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Volumn 12, Issue 7, 2009, Pages

Assessment of the basic parameters of the CERN Superconducting Proton Linac

Author keywords

[No Author keywords available]

Indexed keywords


EID: 68949147864     PISSN: None     EISSN: 10984402     Source Type: Journal    
DOI: 10.1103/PhysRevSTAB.12.070402     Document Type: Article
Times cited : (28)

References (39)
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    • The theoretical magnetic field limit for a perfect superconducting surface is the superheating field Bsh, beyond which magnetic flux will enter into the superconductor. Real surfaces of type II superconductors will allow flux entry already at the lower critical field Bc1
    • The theoretical magnetic field limit for a perfect superconducting surface is the superheating field Bsh, beyond which magnetic flux will enter into the superconductor. Real surfaces of type II superconductors will allow flux entry already at the lower critical field Bc1
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    • This equation is strictly speaking only valid for T
    • This equation is strictly speaking only valid for T
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    • Passband refers to the frequency bandwidth of a mode family (see, for instance, the dispersion curve in Fig. 11). For each cell of the cavity one can find one mode on this dispersion curve.
    • Passband refers to the frequency bandwidth of a mode family (see, for instance, the dispersion curve in Fig. 11). For each cell of the cavity one can find one mode on this dispersion curve.
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    • In comparison to we have additionally approximated ωk2-ωm2 by 2ωm(ωk-ωm).
    • In comparison to we have additionally approximated ωk2-ωm2 by 2ωm(ωk-ωm).
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.