18 September 2022 to 1 October 2022
Lithuania
Europe/Zurich timezone

Contribution List

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  1. 18/09/2022, 08:30
  2. Frank Tecker (CERN)
    19/09/2022, 08:30
  3. Irina Shreyber
    19/09/2022, 09:45

    The purpose of this course is to provide an introduction to Electromagnetic
    Theory. The foundations of electrodynamics starting from the nature of electrical force up to the level of Maxwell equations solutions are presented. It starts with the introduction of the concept of a field, which plays a very important role in the understanding of electricity and magnetism. In addition, moving...

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  4. Irina Shreyber
    19/09/2022, 11:15

    The purpose of this course is to provide an introduction to Electromagnetic Theory. The foundations of electrodynamics starting from the nature of electrical force up to the level of Maxwell equations solutions are presented. It starts with the introduction of the concept of a field, which plays a very important role in the understanding of electricity and magnetism. In addition, moving...

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  5. Wolfgang Hillert (University of Hamburg)
    19/09/2022, 13:45

    The subject of this introductory course is transverse dynamics of charged par-ticle beams in linear approximation. Starting with a discussion of the most im-portant types of magnets and defining their multipole strengths, the linearizedequations of motion of charged particles in static magnetic fields are derivedusing an orthogonal reference frame following the design orbit. ...

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  6. Gijs De Rijk
    19/09/2022, 15:00

    Warm magnets are magnets that function in normal ambient temperature con- ditions. These types are mostly using a soft steel yoke for field amplifica- tion and either Copper or Aluminium coils or permanent magnets to gener- ate the field. Magnets powered with such normal-conducting coils are often also called classical, iron dominated or resistive magnets. Since decades these types of magnets...

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  7. Wolfgang Hillert (University of Hamburg)
    19/09/2022, 16:30

    The subject of this introductory course is transverse dynamics of charged particle beams in linear approximation. Starting with a discussion of the most important types of magnets and defining their multipole strengths, the linearised equations of motion of charged particles in static magnetic fields are derived using an orthogonal reference frame following the design orbit. Analytical...

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  8. 19/09/2022, 17:45
  9. 19/09/2022, 18:45
  10. Irina Shreyber
    20/09/2022, 08:30

    This is an introductory lecture on special relativity which doesn’t require much mathematical background. The theory of special relativity, originally proposed by Albert Einstein in his famous 1905 paper, has had profound consequences on our view of physics, space, and time. The goal of this lecture is to introduce the basic concepts of special relativity without overloading it with formulas....

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  11. Wolfgang Hillert (University of Hamburg)
    20/09/2022, 09:45

    The subject of this introductory course is transverse dynamics of charged particle beams in linear approximation. Starting with a discussion of the most important types of magnets and defining their multipole strengths, the linearised equations of motion of charged particles in static magnetic fields are derived using an orthogonal reference frame following the design orbit. ...

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  12. David Alesini
    20/09/2022, 11:15

    Linear Accelerators (Linacs) are a systems that allow to accelerate charged particles through a linear trajectory by electromagnetic fields. This kind of accelerators find several applications in fundamental research and industry. The main devices used to accelerate the particle beam are described in the first part of the lecture with their main parameters. This includes both Standing (SW) and...

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  13. Gijs De Rijk
    20/09/2022, 13:45
  14. David Alesini
    20/09/2022, 15:00
  15. Wolfgang Hillert (University of Hamburg)
    20/09/2022, 16:30
  16. Andrea Latina (CERN)
    20/09/2022, 17:45
  17. Wolfgang Hillert (University of Hamburg)
    21/09/2022, 08:30
  18. Frank Tecker (CERN)
    21/09/2022, 09:45
  19. Hermann Schmickler (CERN)
    21/09/2022, 11:15
  20. Frank Tecker (CERN)
    21/09/2022, 13:45
  21. Hermann Schmickler (CERN)
    21/09/2022, 15:00
  22. Davide Gamba (CERN), Volker Ziemann (Uppsala University (SE))
    21/09/2022, 16:30
  23. Davide Gamba (CERN), Volker Ziemann (Uppsala University (SE))
    21/09/2022, 17:45
  24. 22/09/2022, 08:30
  25. Dr Suzie Sheehy (University of Oxford and University of Melbourne)
    22/09/2022, 13:45
  26. Volker Ziemann (Uppsala University (SE))
    22/09/2022, 15:00

    After briefly discussing sources of imperfections, we characterize them
    in terms of dipole, quadrupolar, and skew quadrupolar errors and move
    on to discuss how these imperfections are modeled in beam dynamics codes.
    We continue by reviewing the concepts of dispersion and chromaticity and
    explain how they are measured before turning to imperfections that are
    caused by multipoles, in...

