Arūnas Krotkus Center for Physical Sciences & Technology, Vilnius, Lithuania

Transcription

1 Arūnas Krotkus Center for Physical Sciences & Technology, Vilnius, Lithuania

2 Introduction. THz optoelectronic devices. GaBiAs: technology and main physical characteristics. THz time-domain system based on GaBiAs components. THz burst generation by optical mixing. Conclusions. Other possible ultrafast applications of GaBiAs components.

3 Vilnius: Drs.: K. Bertulis, V. Pačebutas, R. Adomavičius. PhD students: G. Molis, A. Bičiūnas. Stockholm: Prof. S. Marcinkevičius Berkeley: Prof. W. Walukiewicz, Dr. K.M. Yu. Lithuanian Science & Study Foundation. Lithuanian Science Council.

4 X Ray Visible Terahertz Infrared Millimetre Ultraviolet Microwave and Radio penetrating spectroscopy Non-ionising penetrating Key properties: Penetrates clothing, leather, paper, plastics, packaging materials. Materials identification using characteristic Terahertz spectra. 3-D imaging capability. Non-ionizing - no damage to body or cells Short wavelength high resolution

5 dc bias fs laser pulse thin SC layer THz output Optical pulse Optical pulse Photocurrent Photocurrent THz pulse 0,0 0,5 1,0 1,5 2,0 time (ps) THz pulse 0,0 0,5 1,0 1,5 2,0 time (ps) Biased photoconductor made from a material sensitive in the fs laser wavelength range; Contact metallization has the shape of a Hertzian dipole type antenna; THz pulse is emitted into free space. j em ( t) P( t) n ( t) qv( t) em E THz ( t) dj em dt ( t)

6 thin SC layer Photocurrent THz input fs laser pulse Delay time, ps Electro-optical and photoconductive detection; Photoconductor made from material with ultrashort carrier lifetime is biased by the incoming THz pulse; By illuminating it at different time delays, different parts of THz pulse are sampled;

7 thin SC layer Photocurrent 0.50 THz input fs laser pulse Delay time, ps Electro-optical and photoconductive detection; Photoconductor made from material with ultrashort carrier lifetime is biased by the incoming THz pulse; By illuminating it at different time delays, different parts of THz pulse are sampled;

8 thin SC layer 1.00 Photocurrent 0.75 THz input fs laser pulse Electro-optical and photoconductive detection; Photoconductor made from material with ultrashort carrier lifetime is biased by the incoming THz pulse; By illuminating it at different time delays, different parts of THz pulse are sampled; Critical material parameter carrier lifetime Delay time, ps

9 Femtosecond laser Polarizing beamsplitter Lock-in amplifier Si lens Step motor driver THz emitter THz detector PC 9

10 THz field amplitude, a.u Delay time, ps Power, a.u Frequency, THz Ultrafast electrical transients generated using femtosecond laser pulses; Their Fast-Fourier transform spectrum is shown on the right; Signal-to-noise ratios better than 60 db easily achievable; Coherent detection both amplitude and phase of different frequency components can be measured.

11 P 1, λ 1 P 2, λ 2 tunable GaAs lasers nm (380 THz) photomixer on Si lens THz I photo Superposition Intensity

12 Energy bandgap semiconductor should be photosensitive at the laser wavelength. THz pulse emitters: dark resistance, electron mobility, breakdown field, lifetime (shorter that the laser pulse repetition period). THz pulse detectors: electron trapping time, electron mobility, dark resistance. Optical mixers: electron and hole trapping times, dark resistance.

13 Advantages: * Mature laser technology ( nm); * LTG GaAs material sub-ps lifetimes, high resistivity, electron mobility, and with energy bandgap matching the laser photon energy. Disadvantages: * Complex optical pumping scheme; * Cannot be made much smaller and cheaper. Diode laser bar =808 nm Nd:YAG laser =1064 nm 2 harmonics =532 nm Ti:sapphire =800 nm

14 Advantages: 1 m or 1.55 m wavelength range solid-state or fiber laser are already commercially available; Directly pumped by diode laser bars; Compact, efficient, cheaper. Disadvantages: Semiconductor material similar to LTG GaAs but sensitive to longer wavelengths required; Longer wavelength means narrower energy bandgap and smaller dark resistivities. Diode laser bar KLM laser

15 In x Ga 1-x As: LTG (at 200 o C) on GaAs. x=0.25 ( ~1.05 m); dark resistivity cm, lifetime ~7 ps. LTG (at 180 o C) on InP substrates. x=0.53 ( ~1.5 m): free electron density >10 18 cm -3, lifetime ~2 ps; LTG, Be-doped. x=0.53 ( ~1.5 m): free electron density cm -3, lifetime ~2 ps; heavy ion implanted (Au +, Br +, or Fe + ): dark resistivity < 10 cm, electron lifetimes ps. GaSb x As 1-x : LTG (at 170 o C) on GaAs substrates. x=0.4 ( ~1.4 m): dark resistivity ~ 10 4 cm.

