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0000008322 00000 n <>>> Project title: Electron beam dynamics studies applied to the synchrotron ALBA Project Description ALBA is a 3 GeV synchrotron ring with a circumference of 268 m an electron beam emittance of 4.5 nm rad. 0000002938 00000 n %%EOF 9 0 obj 0000000947 00000 n

0000001564 00000 n 0000001948 00000 n 12 0 obj This produces nonlinear motion and harmonics. Normalized field strength In weak fields (K < 1), motion is sinusoidal, no harmonics In strong fields (K>1) motion is relativistic in the co-moving frame. <> 2 K.H. e)��� :�L�����h\4���qQ9�7>4�Lfa��'K��vg���d��o9&�s@�Q*3�DA��89�(�h��i��HҦ ALTHOFF et al. 0000004839 00000 n �i����U��ū������n>�A�D-��C{p�x��yX��~�3tz���-Wݢ��.�t�fɵ=�q�����+X�����z�Ӓ����/x��|Z��%tG�u��y�������/��Q����u�ڗ˕Y���\��B�V�a�~��G'X��n����~�=V��� 27�\WUI��H��HjZ�t;軋�֦���Z457��>����f���k ��z���Z��B��~�Up�^�x=\ <>/ExtGState<>/ProcSet[/PDF/Text/ImageB/ImageC/ImageI] >>/MediaBox[ 0 0 612 792] /Contents 19 0 R/Group<>/Tabs/S/StructParents 1>> 0000006635 00000 n

Synchrotron Radiation and Free Electron Lasers Grenoble, France, 22 - 27 April 1996 (A. Hofmann’slectures on synchrotron radiation) CERN Yellow Report 98-04 Brunnen, Switzerland, 2 –9 July 2003 CERN Yellow Report 2005-012 Previous CAS Schools Proceedings CERN Accelerator School Proceedings. On the other hand, we wanted the new machine to be … u �2�jB%��"9���iY���`A�€$��D3�E0s����. x����K�0����Q�t�4? @���Ā�)g���5kxN��ge�8 endobj

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h�b```f``�c`�W@���� (�1��x�qП��H��u�!~WQ>q�/�u|���~�\��[���+���/���g3��^V�@�d�l�V�˼��F||�{�W�e�j�������[#�_��=�)^K>V� �|���tx[xW�M�;ɳ��o� /�k^. A general overview of recent activities at synchrotron radiation and free-electron laser projects is presented.

In the present paper the theory for this latter accelerator is developed with particular reference to the problems of injection and stability in the initial acceleration period.

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<> <> endobj 5 0 obj 6 0 obj %PDF-1.6 %���� 2 0 obj <. Synchrotron and Free electron laser Radiation: generation and application (SFR-2020) July 13 – 16, 2020 Book of Abstracts Conference organized by Budker INP Мероприятие проводится при финансовой поддержке РФФИ, проект № 20-02-22006 Conference sponsored by Novosibirsk 2020 . <> 467 0 obj <>stream APRIL 1968 1 . It was originally observed in early betatron experiments in which electrons were first accelerated to ultrarelativistic energies. 1 INTRODUCTION Whenever relativistic light charged particles such as electrons or positrons are bent in a magnetic field synchrotron radiation (SR) is emitted.

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8 0 obj stream %PDF-1.5 ��"O�C��Z�5��I]fM�E&�������]dg��r�a�m�*=���Z�ߐ2�>��+�7��:;�cV�m27���� �=_�V�,4�i�����l"������9�w,�~����B,�jyظ�oZ��?��U�Z��Hh6S����k6J�}\��7���vR�Â!֠�}��ʅ�o�&v �� �а�:fo�'�~��xy�.�B���d�L���H�2S0��}����}����O䫋����rg�gO?5�Җ�1��̀�佚�mY�t�T���ʹ|�Ļ�v�h���2=rM#G�s۶&/[�����ӷ�B��3m�yW�x{ ��`x�v���?�c����ވ�d]ғm�_|v:�?��]�}�l���B�f�t�D*��=�=��Iu�߷E�����M�=l�-I��a1&�e�7�_L꠨��I�y*dC���#��éh��]i��͢��8 HO^\ѵ�W��(��R��ߝ��{�'팔�I;-ņ���g�F�oJ/�2�Ը<7��tF�w��O��}���;��R:��R Mk}�$�O\�=�`D����4�?bOY0l~ �9`�ǃ:y�$�]�5��U��d�y���2R endobj General view of the 2.5 GeV electron-synchrotron before completion of the shielding tunnel (Photo K. Kiiffner).

