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Experimental studies of decays at long timescales Patrick Rousseau patrick.rousseau@unicaen.fr EMIE-UP summer school patrick.rousseau@unicaen.fr 1 Multiscale Dynamics in Molecular Systems Introduction Instru strume ment ntatio ion


  1. Experimental studies of decays at long timescales Patrick Rousseau patrick.rousseau@unicaen.fr EMIE-UP summer school patrick.rousseau@unicaen.fr 1 “Multiscale Dynamics in Molecular Systems”

  2. Introduction Instru strume ment ntatio ion Me Metastable d disso sociation on Radi diati tive c coo ooling Vibrati tiona nal e electr ctron d detachm chment Slow iso isome merisa sati tion EMIE-UP summer school patrick.rousseau@unicaen.fr 2 “Multiscale Dynamics in Molecular Systems”

  3. Complex systems They posses a large number of degrees of freedom: →! numerous relaxation channels are expected ● in competition ● at difgerent timescales EMIE-UP summer school patrick.rousseau@unicaen.fr 3 “Multiscale Dynamics in Molecular Systems”

  4. Jablonski diagram EMIE-UP summer school patrick.rousseau@unicaen.fr 4 “Multiscale Dynamics in Molecular Systems”

  5. Complex systems They posses a large number of degree of freedom: →! numerous relaxation channels are expected ● in competition ● at difgerent timescales Today we will focus on really long timescales (higher than ns). 10 -15 s 10 -12 s 10 -9 s 10 -6 s 10 -3 s 1 s 10 3 s EMIE-UP summer school patrick.rousseau@unicaen.fr 5 “Multiscale Dynamics in Molecular Systems”

  6. Long timescale At such long timescale, the system can be described by statistical physics. From the experimental point of view, we need to keep the control on the system BUT in 1 µs, a thermal water molecule runs through about 1 mm. One need to store the molecular system in order to study longer timescales. 10 -15 s 10 -12 s 10 -9 s 10 -6 s 10 -3 s 1 s 10 3 s EMIE-UP summer school patrick.rousseau@unicaen.fr 6 “Multiscale Dynamics in Molecular Systems”

  7. Intr trodu ducti ction Instrumentation Me Metastable d disso sociation on Radi diati tive c coo ooling Vibrati tiona nal e electr ctron d detachm chment Slow iso isome merisa sati tion EMIE-UP summer school patrick.rousseau@unicaen.fr 7 “Multiscale Dynamics in Molecular Systems”

  8. Time-of-fmight spectrometer Indeed for relatively “short” timescales (µs range), one may study the so- called delayed fragmentation using time-of-fmight mass spectrometer. With refmectron confjguration, one can observe decays occuring in the fjrst fjeld-free region. ToF EMIE-UP summer school patrick.rousseau@unicaen.fr 8 “Multiscale Dynamics in Molecular Systems”

  9. Storage devices For longer timescales, the fjeld-free region length required is too high. →! one needs to consider alternative confjgurations (multiple refmections, ring…) Storage rings based on magnetic fjeld existed since several decades. However, as the molecular system can be heavy, it is important to consider instead electrostatic device with no mass limitation. In 1997, two families of electrostatic storages devices emerge: ● electrostatic ion beam trap, D. Zajfman et al. in Israel ● electrostatic storage ring, L. H. Anderson et al. in Danmark EMIE-UP summer school patrick.rousseau@unicaen.fr 9 “Multiscale Dynamics in Molecular Systems”

  10. Electrostatic ion beam trap The idea is to use two electrostatic mirrors in order to obtain multiple refmection of the beam. ● compact design (~ 1m) ● long storage time in UHV condition (100 ms to s) D. Zajfman et al. Phys. Rev. A 55 (1997) R1577 EMIE-UP summer school patrick.rousseau@unicaen.fr 10 “Multiscale Dynamics in Molecular Systems”

  11. Electrostatic ion beam trap (2) Neutral detector t Pick-up signal t D. Zajfman et al. Phys. Rev. A 55 (1997) R1577 EMIE-UP summer school patrick.rousseau@unicaen.fr 11 “Multiscale Dynamics in Molecular Systems”

  12. Electrostatic storage ring The use of electrostatic steering elements removes the mass limitation. S. P. Moller Nucl. Instrum. Methods A 394 (1997) 281 EMIE-UP summer school patrick.rousseau@unicaen.fr 12 “Multiscale Dynamics in Molecular Systems”

  13. Electrostatic storage ring (2) t S. P. Moller Nucl. Instrum. Methods A 394 (1997) 281 EMIE-UP summer school patrick.rousseau@unicaen.fr 13 “Multiscale Dynamics in Molecular Systems”

  14. Intr trodu ducti ction Instru strume ment ntatio ion Metastable dissociation Radi diati tive c coo ooling Vibrati tiona nal e electr ctron d detachm chment Slow iso isome merisa sati tion EMIE-UP summer school patrick.rousseau@unicaen.fr 14 “Multiscale Dynamics in Molecular Systems”