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  27. Dr Suzie Sheehy (University of Oxford and University of Melbourne)
    22/09/2022, 16:30
  28. Volker Ziemann (Uppsala University (SE))
    22/09/2022, 17:45

    "
    We introduce the BPM-corrector response coefficient R12 as the key quantity
    to characterise the effect of imperfections on the beam dynamics before
    addressing how the effect of multiple imperfections are combined. We then
    introduce local beam bumps as a means to adjust the beam position locally
    and move on to discuss orbit correction and the orbit response matrix.
    We place special...

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  29. 22/09/2022, 18:45
  30. Peter Forck
    23/09/2022, 08:30
  31. Andrea Latina (CERN)
    23/09/2022, 09:45
  32. Peter Forck
    23/09/2022, 11:15
  33. Volker Ziemann (Uppsala University (SE))
    23/09/2022, 13:45

    "After discussing how to account for the periodicity in rings, we first generalise the response coefficient R12, and then the orbit response matrix to such systems.
    We move on to use the response matrix to correct the orbit and generalise the concept by introducing dispersion-free steering before turning to gradient errors and stop bands. Measuring and correcting the tune addresses one...

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  34. Dan Faircloth (STFC)
    23/09/2022, 15:00
  35. Davide Gamba (CERN), Volker Ziemann (Uppsala University (SE))
    23/09/2022, 16:30
  36. Davide Gamba (CERN), Volker Ziemann (Uppsala University (SE))
    23/09/2022, 17:45
  37. Lenny Rivkin (Paul Scherrer Institute (CH))
    24/09/2022, 08:30
  38. Lenny Rivkin (Paul Scherrer Institute (CH))
    24/09/2022, 09:45
  39. Lenny Rivkin (Paul Scherrer Institute (CH))
    24/09/2022, 11:15
  40. Peter Forck
    24/09/2022, 13:45
  41. Dan Faircloth (STFC)
    24/09/2022, 15:00
  42. Davide Gamba (CERN), Volker Ziemann (Uppsala University (SE))
    24/09/2022, 16:30
  43. Davide Gamba (CERN), Volker Ziemann (Uppsala University (SE))
    24/09/2022, 17:45
  44. Christine Vollinger (CERN)
    26/09/2022, 08:30
  45. Mike Seidel
    26/09/2022, 09:45
  46. Mike Seidel
    26/09/2022, 11:15
  47. Christine Vollinger (CERN)
    26/09/2022, 13:45
  48. Alexandre Lasheen (CERN)
    26/09/2022, 15:00
  49. Alexandre Lasheen (CERN)
    26/09/2022, 16:30
  50. Alexandre Lasheen (CERN)
    26/09/2022, 17:45
  51. Prof. Renaldas Raišutis
    26/09/2022, 18:45

    Development and applications of ultrasonic measurement, monitoring, non-destructive testing and diagnostic techniques

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  52. Kevin Shing Bruce Li (CERN)
    27/09/2022, 08:30
  53. Mike Seidel
    27/09/2022, 09:45
  54. Alexandre Lasheen (CERN)
    27/09/2022, 11:15
  55. Kevin Shing Bruce Li (CERN)
    27/09/2022, 13:45
  56. Alexandre Lasheen (CERN)
    27/09/2022, 15:00
  57. Alexandre Lasheen (CERN)
    27/09/2022, 16:30
  58. Alexandre Lasheen (CERN)
    27/09/2022, 17:45
  59. 28/09/2022, 08:30
  60. Kevin Shing Bruce Li (CERN)
    28/09/2022, 13:45
  61. Hermann Schmickler (CERN)
    28/09/2022, 15:00
  62. Kevin Shing Bruce Li (CERN)
    28/09/2022, 16:30
  63. Kevin Shing Bruce Li (CERN)
    28/09/2022, 17:45
  64. 28/09/2022, 18:45
  65. Hannes Bartosik (CERN)
    29/09/2022, 08:30
  66. Massimo Ferrario
    29/09/2022, 09:45
  67. Hannes Bartosik (CERN)
    29/09/2022, 11:15
  68. Frank Tecker (CERN)
    29/09/2022, 13:45
  69. Yannis Papaphilippou (CERN)
    29/09/2022, 15:00
  70. 29/09/2022, 16:30
  71. Prof. Minvydas Ragulskis
    29/09/2022, 18:45

    Nonlinear dynamical systems - mathematical modelling and applications

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  72. Yannis Papaphilippou (CERN)
    30/09/2022, 08:30
  73. Massimo Ferrario
    30/09/2022, 09:45
  74. Eduard Prat Costa
    30/09/2022, 11:15
  75. Eduard Prat Costa
    30/09/2022, 13:45
  76. Yannis Papaphilippou (CERN)
    30/09/2022, 15:00
  77. Frank Tecker (CERN)
    30/09/2022, 16:30
  78. 01/10/2022, 08:30
  79. Mike Seidel
  80. Mike Seidel
  81. Irina Shreyber (Tomsk State University (RU))