Александр Баланов

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1 Александр Баланов

a.balanov@lboro.ac.uk Collaborators M.T. Greenaway (University of Nottingham, UK) T.

Selskii (Saratov State University, Russia) A.

Khramov (Saratov State University, Russia) K.N.

Shorokhov (Mordovian State University, Russia) N.

2 Collaborators M.T. Greenaway (University of Nottingham, UK) T.M. Fromhold (University of Nottingham, UK) A.O. Selskii (Saratov State University, Russia) A.A. Koronovskii (Saratov State University, Russia) A.E. Khramov (Saratov State University, Russia) K.N. Alekseev (Loughborough University, UK) A.V. Shorokhov (Mordovian State University, Russia) N.N. Khvastunov (Mordovian State University, Russia) N. Alexeeva (Nottingham/Loughborough UK) A. Patanè (University of Nottingham, UK) O. Makarovsky (University of Nottingham, UK) M. Gaifullin (Loughborough University, UK) L. Eaves (University of Nottingham, UK) F.V. Kusmartsev (Loughborough University, UK)

3 SEMICONDUCTOR SUPERLATTICE Quantum well Period (10 s of atoms) Chain of quantum wells forms a 1D periodic structure similar to a crystal lattice But since the lattice period is much longer than for any natural crystal, this type of structure is known as a Superlattice

4 Drift velocity of electron, v d I~ v d Onset of Bloch oscillations localises electrons and reduces their drift velocity ef = E( p x dp dt x v = x ) = Δ(1 cos de dp x pxd ) v d 1 ( F) = vx ( t)exp( t / τ ) dt τ 0

5 THz applications of SL C.P. Edres et al, Rev. Sci. Instr (2007) Frequency multiplier in high-resolution THz spectroscopy (room temperature)

6 THz applications of SL P. Khosropanahet al, Opt. Lett. 34, 2958 (2009) Phase locking of a 2.7 THz quantum cascade laser SL at room T

7 THz applications of SL Y. Shimada et al, Phys. Rev. Lett (2003) absorption: S.A. Ktitorov, G.S. Simin, V.Ya. Sindalovskii, Sov. Phys. Solid State 13 (1971) THz emission under optical injection ( T~10K)

8 MODEL EQUATIONS I: F Electric field: F(-F, 0, 0) Magnetic field: B(BcosΘ, 0, BsinΘ) Dispersion relation: Δ pd 1 E p p x 2 2 ( p) = (1 cos ) + ( y + y) 2 2m Electron impulse: p(p x, p y, p x ) Balance equation: p = ef e( E B) p p = ef ω p tan Θ x y dδ pd x p y = m ω tan Θ sin( ) ω p 2 p = ω p z y z Cyclotron frequency: ω c = eb / m ω = ω cos Θ c

9 MODEL EQUATIONS II: 2 2 m ωc Δsin 2Θ d tan Θ pz + ω pz = sin( pz ωbt) 4 All other states can be expressed in terms of p z : p eft p p p 1 x = z tan Θ, y = ω z dδ dtan Θ p z x = sin( pz ωbt), y =, z = 2 m p z ω m

10 z Barriers ELECTRON ORBITS: θ = 0 o x B Orbit p 2 + ˆ ω p 2 m ωc Δ sin 2Θ d tan Θ = sin( z c z 4 F = 3.6 x 10 6 V m Cyclotron frequency -1 ~ B B = 11 T Bloch frequency ~ F p z ω t) b

11 ωb / ωccosθ n at most field values

12 Θ = 60 x x ωb / ωccosθ = n ~ F ~B i.e. at discrete field values

13 Chaotic electron s trajectory at cyclotron-bloch resonance ω / ω cos Θ = 1 b c

14 ELECTRON DRIFT VELOCITY v d 175 fs 1 ( F) = v ( t)exp( t / τ x ) dt τ 0 Onset of Bloch oscillations localises electrons and reduces their drift velocity Summation over all starting velocities y xb z

15 ELECTRON DRIFT VELOCITY v d 175 fs 1 ( F) = v ( t)exp( t / τ x ) dt τ 0 Summation over all starting velocities Fromhold et al., Phys. Rev. Lett. 87, (2001); Nature 428, 726 y (2004) Fowler et al., Phys. Rev. B. 76, (2007) 1 2 r = ω B /ω C cos θ Balanov et al., Phys. Rev. E. 77, x (2008) Related work on Ultrafast Fiske Effect by Kosevich et al., Phys. Rev. Lett. B 96, (2006) z θ

16 ELECTRON DRIFT VELOCITY v d 175 fs 1 ( F) = v ( t)exp( t / τ x ) dt τ 0 vsummation d (F) curves over were all used as a basis starting for velocities calculating I(V) by self-consistent solution y of 1 2 r = ω B /ω C cos θ Current continuity equation Poisson s equation x θ throughout the device z B

17 Semiclassical transport model Emitter SL Region Collector n + n 1 n 2 n m n N n + V F 0 F 1 F 2 F m F m+1 F N F N+1 Solve charge conservation equations dn m /dt = (J m J m+1 ) /e x, and Poisson equations F m+1 - F m = (n m - n D ) e x / ε 0 ε r self-consistently requiring sum of voltage drops = V Calculate current Current density J m = n m e v d (F m )+D(F m )(n m +1 -n m )/ x I ( t) A N = N +1 J m=0 m