  15. Metastable fragmentation Multiply charged fullerene can accomodate the charge excess. →! they are metastable on the µs timescale. This is due to the presence of a fjssion barrier associated with a transition state during the dissociation. Theoretical predictions stated that is stable while the dissociation energy is favourable from . [S. Díaz-Tendero et al., Phys. Rev. Lett. 95 (2005) 013401] EMIE-UP summer school patrick.rousseau@unicaen.fr 15 “Multiscale Dynamics in Molecular Systems”

  16. Metastable decay of Using a long extraction region (several cm), it is possible to observe decays on the µs range. H. da Silva et al. ToF Phys. Rev. A 90 (2014) 032701 EMIE-UP summer school patrick.rousseau@unicaen.fr 16 “Multiscale Dynamics in Molecular Systems”

  17. Metastable decay of : theory Based on the Weisskopf theory, a fragmentation model is obtained. The dissociation rate depends on the dissociation energy and fjssion barrier energy. Competition between dissociation by emission of neutral/charged C 2 . For higher charged states ( q ≥ 4), one can expect a delayed fjssion. H. da Silva et al. Phys. Rev. A 90 (2014) 032701 EMIE-UP summer school patrick.rousseau@unicaen.fr 17 “Multiscale Dynamics in Molecular Systems”

  18. Metastable fjssion of H. Lebius et al. Phys. Scr. T80 (1999) 197 It is possible to deduce the lifetime of the metastable states studying their delayed fragmentation. EMIE-UP summer school patrick.rousseau@unicaen.fr 18 “Multiscale Dynamics in Molecular Systems”

  19. Power law decay Complex molecules with a broad energy distribution →! population of many initial excited states →! many difgerent exponential decays The emission rate is given by Considering that the energy distribution decays exponentially from an initial one broad enough to be considered as constant If is strongly peaked at its maximum It may be necessary to include a second term to the exponent EMIE-UP summer school patrick.rousseau@unicaen.fr 19 “Multiscale Dynamics in Molecular Systems”

  20. Metastable decay of : higher E Delaying the extraction of the ion into the ToF, one can study longer timescale. Evaporation model fails to fjt data K. Hansen and E. E. B. Campbell →! competitive process J. Phys. Chem. 104 (1996) 5012 EMIE-UP summer school patrick.rousseau@unicaen.fr 20 “Multiscale Dynamics in Molecular Systems”

  21. Take home message #1 Coupling between electronic and vibrational degrees of freedom by internal conversion. →! hot species are produced Decay through: ● Dissociation ● thermoionic electron emission Evaporative model may be applied power law decay if broad initial energy distributions However some discrepancies may appear →! competitive process EMIE-UP summer school patrick.rousseau@unicaen.fr 21 “Multiscale Dynamics in Molecular Systems”

  22. Intr trodu ducti ction Instru strume ment ntatio ion Me Metastable d disso sociation on Radiative cooling Vibrati tiona nal e electr ctron d detachm chment Slow iso isome merisa sati tion EMIE-UP summer school patrick.rousseau@unicaen.fr 22 “Multiscale Dynamics in Molecular Systems”

  23. Radiative cooling Beside the dissociation, the internal energy can be lowered via electronic, vibrational and/or rotational transitions →! emission of one photon →! radiative cooling EMIE-UP summer school patrick.rousseau@unicaen.fr 23 “Multiscale Dynamics in Molecular Systems”

  24. Radiative cooling of fullerene The radiative cooling quenches the thermoionic electron emission. Neutral counts Time [s] J. U. Andersen et al. Eur. Phys. J. D 17 (2001) 189 EMIE-UP summer school patrick.rousseau@unicaen.fr 24 “Multiscale Dynamics in Molecular Systems”

  25. Poincaré fmuorescence The radiative cooling via vibrational transitions is associated with IR photons and long timescale (ms). It was proposed that inverse internal conversion (IIC) can lead to a fast radiative cooling by recurrent fmuorescence. A. Léger, P. Boissel, L. d’Hendecourt Phys. Rev. Lett. 60 (1988) 921 EMIE-UP summer school patrick.rousseau@unicaen.fr 25 “Multiscale Dynamics in Molecular Systems”

  26. Fast radiative cooling of anthracene Using a compact storage ring, the MINI-RING in Lyon, short revolution times (few µs) are accessible. A fast quenching of the dissociation of anthracene cation is observed. S. Martin et al. Phys. Rev. Lett. 110 (2013) 063003 EMIE-UP summer school patrick.rousseau@unicaen.fr 26 “Multiscale Dynamics in Molecular Systems”

  27. Fast radiative cooling of anthracene (2) Decay as a function of the cooling time shows that the anthracene population cools down on the ms timescale. →! internal energy distribution Fast radiative cooling: IR cooling rate: →! Poincaré fmuorescence S. Martin et al. Phys. Rev. Lett. 110 (2013) 063003 EMIE-UP summer school patrick.rousseau@unicaen.fr 27 “Multiscale Dynamics in Molecular Systems”

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