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Volumn , Issue , 1999, Pages 310-320

Status of the laser electron accelerator project

Author keywords

[No Author keywords available]

Indexed keywords

PARTICLE ACCELERATORS; PARTICLE BEAM DYNAMICS; PLASMA ACCELERATORS; TRAVELING WAVE TUBES;

EID: 0012560858     PISSN: None     EISSN: None     Source Type: Conference Proceeding    
DOI: None     Document Type: Conference Paper
Times cited : (1)

References (8)
  • 1
    • 0030569837 scopus 로고    scopus 로고
    • Proposed structure for a crossed laser beam, GeV per meter gradient, vacuum electron linear accelerator
    • Y.C. Huang, D. Zheng, W.M. Tulloch, R.L. Byer, "Proposed structure for a crossed laser beam, GeV per meter gradient, vacuum electron linear accelerator", Appl. Phys. Lett. 68,753 (1996).
    • (1996) Appl. Phys. Lett. , vol.68 , pp. 753
    • Huang, Y.C.1    Zheng, D.2    Tulloch, W.M.3    Byer, R.L.4
  • 2
    • 0000001493 scopus 로고    scopus 로고
    • Proposed high-gradient laser-driven electron accelerator using crossed cylindrical laser focusing
    • Y.C. Huang, R.L. Byer, "Proposed high-gradient laser-driven electron accelerator using crossed cylindrical laser focusing", Appl. Phys. Lett. 69,2175 (1996).
    • (1996) Appl. Phys. Lett. , vol.69 , pp. 2175
    • Huang, Y.C.1    Byer, R.L.2
  • 4
    • 4444239860 scopus 로고
    • On the Classical Radiation of Accelerated Electrons
    • J. Schwinger, "On the Classical Radiation of Accelerated Electrons", Phys. Rev. Vol. 75 12 1912 (1949).
    • (1949) Phys. Rev , vol.75 , Issue.12 , pp. 1912
    • Schwinger, J.1
  • 5
    • 85032574720 scopus 로고    scopus 로고
    • Limitations Imposed by Beam-Beam Effects and Their Remedies" to be published in the Int'l
    • J.E. Spencer, "Limitations Imposed by Beam-Beam Effects and Their Remedies" to be published in the Int'l. Jrnl. Of Physics A (1998).
    • (1998) Jrnl. of Physics A
    • Spencer, J.E.1
  • 6
    • 85032568772 scopus 로고    scopus 로고
    • ½ rather than n. The scattering in the forward direction is coherent but with a classical phase uncertainty
    • ½ rather than n. The scattering in the forward direction is coherent but with a classical phase uncertainty.
  • 7
    • 85032590901 scopus 로고    scopus 로고
    • 2/2 can be identified as the ponderomotive potential in the equivalent Hamiltonian for the electron in the laser field
    • 2/2 can be identified as the ponderomotive potential in the equivalent Hamiltonian for the electron in the laser field.
  • 8
    • 85032578480 scopus 로고    scopus 로고
    • When the E- and B- fields are equal and orthogonal as in a plane wave the coupling goes to zero as the particle velocity v approaches c for copropagating beams. This is one reason why we cross a pair of laser beams at an angle with respect to the particle beam. This also eliminates any transverse acceleration and its larger radiative effects. Body self fields cancel but external B-fields, imposed for better synchronism, require radiative corrections that are seldom discussed. This is one reason why we don't use external B-fields. Other technical objections3 such as reduced beam intensities are discussed in Ref.5
    • When the E- and B- fields are equal and orthogonal as in a plane wave the coupling goes to zero as the particle velocity v approaches c for copropagating beams. This is one reason why we cross a pair of laser beams at an angle with respect to the particle beam. This also eliminates any transverse acceleration and its larger radiative effects. Body self fields cancel but external B-fields, imposed for better synchronism, require radiative corrections that are seldom discussed. This is one reason why we don't use external B-fields. Other technical objections3 such as reduced beam intensities are discussed in Ref.5.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.