18 Θ = 90 Θ = 90 Θ = 0 Θ = 0 Fromhold et al, Nature 428, 726 (2004)

19 y Theory z θ x B = 15 T θ = 40 o θ = 25 o θ = 0 o

20 Theory Unstable stationary solutions in very good agreement with DC experiments θ = 40 o θ = 25 o θ = 0 o

21 V = 490 mv, θ = 0 o Electron density (log scale) Collector Emitter Emitter Collector x

22 V = 490 mv, θ = 0 o Domains originate from negative differential velocity Esaki-Tsu peak Collector Emitter For reviews see, e.g., A. Wacker, Phys. Rep. 357, 1 (2002); L. Bonilla and H. Grahn, Rep. Prog. Phys , (2005); E. Schöll, Nonlinear Spatio-temporal Dynamics and Chaos in Semiconductors (CUP, 2001) Propagating domains can generate electromagnetic radiation at frequencies > 100 GHz [e.g. Schomberg, Renk et al., Appl. Phys. Lett. 74, 2179 (1999)]

23 V = 610 mv, θ = 40 o Electron density (Log scale) Collector Emitter Emitter Collector x

24 V = 610 mv, θ = 40 o θ = 40 o Collector Emitter When θ = 0 o, there is only one region of negative differential velocity But when θ = 40 o, there are 4 and each creates a charge domain

25 V = 610 mv, θ = 40 o Collector Eventually, the domains merge into one fast superdomain which creates a large I(t) peak when it arrives at the collector Emitter Let s now compare Fourier power spectra of I(t) for θ = 0 o and θ = 40 o

26 10 I (ma) o 0 V = 610t (ps) mv, θ = t (ps) 100 Fourier power (arb. units) Fourier power (arb. units) I (ma) V = 490 mv, θ = 0o Fundamental peak at 12 GHz dominates little power > 200 GHz x10 0 5th harmonic at 92 GHz dominates more power > 200 GHz f (THz)

27 10 I (ma) o 0 V = 610t (ps) mv, θ = t (ps) 100 Fourier power (arb. units) Fourier power (arb. units) I (ma) V = 490 mv, θ = 0o Vertical axes have same scale x10 0 x f (THz)

28 Effect of temperature on drift velocity of electrons v d Cyclotron frequencies, Maximal miniband velocity of electron Drift velocity for particular initial momentum P(P x, P y, P z ) ν = 1/ τ - scattering rate

29 Effect of temperature on drift velocity of electrons v d Drift velocity for particular initial momentum P(P x, P y, P z ) We assume the Boltzmann statistics for electron momenta Averaged drift velocity of electrons A. Selskii et al, in preparation

30 Effect of temperature on v d : analytical approach If F.G. Bass et al, JETP Letters 31, 314 (1980).

31 Effect of temperature on v d : analytical approach Solution!

32 Effect of temperature on v d : analytical approach - Bloch frequency

33 Effect of temperature on v d : analytical approach

34 Effect of temperature on v d : analytical approach

35 analytical approach vs numerical simulation for B=0 If there is no magnetic filed, B=0, the formula becomes exact. It coincides with one derived,e.g in Y.A. Romanov, Optika i Spektroskopiya 33, 917 (1972). maximal drift velocity solid lines analytics symbol numerical simulation

36 Effect of temperature on drift velocity of electrons analytics numerics 1-T=0 K 2-T=50 K 3-T=200 K 4-T=300 K 5- T=400 K B=15 T, =40 o (!) A. Selskii et al, (2011)

37 Effect of temperature on electric current: I-V curves A. Selskii et al, (2011)

38 Effect of temperature on electric current: frequency A. Selskii et al, (2011)

39 Effect of temperature on electric current: amplitude A. Selskii et al, (2011)

40 Conclusions A tilted magnetic field strongly affects, and can significantly enhance, the transport characteristics of SLs even at room temperature. Increasing T quickly suppresses the B = 0 Esaki-Tsu peak in the vd(f) curve, but has a much smaller effect when a tilted magnetic field is applied. Increasing T can enhance the drift velocity peaks caused by the Bloch-cyclotron resonances At the presence of magnetic field electrons demonstrate much higher mobility, which amplifies DC- and ACcomponents of the current through SL, and also improves its frequency characteristics.

41 Related systems Miniband electrons driven by an acoustic wave Greenaway et al., Phys. Rev. B 81, (2010) - Semiclassical predictions of very high NDV now supported by recent wavepacket and charge domain studies Ultracold atoms in an optical lattice with a tilted harmonic trap Scott et al., Phys. Rev. A. 66, (2002) - Intrinsically low scattering rates - Could using Bose-Fermi interactions to control scattering rate? [Ponomarev, Madroñero, Kolovsky, Buchleitner, Phys. Rev. Lett. 96, (2006)] Optical analogue Wilkinson & Fromhold, Optics Letters 28, 1034 (2003)

Controlling the harmonic conversion efficiency in semiconductor superlattices by interface roughness design

Controlling the harmonic conversion efficiency in semiconductor superlattices by interface roughness design Apostolos Apostolakis a), and Mauro F. Pereira b) Department of Condensed Matter Theory, Institute