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Proposed structure for a crossed laser beam, GeV per meter gradient, vacuum electron linear accelerator
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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).
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Huang, Y.C.1
Zheng, D.2
Tulloch, W.M.3
Byer, R.L.4
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0000001493
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Proposed high-gradient laser-driven electron accelerator using crossed cylindrical laser focusing
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Y.C. Huang, R.L. Byer, "Proposed high-gradient laser-driven electron accelerator using crossed cylindrical laser focusing", Appl. Phys. Lett. 69,2175 (1996).
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Huang, Y.C.1
Byer, R.L.2
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4
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4444239860
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On the Classical Radiation of Accelerated Electrons
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J. Schwinger, "On the Classical Radiation of Accelerated Electrons", Phys. Rev. Vol. 75 12 1912 (1949).
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Schwinger, J.1
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5
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Limitations Imposed by Beam-Beam Effects and Their Remedies" to be published in the Int'l
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J.E. Spencer, "Limitations Imposed by Beam-Beam Effects and Their Remedies" to be published in the Int'l. Jrnl. Of Physics A (1998).
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Spencer, J.E.1
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6
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85032568772
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½ rather than n. The scattering in the forward direction is coherent but with a classical phase uncertainty
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½ rather than n. The scattering in the forward direction is coherent but with a classical phase uncertainty.
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7
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85032590901
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2/2 can be identified as the ponderomotive potential in the equivalent Hamiltonian for the electron in the laser field
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2/2 can be identified as the ponderomotive potential in the equivalent Hamiltonian for the electron in the laser field.
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8
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85032578480
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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
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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.
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