Zobrazeno 1 - 10
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pro vyhledávání: '"David C. Carey"'
Autor:
David C. Carey
Publikováno v:
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 427:1-5
Standardization of beam line representations means that a single set of data can be used in many situations to represent a beam line. This set of data should be the same no matter what the program to be run or the calculation to be made. We have conc
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::6b1caaa8632779d14f5f5fdb10de45f8
https://doi.org/10.1016/s0168-9002(98)01533-2
https://doi.org/10.1016/s0168-9002(98)01533-2
Autor:
David C. Carey
Publikováno v:
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 363:162-172
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::c6fafa577be98debea55f68828201594
https://doi.org/10.1016/0168-9002(95)00363-0
https://doi.org/10.1016/0168-9002(95)00363-0
Autor:
David C. Carey, George H. Gillespie, Nathan A. Brown, Barrey W. Hill, R. Chris Babcock, Hendy Martono
Publikováno v:
AIP Conference Proceedings.
The Particle Beam Optics Interactive Computer Laboratory (PBO Lab) is an educational software concept to aid students and professionals in learning about charged particle beams and particle beam optical systems. The PBO Lab is being developed as a cr
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::eba6a23b4225be78509c20cf7bc58e14
https://doi.org/10.1063/1.52349
https://doi.org/10.1063/1.52349
Autor:
David C. Carey
Publikováno v:
AIP Conference Proceedings.
For the initial design of a beam line or charged particle optical system, it is both useful and convenient to be able to describe the components in terms of a small number of parameters. These parameters are used in a calculation of a transfer map wh
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::9f750ed4677652fcbbe95bf33c81ce94
https://doi.org/10.1063/1.45329
https://doi.org/10.1063/1.45329
Autor:
David C. Carey
Publikováno v:
Physics Today. 56:14-14
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::b3cf25362a9cca5389dc2ec1e53c454b
https://doi.org/10.1063/1.1611339
https://doi.org/10.1063/1.1611339
Autor:
David C. Carey
Publikováno v:
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 258:417-420
Designs of charged particle optical systems are invariably based on two assumptions: (1) The existence of a reference trajectory and (2) midplane symmetry. The reference trajectory is taken to be the path of a charged particle with certain specified
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::e303a1661edf5cec7dbcdba89acbde7b
https://doi.org/10.1016/0168-9002(87)90924-7
https://doi.org/10.1016/0168-9002(87)90924-7
Autor:
David C. Carey, Joseph B. Keller, J. W. Prothero, Fletcher Osterle, Harvey Borovetz, James Hamerly, Jean Toots
Publikováno v:
Physics Today. 27:11-15
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::c5f387d7bf90a6c239da62ea62fc5e14
https://doi.org/10.1063/1.3128796
https://doi.org/10.1063/1.3128796
Publikováno v:
Nuclear Instruments and Methods. 141:393-399
The misalignment of a magnet in a beam line will cause an alteration of the beam envelope at any later point in that beam line. The position of a misaligned magnet may be described in terms of six coordinates, three translational and three rotational
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::43e6a2d2ec16200984129ce635f54f1c
https://doi.org/10.1016/0029-554x(77)90628-0
https://doi.org/10.1016/0029-554x(77)90628-0
Autor:
David C. Carey
Publikováno v:
Physical Review D. 2:163-166
The inelastic channels ${K}^{*}\ensuremath{\pi}$ and $K$ are included in a three-channel model of the $I=\frac{1}{2} p$-wave $K\ensuremath{\pi}$ amplitude. Feynman diagrams for vector-meson exchange are used as input to multichannel $\frac{N}{D}$ equ
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::b98395d52732b676319d04a1e7313e97
https://doi.org/10.1103/physrevd.2.163
https://doi.org/10.1103/physrevd.2.163