16 In 0.53 Ga 0.47 As ErAs islands Be doping InGaAs photoconductive layer; Be- doping for compensation of the residual donors; InAlAs LTG electron trapping layer. B. Sartorius, Opt.Expr., 16, 9565 (2008) InGaAs photoconductive layer; Be- doping for compensation of the residual donors; ErAs electron trapping nanoclusters. F. Ospald, APL., 92, (2008)

17 Low-temperature MBE grown GaAs; heavy ion implanted GaAs for ultrafast optoelectronic applications; Search of a short-lifetime material with a low mismatch to GaAs Papers from T. Tiedje and Kyoto groups on GaBi x As 1-x grown by MBE. x=3.1% (S.Tixier et.al, APL) and x=4.5% (M. Yoshimoto et.al., Jpn.J. Appl. Phys.). Growth temperatures were 380 o C and 350 o C, respectively Starting MBE growth at even lower substrate temperatures o C.

18 g, ev 1,5 1,4 1,3 1,2 1,1 1,0 0,9 0,8 0,7 0,6 0, T growth, o C Bandgap versus the growth temperature for 30 GaBiAs growth runs x Soviet made MBE machine (ШТАТ). As 4 source. x=5 % (K. Bertulis et.al. APL,2006). x=8.5% (V. Pacebutas et.al., Sem.Sc.Technol., 2007). x=11 % (V. Pacebutas et.al., J. Mater,Sc.., 2008)

19 Rutherford Back-Scattering. W. Walukiewicz, Lawrence Livermore Nat. Lab. X-ray diffraction.

20 Absorption coefficeient, cm -1 5x10 4 4x10 4 3x10 4 2x10 4 1x Wavelength, nm Bi9 Bi13 Bi14 Photoconductivity, a.u. 1,0 0,8 0,6 0,4 0,2 0, Wavelength, nm GaBi9 GaBi10 GaBi12 Optical absorption spectra at room temperature. Photoconductivity spectra at room temperature.

21 R/R, T/T (a.u.) GaBiAs #36A 300 K T/T R/R a) g E g = ev ± 3meV = 103mev ± 3meV E g = ev ± 3meV = 120 mev ± 3meV 0,8 0,9 1,0 1,1 1,2 Energy (ev) Exp. Fit R/R, T/T (a.u.) 1,0 0,5 0,0-0,5 GaBiAs #35A 300 K E g = ev ± 3meV = 94mev ± 3meV T/T R/R b) E g = ev ± 4 mev = 78 mev ± 4meV 0,8 0,9 1,0 1,1 1,2 Energy (ev) Photomodulated transmittance ( T/T) and photomodulated reflectance ( R/R) spectra for two GaBiAs samples measured at room temperature.

22 GaBiAs-9, PL (473 nm), 300K PL intensity, a.u. 1,0 0,8 0,6 0,4 0,2 T g =330 o C T g =280 o C Intensity (arb. u.) non-annealed 400 C 500 C 600 C Lazerio linija 0, Wavelength nm -1 0,8 0,9 1,0 1,1 1,2 1,3 1,4 Energy (ev) GaBiAs layers with the carrier lifetime shorter than 10 ps. PL measured by frequency upconversion, single-photon counting technique. GaBiAs layer with a long carrier lifetime (~200 ps non-annealed). PL measured by a standard cw technique. Complex annealing behavior. Prof. S. Marcinkevičius lab., KTH, Stockholm.

23 Bandgap, ev 1,5 1,4 1,3 1,2 1,1 1,0 0,9 0,8 0,7 1,05 m 1,3 m 1,55 m GaBi part, % With the addition of Bi, the energy bandgap decreases at a rate of -62 mev/%bi. Other material parameters: Conductivity p-type. Hole concentration ~10 15 cm -3, Hole mobility cm 2 /Vs (decreasing in layers with a larger GaBi part). Resistivity typically 100 s of cm for nominally undoped layers; >10 4 cm in Si-compensated GaBiAs. V. Pacebutas et.al., Sem.Sc.Technol., 2007

24 Optical pump THz probe experiment. THz pulse absorption caused by nonequilibrium electrons is measured at different time delays with respect to the sample photoexcitation. Optically induced change in THz pulse transmittance is proportional to ln(i/i 0 )=- i L=- (4 n i /l 0 )L~ dc ~N Both the electron mobility and their lifetime can be determined.

