Difference between revisions of "Resonant Polarimeter"
| Line 22: | Line 22: | ||
* ''The Stern-Gerlach interaction between a traveling particle and a time varying magnetic field'' | * ''The Stern-Gerlach interaction between a traveling particle and a time varying magnetic field'' | ||
| − | M. Conte, M. Ferro, G. Gemme, W.W. MacKay, R. Parodi, M. Pusterla, '''arXiv:physics/ | + | M. Conte, M. Ferro, G. Gemme, W.W. MacKay, R. Parodi, M. Pusterla, '''arXiv:physics/0003069v1''' (March 24, 2000): [https://arxiv.org/abs/physics/0003069v1] [[media:arXiv_physics_0003069v1.pdf]] |
* ''Relativistic Stern-Gerlach Interaction in an RF Cavity'' | * ''Relativistic Stern-Gerlach Interaction in an RF Cavity'' | ||
| − | M. Conte, A. U. Luccio, and M. Pusterla, '''arXiv:physics/0907.2161v1''' (February 22, 2013): [https://arxiv.org/abs/0907.2161] [[media:]] | + | M. Conte, A. U. Luccio, and M. Pusterla, '''arXiv:physics/0907.2161v1''' (February 22, 2013): [https://arxiv.org/abs/0907.2161] [[media:arXiv_physics_0907.2161v1.pdf]] |
* ''RF-resonance beam polarimeter Part I. Fundamental concepts'' | * ''RF-resonance beam polarimeter Part I. Fundamental concepts'' | ||
Revision as of 11:44, 20 July 2016
Resonant polarimeter, first proposed by Derbenev in 1993, measures the spin-dependent energy deposited by a beam in cavity via the Stern-Gerlach interaction. This technique of fast non-destructive measurement of beam polarization has been never demonstrated experimentally. We are planning a proof-of-principle test using polarized electrons and a room temperature copper cavity.
Meetings and Discussion
- Richard Talman's SLAC seminar (July 21, 2016): media:Talman_seminar_SLAC-July2016.pdf
- Richard Talman's thoughts on resonant polarimetry (June 1, 2016): media:Talman_Stern_Gerlach_Resonance_Polarimeter.pdf
- Brock's prototype (June 9, 2016): media:Brock_resonant_cavity_prototype.jpg
- Brock's idea (April 27, 2016): media:Brock's_schematic.docx
- Local meeting with Juelich, Bonn and Cornell visitors to discuss resonant polarimeter (February 3-5, 2016): https://www.jlab.org/indico/event/142/
References and Documents
- Measuring the intensity and position of a pA electron beam with resonant cavities
Thorsten R. Pusch, F. Frommberger, W. C. A. Hillert, and B. Neff, Phys. Rev. ST Accel. Beams 15, 112801 (2012): [1] media:PhysRevSTAB.15.112801.pdf
- The Stern-Gerlach interaction between a traveling particle and a time varying magnetic field
M. Conte, M. Ferro, G. Gemme, W.W. MacKay, R. Parodi, M. Pusterla, arXiv:physics/0003069v1 (March 24, 2000): [2] media:arXiv_physics_0003069v1.pdf
- Relativistic Stern-Gerlach Interaction in an RF Cavity
M. Conte, A. U. Luccio, and M. Pusterla, arXiv:physics/0907.2161v1 (February 22, 2013): [3] media:arXiv_physics_0907.2161v1.pdf
- RF-resonance beam polarimeter Part I. Fundamental concepts
Ya. S. Derbenev, Nucl. Inst. Meth. A 336, 12 (1993): [4] media:NuclInstMethA.336.12.pdf
- Lorentz Transform of an Arbitrary Force Field Acting on a Particle in its Rest Frame, using the Hamilton-Lagrangian Formalism
C. Tschalär, BIR#15-01, Bates Lab Report (June 24, 2016): media:Tschaller_Tech_Note_B-IR.pdf
- Proposal for a cavity polarimeter at MIT-Bates
P. Cameron et al., Proceedings of the 2001 Particle Accelerator Conference, Chicago: [5] media:BATES_PAC2001.00987396.pdf