Robert L. Gluckstern, Johannes van Zeijts, and Bruno Zotter. Coupling impedance of beam pipes of general cross section. Phys. Rev. E, 47(1):656--663, January 1993. Home/Search Document Not in Database Summary Related Articles Check |
This paper is cited in the following contexts:
Coherent Modes for Multiple Non-Rigid Bunches in a Storage Ring - Berg (1996) (Correct)
....(5. 3) Here b p is the smallest half dimension (vertical or horizontal) of the vacuum chamber, L p is the length of the vacuum chamber, # is the vacuum chamber wall conductivity, Z 0 is the impedance of free space (#377##0 and F is a form factor which depends only on the shape of the vacuum chamber [28]. The arc sections of the vacuum chamber are elliptical with a major axis of 3.740 inches and a minor axis of 2.170 inches [50] This geometry makes F 0.8263 [28] The vacuum chamber is made of 6063 T5 aluminum alloy [50] which has a resistivity of 1 # = 32 ## nm [4] Thus, RRW for the arc ....
....conductivity, Z 0 is the impedance of free space (#377##0 and F is a form factor which depends only on the shape of the vacuum chamber [28] The arc sections of the vacuum chamber are elliptical with a major axis of 3.740 inches and a minor axis of 2.170 inches [50] This geometry makes F 0. 8263 [28]. The vacuum chamber is made of 6063 T5 aluminum alloy [50] which has a resistivity of 1 # = 32 ## nm [4] Thus, RRW for the arc sections is m. The straight sections of the vacuum chamber are round with a diameter of 3.5 in. 51] F is 1 for this geometry [28] The vacuum chamber is made of ....
[Article contains additional citation context not shown here]
Robert L. Gluckstern, Johannes van Zeijts, and Bruno Zotter. Coupling impedance of beam pipes of general cross section. Phys. Rev. E, 47(1):656--663, January 1993.
Coherent Modes for Multiple Non-Rigid Bunches in a Storage Ring - Berg (1996) (Correct)
....(5. 3) Here b p is the smallest half dimension (vertical or horizontal) of the vacuum chamber, L p is the length of the vacuum chamber, # is the vacuum chamber wall conductivity, Z 0 is the impedance of free space (#377##0 and F is a form factor which depends only on the shape of the vacuum chamber [28]. The arc sections of the vacuum chamber are elliptical with a major axis of 3.740 inches and a minor axis of 2.170 inches [50] This geometry makes F 0.8263 [28] The vacuum chamber is made of 6063 T5 aluminum alloy [50] which has a resistivity of 1 # = 32 ## nm [4] Thus, RRW for the arc ....
....conductivity, Z 0 is the impedance of free space (#377##0 and F is a form factor which depends only on the shape of the vacuum chamber [28] The arc sections of the vacuum chamber are elliptical with a major axis of 3.740 inches and a minor axis of 2.170 inches [50] This geometry makes F 0. 8263 [28]. The vacuum chamber is made of 6063 T5 aluminum alloy [50] which has a resistivity of 1 # = 32 ## nm [4] Thus, RRW for the arc sections is m. The straight sections of the vacuum chamber are round with a diameter of 3.5 in. 51] F is 1 for this geometry [28] The vacuum chamber is made of ....
[Article contains additional citation context not shown here]
Robert L. Gluckstern, Johannes van Zeijts, and Bruno Zotter. Coupling impedance of beam pipes of general cross section. Phys. Rev. E, 47(1):656--663, January 1993.
Status of the Transverse Multibunch Modes in PEP-II - Scott Berg (Correct)
.... (2) Here b p is the smallest half dimension (vertical or horizontal) of the vacuum chamber, L p is the length of the vacuum chamber, # is the vacuum chamber wall conductivity, Z 0 is the impedance of free space (#377##0 and F is a form factor which depends only on the shape of the vacuum chamber [GvZZ93] The arc sections of the low energy ring vacuum chamber are elliptical with a major axis of 3.740 inches and a minor axis of 2.170 inches [PEPa] This geometry makes F 0.4219 in the horizontal direction, and 0.8263 in the vertical direction [GvZZ93] The vacuum chamber is made of 6063 T5 ....
....depends only on the shape of the vacuum chamber [GvZZ93] The arc sections of the low energy ring vacuum chamber are elliptical with a major axis of 3.740 inches and a minor axis of 2.170 inches [PEPa] This geometry makes F 0.4219 in the horizontal direction, and 0. 8263 in the vertical direction [GvZZ93] The vacuum chamber is made of 6063 T5 aluminum alloy [PEPa] which has a resistivity of 1 # = 32###2 [ASM90] The lengths of the low energy ring arc sections can be estimated to be the same as those of the high energy ring arc sections (see below) giving 1490.482 m [Dal] Thus, RRW for the arc ....
[Article contains additional citation context not shown here]
Robert L. Gluckstern, Johannes van Zeijts, and Bruno Zotter. Coupling impedance of beam pipes of general cross section. Phys. Rev. E, 47(1):656--663, January 1993.
Coherent Modes for Multiple Non-Rigid Bunches in a Storage Ring - Berg (1996) (Correct)
.... Here b p is the smallest half dimension (vertical or horizontal) of the vacuum chamber, L p is the length of the vacuum chamber, # is the vacuum chamber wall conductivity, Z 0 is the impedance of free space (#377##0 and F is a form factor which depends only on the shape of the vacuum chamber [28]. The arc sections of the vacuum chamber are elliptical with a major axis of 3.740 inches and a minor axis of 2.170 inches [50] This geometry makes F 0.8263 [28] The vacuum chamber is made of 6063 T5 aluminum alloy [50] which has a resistivity of 1 # = 32 ## nm [4] Thus, RRW for the arc ....
....conductivity, Z 0 is the impedance of free space (#377##0 and F is a form factor which depends only on the shape of the vacuum chamber [28] The arc sections of the vacuum chamber are elliptical with a major axis of 3.740 inches and a minor axis of 2.170 inches [50] This geometry makes F 0. 8263 [28]. The vacuum chamber is made of 6063 T5 aluminum alloy [50] which has a resistivity of 1 # = 32 ## nm [4] Thus, RRW for the arc sections is 825k# m. The straight sections of the vacuum chamber are round with a diameter of 3.5 in. 51] F is 1 for this geometry [28] The vacuum chamber is ....
[Article contains additional citation context not shown here]
Robert L. Gluckstern, Johannes van Zeijts, and Bruno Zotter. Coupling impedance of beam pipes of general cross section. Phys. Rev. E, 47(1):656--663, January 1993.
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