluorescence SpectraFree RbSr molecules
shifted by-90 cm-1
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What’s coming next ?
Thursday, 2014-06-19Florian Lackner
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RbCa
Ca2
Helium droplet assisted “molecular engineering”
R2PI
LIF
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SummaryRecipe for the investigation of RbSr
Helium droplet assisted preparation of RbSr molecules
Covering large spectral ranges (11600 – 23000 cm-1) with R2PI spectroscopy
Preparing free RbSr molecules – DF spectroscopy
New perspectives for the formation of tailored molecules and ultracold molecular physics
Thursday, 2014-06-19Florian Lackner
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Thank you !
Thursday, 2014-06-19Florian Lackner
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Günter Krois
Johann V. Pototschnig
Wolfgang E. Ernst
Thomas Buchsteiner
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Thursday, 2014-06-19Florian Lackner
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LIF vs. R2PI and Fragmentation
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4²Σ+ Fit and Sr2 background correction
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Dispersed Fluorescence Spectroscopy – Sr2
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(3)2Π1/2,3/2←(1)2Σ+ Transition
SO splitting ~13.5 cm-1
resolved on the droplet!
Broadened, asymmetric peaks due to the simultaneous excitation of the molecule and vibrations of the droplet (phonons)
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Isotope-shift: (3)2Π1/2,3/2←(1)2Σ+ Transition
Isotope-shift
Free molecule[4]
8.2 cm-1
17.4 cm-1
28.2 cm-1
[4] Russon et al., J. Chem. Phys., 138, 194307 (2013)
9 cm-1
18 cm-1 31 cm-1
LiCa on HeN
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