Part III. Interaction with Single Electrons - Plane Wave Orbits

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Oswald Daniels
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1 Part III - Orbits 52 / 115

2 3 Motion of an Electron in an Electromagnetic 53 / 115

3 Single electron motion in EM plane wave Electron momentum in electromagnetic wave with fields E and B given by Lorentz equation (cgs units): dp dt = e(e + 1 v B), (22) c 54 / 115

4 Single electron motion in EM plane wave Electron momentum in electromagnetic wave with fields E and B given by Lorentz equation (cgs units): dp dt = e(e + 1 v B), (22) c Energy equation (taking dot product of v with Eq. (22)) d ( γmc 2 ) = e(v E), (23) dt where p = γmv, and γ = (1 + p 2 /m 2 c 2 ) 1 2 factor. is the relativistic 55 / 115

5 Electromagnetic plane wave Consider elliptically polarized plane-wave A(ω, k) travelling in the positive x-direction. Vector potential A = (0, δa 0 cos φ, (1 δ 2 ) 1 2 a0 sin φ), (24) where φ = ωt kx is the phase of the wave; a 0 is the normalized amplitude (v os /c) 56 / 115

6 Electromagnetic plane wave Consider elliptically polarized plane-wave A(ω, k) travelling in the positive x-direction. Vector potential A = (0, δa 0 cos φ, (1 δ 2 ) 1 2 a0 sin φ), (24) where φ = ωt kx is the phase of the wave; a 0 is the normalized amplitude (v os /c) Polarization parameter δ: δ = {±1, 0} linearly polarized wave δ = ±1/ 2 circular wave. 57 / 115

7 Normalized (dimensionless) units t ωt x kx v v/c p p/mc A ea/mc 2 E ee/mωc B eb/mωc Equivalent to setting ω = k = c = e = m = 1 (cf. atomic units) 58 / 115

8 Perpendicular (canonical) momentum Using the relations and E = A/ t B = A = (0, A z / x, A y / x) the perpendicular component of momentum Eq. (22) becomes: dp dt = A t + v A x x, 59 / 115

9 Perpendicular (canonical) momentum Using the relations and E = A/ t B = A = (0, A z / x, A y / x) the perpendicular component of momentum Eq. (22) becomes: dp dt = A t + v A x x, which after integrating gives canonical momentum: where p 0 is a constant of motion. p A = p 0, (25) 60 / 115

10 Longitudinal momentum The longitudinal components of Eq. (22) and Eq. (23) yield a pair of equations which can be subtracted from each other thus: dp x dt dγ ( dt = v Ay y + A ) ( y Az v z + A ) z. t x t x Because the EM wave is a function of t x only, the terms on the RHS vanish identically, so we can immediately integrate the RHS to get: γ p x = α, where α is a constant of motion still to be determined. 61 / 115

11 General solution Use identity γ 2 p 2 x p 2 = 1 and choose p 0 = 0 to get relationship between the parallel and perpendicular momenta: independent of polarization δ. p x = 1 α2 + p 2. (26) 2α 62 / 115

12 Change of variables: wave phase Need to specify α and integrate Eq. (25) and Eq. (26). This is simplified by changing variables. Noting that dφ dt = φ t + p x φ γ x = α γ, we have p = γ dr dt = γ dφ dr dt dφ = α dr dφ. (27) 63 / 115

13 Special cases: (1) laboratory Lab : the electron initially at rest before the EM wave arrives, so that at t = 0, p x = p y = 0 and γ = 1. From Eq. (26) it follows that α = / 115

14 Special cases: (1) laboratory Lab : the electron initially at rest before the EM wave arrives, so that at t = 0, p x = p y = 0 and γ = 1. From Eq. (26) it follows that α = 1. This leads to the following expression for the momenta in the lab : p x = a2 [ (2δ 2 1) cos 2φ ], 4 p y = δa 0 cos φ, (28) p z = (1 δ 2 ) 1/2 a 0 sin φ. 65 / 115

15 : solution With Eq. (27) we can integrate expressions Eqs. (28a 28c) to obtain the lab- orbits valid for arbitrary polarization δ: x = 1 [ ] 4 a2 0 φ + 2δ2 1 sin 2φ, 2 y = δa 0 sin φ, (29) z = (1 δ 2 ) 1/2 a 0 cos φ. NB: solution is self-similar in the variables (x/a 2 0, y/a 0) 66 / 115

