27 February 2024 to 1 March 2024
GANIL
Europe/Paris timezone

List of posters

62 out of 62 displayed
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  1. Franck VARENNE ({CNRS}UPR3266)
    27/02/2024, 14:00
  2. Pierre Chauveau (GANIL)
    27/02/2024, 14:25
  3. Vladimir Manea (IKS, KU Leuven, Belgium)
    27/02/2024, 14:50
  4. Luc PERROT (IJCLAB - Laboratoire de Physique des 2 Infinis Irène Joliot-Curie)
    27/02/2024, 15:15
  5. Gilles Ban (Laboratoire de Physique Corpusculaire de Caen, LPC Caen)
    27/02/2024, 16:00
  6. Julien Michaud (IJCLab - CNRS)
    27/02/2024, 16:20
  7. Mathias Gerbaux (LP2iB - Université de Bordeaux)
    27/02/2024, 16:40
  8. Pauline Ascher (LP2iB)
    27/02/2024, 17:00
  9. Gerda Neyens (KU Leuven)
    28/02/2024, 09:00
  10. Agota Koszorus (KU Leuven, SCK CEN)
    28/02/2024, 09:10
  11. Sarina Geldhof (GANIL)
    28/02/2024, 09:35
  12. Liss Vazquez Rodriguez (CERN, MPIK)
    28/02/2024, 10:00
  13. Louis Lalanne (IPN)
    28/02/2024, 10:25
  14. Pauline Ascher (LP2iB)
    28/02/2024, 11:20
  15. Sarah Naimi (IJCLab)
    28/02/2024, 11:30
  16. Antoine de Roubin (CENBG)
    28/02/2024, 11:55
  17. Matthieu Lebois (IJCLab/Univ. Paris-SAclay)
    28/02/2024, 14:00
  18. Dr Sonja Orrigo (IFIC (CSIC-UV))
    28/02/2024, 14:15
  19. Guillem Tocabens (IPNO)
    28/02/2024, 14:40
  20. James Cubiss (University of York)
    28/02/2024, 15:05
  21. Antoine de Roubin (CENBG)
    28/02/2024, 16:00
  22. Dr Enrique Minaya Ramirez (IJCLab)
    28/02/2024, 16:25
  23. Francesca Giacoppo (GSI Helmholtzzentrum für Schwerionenforschung GmbH)
    28/02/2024, 16:50
  24. Simon Lechner (CERN)
    28/02/2024, 17:15
  25. Dr Emmanuel Rey-herme (LP2IB)
    29/02/2024, 09:00
  26. Bernadette Rebeiro (GANIL)
    29/02/2024, 09:25
  27. 29/02/2024, 09:50
  28. Piet Van Isacker (GANIL)
    29/02/2024, 10:15
  29. zhuang ge (GSI)
    29/02/2024, 11:15
  30. Lukas Nies (CERN / University of Greifswald (DE))
    29/02/2024, 11:40
  31. Hervé Savajols (GANIL/CNRS)
    29/02/2024, 12:05
  32. Ruben de Groote
    29/02/2024, 14:00
  33. Monika Piersa-Siłkowska (CERN)
    29/02/2024, 14:25
  34. Mark Bissell (CERN)
    29/02/2024, 14:50
  35. Phillip Imgram (Institute for Nuclear Physics, Technical University Darmstadt)
    29/02/2024, 15:15
  36. Mustapha Laatiaoui
    29/02/2024, 16:10
  37. Michail Athanasakis-Kaklamanakis (CERN)
    29/02/2024, 16:35
  38. Iolanda MATEA MACOVEI (IPN Orsay)
    29/02/2024, 17:00
  39. Jérôme Giovinazzo (LP2IB (CENBG) CNRS / Univ. Bordeaux)
    29/02/2024, 17:25
  40. Georgi Georgiev (CSNSM, Orsay, France)
    29/02/2024, 17:50
  41. Alberto Perez de Rada Fiol (CIEMAT)
    29/02/2024, 18:15
  42. Luis Miguel Motilla Martinez (University of Caen, GANIL, University of Jyvaskyla)
    01/03/2024, 09:00
  43. Maud Versteegen (CENBG)
    01/03/2024, 09:25
  44. Michele Sguazzin (CNRS)
    01/03/2024, 09:50
  45. List of posters

    Core Collapse Supernova (CCSN) explosion is the final process suffer by starts with initial mass greater than 8 M⨀. In such processes the 44Ti nucleosynthesis takes place, doing the isotope a good gamma tracer of Supernovae events, due to its characteristic gamma decay chain. The comparison between observations and models of the synthetized 44Ti in CCSN gives important constrains to the models...

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  46. Collinear laser spectroscopy coupled with optical pumping, within the cooler-buncher, has proved a highly successful technique at IGISOL-4 (and at the previous IGISOL-3) [1-3] and has facilitated spectroscopy on manganese, niobium, yttrium and even the doubly charged yttrium ion. The technique is however critically limited by conditions within the cooler-buncher. The pumping, while highly...

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  47. List of posters

    $\beta$-delayed neutron emissions play a crucial role in various fields, including nuclear technology and nuclear astrophysics. Our research group boasts extensive expertise in measuring $\beta$-delayed one and two neutron emission probabilities ($P_{1n}$ and $P_{2n}$ values), as well as decay half-lives of exotic nuclei, utilizing the state-of-the-art BELEN and BRIKEN (Beta delayed neutron...

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  48. List of posters

    Laser spectroscopy can study many ground-state properties (spin, nuclear electromagnetic moments, changes in the charge radius) of the nucleus which can challenge state-of-the-art nuclear models, and enhance our understanding of the nuclear forces. Furthermore, its application at ISOL facilities can give access to the same properties of long-lived states (>10ms). One major challenge that laser...

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  49. Luis Miguel Motilla Martinez (University of Caen, GANIL, University of Jyvaskyla)
  50. List of posters

    In the past few years, the spectroscopy of radioactive molecules has been performed at ISOLDE (CERN) using the Collinear Resonance Ionization Spectroscopy (CRIS) experiment [1]. Given their structure and chemical properties, molecules are a promising candidate for studies in different fields [2] and for extracting elements with low production yields due to their refractory or reactive...

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  51. Pauline Ascher (LP2iB)
  52. List of posters

    RIALTO, the Resonant Ionization Laser Ion Source at the ALTO facility, uses a multi-step laser excitation process to produce pure ion beams through the resonance ionization technique.
    The laser laboratory is equipped with three high-power Nd:YAG operating at 10 kHz and pumping three dye lasers; these lasers are coupled with BBO doubling units and one tripling unit; this laser system allows us...

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  53. List of posters

    The double Penning trap PIPERADE (PIèges de PEnning pour les RAdionucléides à DESIR) [1] for the DESIR facility has been advancing in its commissioning phase at the LP2i-Bordeaux laboratory. The traps were designed with the objective of performing high-precision mass measurements and high-resolution mass purification of strongly contaminated ion beams. The latter will be produced by the...

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  54. List of posters

    The objective of the WISArD experiment is to test the existence of new physics in the weak interaction sector of the Standard Model of particle physics using beta decay. The goal of the WISArD experiment is to measure the angular correlation parameter a and the Fierz interference term b in the decay of 32Ar with a precision of about 0.1%, in order to provide constraints on new physics that...

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