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0000001564 00000 n 0000001948 00000 n 12 0 obj This produces nonlinear motion and harmonics. Normalized field strength In weak fields (K < 1), motion is sinusoidal, no harmonics In strong fields (K>1) motion is relativistic in the co-moving frame. <> 2 K.H. e)��� :�L�����h\4���qQ9�7>4�Lfa��'K��vg���d��o9&�s@�Q*3�DA��89�(�h��i��HҦ ALTHOFF et al. 0000004839 00000 n �i����U��ū������n>�A�D-��C{p�x��yX��~�3tz���-Wݢ��.�t�fɵ=�q�����+X�����z�Ӓ����/x��|Z��%tG�u��y�������/��Q����u�ڗ˕Y���\��B�V�a�~��G'X��n����~�=V��� 27�\WUI��H��HjZ�t;軋�֦���Z457��>����f���k ��z���Z��B��~�Up�^�x=\ <>/ExtGState<>/ProcSet[/PDF/Text/ImageB/ImageC/ImageI] >>/MediaBox[ 0 0 612 792] /Contents 19 0 R/Group<>/Tabs/S/StructParents 1>> 0000006635 00000 n

Synchrotron Radiation and Free Electron Lasers Grenoble, France, 22 - 27 April 1996 (A. Hofmann’slectures on synchrotron radiation) CERN Yellow Report 98-04 Brunnen, Switzerland, 2 –9 July 2003 CERN Yellow Report 2005-012 Previous CAS Schools Proceedings CERN Accelerator School Proceedings. On the other hand, we wanted the new machine to be … u �2�jB%��"9���iY���`A�€$��D3�E0s����. x����K�0����Q�t�4? @���Ā�)g���5kxN��ge�8 endobj

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In the present paper the theory for this latter accelerator is developed with particular reference to the problems of injection and stability in the initial acceleration period.

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<> <> endobj 5 0 obj 6 0 obj %PDF-1.6 %���� 2 0 obj <. Synchrotron and Free electron laser Radiation: generation and application (SFR-2020) July 13 – 16, 2020 Book of Abstracts Conference organized by Budker INP Мероприятие проводится при финансовой поддержке РФФИ, проект № 20-02-22006 Conference sponsored by Novosibirsk 2020 . <> 467 0 obj <>stream APRIL 1968 1 . It was originally observed in early betatron experiments in which electrons were first accelerated to ultrarelativistic energies. 1 INTRODUCTION Whenever relativistic light charged particles such as electrons or positrons are bent in a magnetic field synchrotron radiation (SR) is emitted.

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8 0 obj stream %PDF-1.5 ��"O�C��Z�5��I]fM�E&�������]dg��r�a�m�*=���Z�ߐ2�>��+�7��:;�cV�m27���� �=_�V�,4�i�����l"������9�w,�~����B,�jyظ�oZ��?��U�Z��Hh6S����k6J�}\��7���vR�Â!֠�}��ʅ�o�&v �� �а�:fo�'�~��xy�.�B���d�L���H�2S0��}����}����O䫋����rg�gO?5�Җ�1��̀�佚�mY�t�T���ʹ|�Ļ�v�h���2=rM#G�s۶&/[�����ӷ�B��3m�yW�x{ ��`x�v���?�c����ވ�d]ғm�_|v:�?��]�}�l���B�f�t�D*��=�=��Iu�߷E�����M�=l�-I��a1&�e�7�_L꠨��I�y*dC���#��éh��]i��͢��8 HO^\ѵ�W��(��R��ߝ��{�'팔�I;-ņ���g�F�oJ/�2�Ը<7��tF�w��O��}���;��R:��R Mk}�$�O\�=�`D����4�?bOY0l~ �9`�ǃ:y�$�]�5��U��d�y���2R endobj General view of the 2.5 GeV electron-synchrotron before completion of the shielding tunnel (Photo K. Kiiffner).

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�AEAT`.�"��.� a�x��h4��C)��n4�N�Qd@l4�M1�$l�4I����f9M�Ay��)*�PHx�`8�C�Pz. endobj Seeing the electron beam (SLS) Making an image of the electron beam using the vertically polarised synchrotron light . endobj 0000004818 00000 n endobj 0000001711 00000 n 10 0 obj endobj

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Relativistic electron moves in alternating magnetic field In the average co-moving frame of the electron the undulator wavelength is shortened by gamma. 19 0 obj 459 0 obj <>/Filter/FlateDecode/ID[<5F4AB798CD113F15644B41BA1C951A83>]/Index[445 23]/Info 444 0 R/Length 81/Prev 749328/Root 446 0 R/Size 468/Type/XRef/W[1 2 1]>>stream <>

0000008322 00000 n <>>> Project title: Electron beam dynamics studies applied to the synchrotron ALBA Project Description ALBA is a 3 GeV synchrotron ring with a circumference of 268 m an electron beam emittance of 4.5 nm rad. 0000002938 00000 n %%EOF 9 0 obj 0000000947 00000 n