16 : linearly polarized wave (δ = 1) ky a 0 =0.3 a 0 =1.0 a 0 = /8 /4 3 /8 /2 2 kx/a 0 Figure: For a 1 µm laser wavelength, the pump strengths a 0 correspond roughly to intensities of 10 17, and Wcm 2 respectively. 67 / 115

17 : drift velocity Longitudinal motion has a secular component which will grow in time or with propagation distance. Electron starts to drift with an average momentum corresponding to a velocity: p D p x = a2 0 4 v D c = v x = p x γ = a a0 2, (30) where the overscore denotes averaging over the rapidly varying EM phase φ. 68 / 115

18 : circularly polarized light (δ = ±1/ 2) Longitudinal oscillating component at 2φ vanishes identically Transverse motion is circular with radius a 0 and momentum p = a 0 / 2. Combines with the linear drift in Eq. (30) to give a helical orbit with pitch angle θ p = p /p D = 8a 1 0. (31) 69 / 115

19 Special cases: (2) Require drift velocity to vanish: p x = 0 in Eq. (26), then: 1 + A 2 α 2 = 0. Average over a laser cycle to remove rapidly varying terms, and noting that cos 2 φ = 1/2 gives: α = ( ) 1/2 1 + a2 0 γ 0. (32) 2 70 / 115

20 Rest : solution Plugging α from Eq. (32) back into Eq. (26) gives the momenta: p x = ( 2δ 2 1 ) a0 2 cos 2φ, 4γ 0 p y = δa 0 cos φ, (33) p z = (1 δ 2 ) 1 2 a0 sin φ. Noting that in this case, p = γ 0 dr/dφ, we can integrate again to get the orbits: ( x = δ 2 1 ) q 2 sin 2φ, 2 where q = a 0 /2γ 0. r = 2(δq sin φ, (1 δ 2 ) 1 2 q cos φ), (34) 71 / 115

21 Rest : linearly polarized wave (δ = 1) Eliminate φ for linear polarization (δ = 1), to obtain figure-of-eight orbit x 2 = y 2 (4q 2 y 2 ). (35) ky kx 72 / 115

22 Rest : limits Extreme intensity limit, a 0 1: γ 0 a 0 / 2 q 1/ 2 fat-8 orbit with x max = 1/4, y max = 2. Circularly polarized light: δ = ±1/ 2; p x = 0 circle with radius. a 0 2γ0 73 / 115

23 Adiabatic approximation: df /dt ωf. Example f (t) = sin(πt/2t L ), with ωt L = 600/π. p y y t t A(x, t) = a 0 f (t) cos φ, (36) p x x t t 74 / 115

24 force Single electron oscillating slightly off-centre of focused laser beam: y x laser I(r) E (r) y f p e After 1st quarter-cycle, sees lower field Doesn t quite return to initial position Accelerated away from axis 75 / 115

25 force: non-relativistic In the limit v/c 1, the equation of motion (22) for the electron becomes: v y t = e m E y (r). (37) Taylor expanding electric field: E y (r) E 0 (y) cos φ + y E 0(y) y cos φ +..., where φ = ωt kx as before. To lowest order, we therefore have where v os = ee L /mω. v y (1) = v os sin φ; y (1) = v os cos φ, ω 76 / 115

26 force: non-relativistic (contd.) Substituting back into Eq. (37) gives v (2) y t = e2 m 2 ω 2 E E 0 (y) 0 cos 2 φ. y Multiplying by m and taking the cycle-average yields the ponderomotive force on the electron: f p m v (2) y t = e2 4mω 2 E 2 0 y. (38) 77 / 115

27 force: relativistic Lorentz equation (22) in terms of the vector potential A: p t + (v. )p = e A c t e v A. (39) c Separate the timescales of the electron motion into slow and fast components p = p s + p f and average over a laser cycle, f p = dps dt = mc 2 γ, (40) ( 1/2. where γ = 1 + p2 s m 2 c ) a2 78 / 115

28 : electron motion in plane wave Linear polarisation ky a 0 =0.3 a 0 =1.0 a 0 =3.0 Solution in terms of wave phase φ = ωt kx: x = 1 4 a2 0 (φ + 12 ) sin 2φ, y = a 0 sin φ Drift velocity: -3 0 /8 /4 3 /8 /2 2 kx/a 0 v D c = a a / 115

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