25 4 3,5 3,0 A B C T THz, a.u mw 200 mw, ps 2,5 2,0 1, mw 1, Delay, ps P o, mw Lifetime varies from less than 1 ps to more than 200 ps. Electron mobility as determined from the amplitude of the induced THz absorption >2000 cm 2 /Vs. Electron lifetime is dependent on the photoexcitation level. Trap filling effect. Best fit with a single trap model obtained for the capture cross-section of cm 2 and the trap density of cm -3 (sample A) and cm -3 (samples B and C). V. Pačebutas et.al., pss(c), (2009)

26 The main carrier trapping center in LTG GaAs. Electron capture cross-section by As Ga in GaAs cm 2 A. Krotkus et.al. IEE Proc. Optoelectron., In LTG GaAs the lifetime increases after annealing because the majority of the excess As atoms precipitate into nm size clusters. As-antisite. Point defect leading to a deep level in the band gap. M.Kaminska, E.Weber, (1990)

27 GaBiAs-9, PL (473 nm), 300K Intensity (arb. u.) non-annealed 400 C 500 C 600 C Lazerio linija T/T. a.u o C 500 o C 400 o C non-annealed 0 0,1-1 0,8 0,9 1,0 1,1 1,2 1,3 1,4 Energy (ev) Delay, ps Photoluminescence in GaBiAs layer with a long carrier lifetime (~200 ps non-annealed). PL measured by a standard cw technique. Complex annealing behavior. Additional PL band at ~1.3 m (Biclusters?) THz probe measurement. Lifetime in as-grown layer is ~200 ps, it slightly increases after anneal at 400 and 500 o C, and drops to <30 ps at T=600 o C.

28 1,00 SI GaAs Au GaBiAs THz field amplitude, a.u. 0,75 0,50 0,25 0,00-0,25 GaBi InGaAs L Delay, ps The width of the gap 15 m. Detected THz pulse amplitude is 5 times and S/N ratio 100 times larger than when detector made from LTG InGaAs layer is used. THz emitter is p-type InAs. Power GaBi InGaAs L-1 G. Molis et.al., Electron. Lett. 43, (2007) Frequency, THz

29 SI GaAs Au GaBiAs The geometry of the antenna is similar to one used for THz detectors, except for mesaetching of GaBiAs layer area between the microstriplines. GaBiAs doping with Si used for residual p-type conduction compensation. Dark resistance of the emitter >100 M. Breakdown field larger than 50 kv/cm.

30 A Golay Cell is a type of detector mainly used for FIR spectroscopy. It consists of a small metal cylinder which is closed by a blackened metal plate at one end and by a flexible metalized diaphragm at the other. The cylinder is filled with Xe and then sealed. Measurements of THz power as functions of the bias voltage and the optical power. Optical-to-THz conversion efficiency obtained was up to , much better than ~10-5 reached with other similar systems mW 20mW 30mW THz power, W GaBi 24B 2d U, V

31 The Yb:fiber oscillator operated at a repetition rate of 45 MHz; an average output power of ~8 mw and ~11 mw was used for photoexcitation of the THz emitter and detector respectively. 20 db-bandwidth of THz-TDS system as a function of the optical pulse duration. Solid lines calculations for different carrier lifetimes in the detector.

32 Power, a.u Dry N 2 Power, a.u Ambient air Frequency, THz Frequency, THz Yb:KGW laser, 1030 nm, 70 fs. Spectral width ~5 THz, S/N ratio ~70 db. Average fs laser power of ~ 10 mw is sufficient for activating both the emitter and the detector.

33 Fs laser pulse Stretched chirped pulse Splitting in two equal parts f THz radiation Photoconductive antenna f 0 t Variable delay between two parts t

34

35 0,0010 t=1,8 ps, f=0,26 THz 1E-8 THz field amplitude 0,0005 0,0000-0,0005 Power, a.u. 1E-9 1E-10-0,0010 THz field amplitude 0,0006 0,0004 0,0002 0,0000-0,0002-0, Delay, ps -0, Delay, ps 0.6 THz 1E-11 0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6 1,8 2,0 f. THz Emitter Hertzian dipole, length 70 m, resonance ~0.5 THz. Yb:KGW laser pulses stretched to 30 ps, average optical power in both arms 25 mw, bias voltage 30 V. Maximum frequency observed 1.3 THz.

36 T 1,8 1,6 1, µj µj µj 0.53 µj 0.53i0.274 GW/cm i0.274 GW/cm i0.249 GW/cm i0.249 GW/cm 2 1,2 1, p- GaBiAs SI-GaAs Uni-travelling carrier photodiode. Response time limited by the electron sweep-out through the collection layer. Bandwidths >1THz demonstrated. z/z 0 Open aperture Z-scan measurement. Large optical bleaching effect with relatively low saturation intensity. Possible applications in saturable absorbers for mode-locked lasers and all-optical switches.

37 Dilute GaBiAs due to its large electron mobility in a material with sub-picosecond carrier lifetimes is a prospective material for ultrafast optoelectronic application in the wavelength range of from 1 m to 1.5 m. THz time-domain-spectroscopy system with components manufactured from GaBiAs and activated by femtosecond pulses of compact 1-mm wavelength laser was demonstrated. This material shows great prospects in other ultrafast device applications, such as cw THz optical mixers, semiconducting saturable absorbers, and all-optical switches.