0000001564 00000 n 0000001948 00000 n 12 0 obj This produces nonlinear motion and harmonics. Normalized field strength In weak fields (K < 1), motion is sinusoidal, no harmonics In strong fields (K>1) motion is relativistic in the co-moving frame. <> 2 K.H. e)��� :�L�����h\4���qQ9�7>4�Lfa��'K��vg���d��o9&�s@�Q*3�DA��89�(�h��i��HҦ ALTHOFF et al. 0000004839 00000 n �i����U��ū������n>�A�D-��C{p�x��yX��~�3tz���-Wݢ��.�t�fɵ=�q�����+X�����z�Ӓ����/x��|Z��%tG�u��y�������/��Q����u�ڗ˕Y���\��B�V�a�~��G'X��n����~�=V��� 27�\WUI��H��HjZ�t;軋�֦���Z457��>����f���k ��z���Z��B��~�Up�^�x=\ <>/ExtGState<>/ProcSet[/PDF/Text/ImageB/ImageC/ImageI] >>/MediaBox[ 0 0 612 792] /Contents 19 0 R/Group<>/Tabs/S/StructParents 1>> 0000006635 00000 n

Synchrotron Radiation and Free Electron Lasers Grenoble, France, 22 - 27 April 1996 (A. Hofmann’slectures on synchrotron radiation) CERN Yellow Report 98-04 Brunnen, Switzerland, 2 –9 July 2003 CERN Yellow Report 2005-012 Previous CAS Schools Proceedings CERN Accelerator School Proceedings. On the other hand, we wanted the new machine to be … u �2�jB%��"9���iY���`A�€$��D3�E0s����. x����K�0����Q�t�4? @���Ā�)g���5kxN��ge�8 endobj

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h�b```f``�c`�W@���� (�1��x�qП��H��u�!~WQ>q�/�u|���~�\��[���+���/���g3��^V�@�d�l�V�˼��F||�{�W�e�j�������[#�_��=�)^K>V� �|���tx[xW�M�;ɳ��o� /�k^. A general overview of recent activities at synchrotron radiation and free-electron laser projects is presented.

In the present paper the theory for this latter accelerator is developed with particular reference to the problems of injection and stability in the initial acceleration period.

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0000001044 00000 n 4 0 obj �S�aBBm�Qw�� ?sj� U3��G�浰�X���G��+�A_R;�M^] r*�ˆ(�mڹ�s.�Y��/n�ܵ�Q}�Þl2OT���po�ݤng�؞�E�.��\��]e�8��2����z��Kk�d�B�K�+��3���{zpcZP����'�b:�c9��� efL���b������Yȓu�[����c�t�b���EM�pΚ��g�r�t��clI@N= ��5��� Electron Beam Dynamics, L. Rivkin, Intro to Accelerator Physics, Vysoke-Tatry Seeing the electron beam (SLS) X rays visible light, vertically polarised V x ~ 55Pm. endobj 0000005702 00000 n 16 0 obj

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<> <> endobj 5 0 obj 6 0 obj %PDF-1.6 %���� 2 0 obj <. Synchrotron and Free electron laser Radiation: generation and application (SFR-2020) July 13 – 16, 2020 Book of Abstracts Conference organized by Budker INP Мероприятие проводится при финансовой поддержке РФФИ, проект № 20-02-22006 Conference sponsored by Novosibirsk 2020 . <> 467 0 obj <>stream APRIL 1968 1 . It was originally observed in early betatron experiments in which electrons were first accelerated to ultrarelativistic energies. 1 INTRODUCTION Whenever relativistic light charged particles such as electrons or positrons are bent in a magnetic field synchrotron radiation (SR) is emitted.

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8 0 obj stream %PDF-1.5 ��"O�C��Z�5��I]fM�E&�������]dg��r�a�m�*=���Z�ߐ2�>��+�7��:;�cV�m27���� �=_�V�,4�i�����l"������9�w,�~����B,�jyظ�oZ��?��U�Z��Hh6S����k6J�}\��7���vR�Â!֠�}��ʅ�o�&v �� �а�:fo�'�~��xy�.�B���d�L���H�2S0��}����}����O䫋����rg�gO?5�Җ�1��̀�佚�mY�t�T���ʹ|�Ļ�v�h���2=rM#G�s۶&/[�����ӷ�B��3m�yW�x{ ��`x�v���?�c����ވ�d]ғm�_|v:�?��]�}�l���B�f�t�D*��=�=��Iu�߷E�����M�=l�-I��a1&�e�7�_L꠨��I�y*dC���#��éh��]i��͢��8 HO^\ѵ�W��(��R��ߝ��{�'팔�I;-ņ���g�F�oJ/�2�Ը<7��tF�w��O��}���;��R:��R Mk}�$�O\�=�`D����4�?bOY0l~ �9`�ǃ:y�$�]�5��U��d�y���2R endobj General view of the 2.5 GeV electron-synchrotron before completion of the shielding tunnel (Photo K. Kiiffner).

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