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The electric dipole moment challenge /

The electric dipole moment (EDM) challenge measures a non-zero proton EDM value and this book suggests how the challenge can be met. Any measurably large proton EDM would violate the standard model. The method to be employed uses an intense beam of 'frozen spin' protons circulating for hou...

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Detalles Bibliográficos
Clasificación:Libro Electrónico
Autor principal: Talman, Richard, 1934- (Autor)
Formato: Electrónico eBook
Idioma:Inglés
Publicado: San Rafael [California] (40 Oak Drive, San Rafael, CA, 94903, USA) : Morgan & Claypool Publishers, [2017]
Colección:IOP (Series). Release 3.
IOP concise physics.
Temas:
Acceso en línea:Texto completo

MARC

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100 1 |a Talman, Richard,  |d 1934-  |e author. 
245 1 4 |a The electric dipole moment challenge /  |c Richard Talman. 
264 1 |a San Rafael [California] (40 Oak Drive, San Rafael, CA, 94903, USA) :  |b Morgan & Claypool Publishers,  |c [2017] 
264 2 |a Bristol [England] (Temple Circus, Temple Way, Bristol BS1 6HG, UK) :  |b IOP Publishing,  |c [2017] 
300 |a 1 online resource (various pagings) :  |b illustrations (some color). 
336 |a text  |2 rdacontent 
337 |a electronic  |2 isbdmedia 
338 |a online resource  |2 rdacarrier 
490 1 |a [IOP release 3] 
490 1 |a IOP concise physics,  |x 2053-2571 
500 |a "Version: 20170401"--Title page verso. 
500 |a "A Morgan & Claypool publication as part of IOP Concise Physics"--Title page verso. 
504 |a Includes bibliographical references. 
505 0 |a Preface -- 1. Symmetry, physical laws, and electric dipole moments -- 1.1. Introduction -- 1.2. Force field symmetries -- 1.3. Why measure EDMs, which, and how? 
505 8 |a 2. Some essential experiments -- 2.1. Neutron EDM measurements -- 2.2. Penning traps and Penning-like traps -- 2.3. Electron EDM measurement using polar molecule enhancement -- 2.4. The future 
505 8 |a 3. Magnetic precessions -- 3.1. Cyclotron rotation, gyromagnetic ratio, and Larmor precession -- 3.2. Storage ring EDM measurement -- 3.3. Spurious magnetic precessions 
505 8 |a 4. Just enough accelerator physics -- 4.1. Preview -- 4.2. The uniform field ring -- 4.3. Horizontal stability -- 4.4. Vertical stability -- 4.5. Simultaneous horizontal and vertical stability -- 4.6. Dispersion -- 4.7. Momentum compaction -- 4.8. Chromaticity -- 4.9. Transfer matrices -- 4.10. Transfer matrices for simple elements -- 4.11. Transfer matrix parameterization -- 4.12. Strong focusing -- 4.13. General transverse motion 
505 8 |a 5. All-electric particle dynamics -- 5.1. Background -- 5.2. Introduction -- 5.3. Particle tracking paradigms -- 5.4. Relativistic kinematics in central force electric field 
505 8 |a 6. The all-electric Brookhaven electron storage ring -- 6.1. Introduction -- 6.2. Storage rings for frozen spin electrons or protons -- 6.3. The AGS electron analogue ring -- 6.4. Current day simulation of 1955 machine studies tune plane scan 
505 8 |a 7. A self-magnetometer storage ring -- 7.1. Abstract -- 7.2. Introduction -- 7.3. Orbit equations for the storage ring bottle -- 7.4. Self-magnetometer precision 
505 8 |a 8. Frequency domain EDM experiment design -- 8.1. Introduction -- 8.2. Proposed method -- 8.3. Error analysis strategy -- 8.4. Spin precession -- 8.5. Conquering [delta]Br field errors -- 8.6. Roll-reversal accuracy -- 8.7. Other calculations -- 8.8. Recapitulation and conclusions 
505 8 |a 9. The Bargmann-Michel-Telegdi equation -- 9.1. Relativistic mechanics -- 9.2. Angular momentum 3-vector s -- 9.3. The momentum-weighted spin 4-vector W -- 9.4. Lorentz transformation of 4-spin components -- 9.5. The BMT equation -- 9.6. Special cases of spin precession 
505 8 |a 10. Relativistic Stern-Gerlach deflection -- 10.1. Introduction -- 10.2. Brief historical perspective -- 10.3. Lorentz force law -- 10.4. Relativistic S-G deflection -- 10.5. Deflection examples -- 10.6. Practical observation of S-G deflection -- 10.7. S-G deflection of a relativistic particle -- 10.8. S-G specific beam preparation -- 10.9. Signal levels and background rejection -- 10.10. Recapitulation and acknowledgements. 
520 3 |a The electric dipole moment (EDM) challenge measures a non-zero proton EDM value and this book suggests how the challenge can be met. Any measurably large proton EDM would violate the standard model. The method to be employed uses an intense beam of 'frozen spin' protons circulating for hour-long times in a storage ring 'trap'. The smallness of EDMs allows them to test existing theories, but also makes them hard to measure. Such EDM experiments are inexpensive, at least compared to building accelerators of ever-greater energy. 
530 |a Also available in print. 
538 |a Mode of access: World Wide Web. 
538 |a System requirements: Adobe Acrobat Reader, EPUB reader, or Kindle reader. 
545 |a Richard Talman is Professor Emeritus in the Department of Physics, Cornell University. He received his PhD in 1963 from the California Institute of Technology. His recent efforts have been devoted to planning for a new generation of accelerators following the LHC p,p collider at CERN He has also been developing a method for measuring the electric dipole moments (EDM) of the electron and proton. His multiple visiting appointments include Stanford, CERN, UC Berkeley, University of Chicago, University of Texas at Austin, Duke, and many more. 
588 |a Title from PDF title page (viewed on June 12, 2017). 
650 0 |a Dipole moments. 
650 0 |a Proton accelerators. 
650 7 |a Particle & high-energy physics.  |2 bicssc 
650 7 |a Particle & High Energy Physics.  |2 bisacsh 
710 2 |a Morgan & Claypool Publishers,  |e publisher. 
710 2 |a Institute of Physics (Great Britain),  |e publisher. 
776 0 8 |i Print version:  |z 9781681745084 
830 0 |a IOP (Series).  |p Release 3. 
830 0 |a IOP concise physics. 
856 4 0 |u https://iopscience.uam.elogim.com/book/978-1-6817-4509-1  |z Texto completo