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Refresher on Smith-Purcell parameters

λ = l

n

⎛ 1 ⎞

− cosθ

⎝

⎜

β ⎠

⎟ θ

• n = order number, θ = angle from electron beam,

φ = azimuthal angle

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Refresher on Smith-Purcell parameters λ = l n ⎛ 1 ⎞ − cosθ ⎝ ⎜ β ⎠ ⎟ θ • n = order number, θ = angle from electron beam, φ = azimuthal angle φ

Angular power (nW/steradian) 160 140 120 100 80 60 40 20 Spontaneous azimuthal power -1 order -3 order -2 order 0 0 20 40 60 80 100 Azimuthal angle (degrees) θ = 90°

Page 1 and 2: Progress on the Vanderbilt Table To
Page 3 and 4: WANTED: a narrowband THz source for
Page 5 and 6: Examine protein secondary structure
Page 7 and 8: How this compares to other THz sour
Page 9 and 10: Experimental apparatus
Page 11 and 12: Needle cathode e-beam has high brig
Page 13 and 14: Dimensions of the aluminum grating
Page 15 and 16: • Evanescent wave: Details of las
Page 17 and 18: Amplitude growth rate, µ (m -1 ) 6
Page 19: Net gain (m -1 ) 200 150 100 50 Net
Page 23 and 24: We will conduct the following exper

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