超快光学第02章概述ppt课件.ppt

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1、The Generation of Ultrashort Laser Pulses,The importance of bandwidthMore than just a light bulbLasers, laser modes, and mode-lockingMaking shorter and shorter pulsesPulse-pumpingQ-switching and distributed-feedback lasersPassive mode-locking and the saturable absorberKerr-lensing and Ti:SapphireAct

2、ive mode-lockingOther mode-locking techniquesLimiting factorsCommercial lasers,Prof. Rick TrebinoGeorgia Techwww.frog.gatech.edu,But first: the progress has been amazing!,The shortest pulse vs. year (for different media),Continuous vs. ultrashort pulses of light,A constant and a delta-function are a

3、 Fourier-Transform pair.,Continuous beam:Ultrashort pulse:,Irradiance vs. time,Spectrum,time,time,frequency,frequency,Long vs. short pulses of light,The uncertainty principle says that the product of the temporal and spectral pulse widths is greater than 1.,Long pulse,Short pulse,Irradiance vs. time

4、,Spectrum,time,time,frequency,frequency,For many years, dyes have been the broadband media that have generated ultrashort laser pulses.,Ultrafast solid-state laser media have recently replaced dyes in most labs.,Solid-state laser media have broad bandwidths and are convenient.,But a light bulb is al

5、so broadband. What exactly is required to make an ultrashort pulse?Answer: A Mode-locked LaserOkay, whats a laser, what are modes, and what does it mean to lock them?,Light bulbs, lasers, and ultrashort pulses,Stimulated emission leads to a chain reaction and laser emission.,Excited medium,If many m

6、olecules in a medium are excited, one photon can become many.,This is the essence of the laser. The factor by which an input beam is amplified by a medium is called the gain and is represented by G.,Usually, additional losses in intensity occur, such as absorption, scat-tering, and reflections. In g

7、eneral, the laser will lase if, in a round trip: Total Gain Total Loss This called achieving Threshold.,The Laser,A laser is a medium that stores energy, surrounded by two mirrors.The output mirror is partially reflecting and so lets some light out.,A laser will lase if the beam increases in intensi

8、ty during a round trip:that is, if .,in the form of excited states,Calculating the Gain:Einstein A and B Coefficients,In 1916, Einstein considered the various transition rates between molecular states (say, 1 and 2) involving light of irradiance, I: Absorption rate = B N1 I Spontaneous emission rate

9、 = A N2 Stimulated emission rate = B N2 I,where Ni is the number density of molecules in the ith state, and I is the irradiance.,Laser Gain,Neglecting spontaneous emission:,Stimulated emission minus absorption,Proportionality constant is the absorption/gain cross-section, s,If N2 N1:,If N2 N1 :,Ther

10、e can be exponential gain or loss in irradiance. Normally, N2 N1, theres gain, and we define the gain, G:,The solution is:,g and a are the gain and absorption coefficients.,I = I(z-ct),Inversion,In order to achieve G 1, stimulated emission must exceed absorption:,Energy,Inversion,“Negative temperatu

11、re”,B N2 I B N1 I,Here, there is inversion from level 4 to levels 3 and 2.,4,In order to achieve inversion, we must hit the laser medium very hard in some way and choose our medium correctly.,This condition is called inversion. It does not occur naturally (its forbidden by the Boltzmann distribution

12、). Its inherently a non-equilibrium state.,Canceling the BI factors, N2 N1, or:,Achieving Inversion: Pumping the Laser Medium,Now let Ip be the intensity of (flash lamp) light used to pump energy into the laser medium:,Ip,Will this intensity be sufficient to achieve inversion, N2 N1?Itll depend on t

13、he laser mediums energy level system.,Output mirror,Back mirror,Laser medium,Rate Equations for a Two-Level System,Rate equations for the densities of the two states:,Absorption,Stimulated emission,Spontaneous emission,If the total number of molecules is N:,Pump,Pump intensity,Why Inversion is Impos

14、sible in a Two-Level System,In steady-state:,where:,DN is always positive, no matter how high Ip is! Its impossible to achieve an inversion in a two-level system!,Isat is the saturation intensity.,Rate Equations for a Three-Level System,Assume we pump to a state 3 that rapidly decays to level 2elimi

15、nating pump stimulated emission!,Absorption,Spontaneous emission,The total number of molecules is N:,Level 3 decays fast and so is zero.,Why Inversion is Possible in a Three-Level System,In steady-state:,Now if Ip Isat, DN is negative!,Rate Equations for a Four-Level System,Now assume the lower lase

16、r level 1 also rapidly decays to a ground level 0.So also! And,As before:,Because,The total number of molecules is N :,At steady state:,Why Inversion is Easy in a Four-Level System (contd),Now, DN is negativealways!,Two-, Three-, and Four-Level Systems,Two-level system,Laser Transition,Pump Transiti

17、on,At best, you get equal populations. No lasing.,It took laser physicists a while to realize that four-level systems are best.,Four-level system,Lasing is easy!,Fast decay,Fast decay,Three-level system,If you hit it very hard, it lases.,Fast decay,What about the saturation intensity?,A is the excit

18、ed-state relaxation rate: 1/t,B is the absorption cross-section, s, divided by the energy per photon, w: s / w,The saturation intensity plays a key role in lasers. For example, when the intensity approaches (or exceeds) it, the medium becomes less absorbing (N1 decreases).,Both s and t depend on the

19、 molecule, the frequency, and the various states involved.,w 10-19 J for visible/near IR light,t 10-12 to 10-8 s for most molecules 10-9 to 10-3 s for laser molecules,s 10-20 to 10-16 cm2 for molecules (on resonance),1 to 1013 W/cm2,A dyes energy levels,Dyes are big molecules, and they have complex

20、energy level structure.,S0: Ground electronic state,S1: 1st excited electronic state,S2: 2nd excited electronic state,Energy,Laser Transition,Lowest vibrational and rotational level of this electronic “manifold”,Excited vibrational and rotational level,Dyes can lase into any (or all!) of the vibrati

21、onal/rotational levels of the S0 state, and so can lase very broadband.,Pump Transition,Lasers emit trains of identical pulses.,where I(t) represents a single pulse intensity vs. time and T is the time between pulses.,Every time the laser pulse hits the output mirror, some of it emerges.,The output

22、of a typical ultrafast laser is a train of identical very short pulses:,R = 100%,R 100%,Output mirror,Back mirror,Laser medium,The Shah Function,The Shah function, III(t), is an infinitely long train of equally spaced delta-functions.,The Fourier Transform of the Shah Function,If w = 2np, where n is

23、 an integer, the sum diverges; otherwise, cancellation occurs.,III(t),So:,The Shah Function and a Pulse Train,where f(t) is the shape of each pulse and T is the time between pulses.,To do the integral, set: t/T = m or t = mT,But E(t) can also can be written:,An infinite train of identical pulses can

24、 be written:,Proof:,QED,An infinite train of identical pulses can be written:,The Fourier Transform of an Infinite Train of Pulses,The spacing between frequencies (modes) is then dw = 2p/T or dn = 1/T.,The Convolution Theorem says that the Fourier Transform of a convolution is the product of the Fou

25、rier Transforms. So:,E(t) = III(t/T) * f(t),The Fourier Transform of a Finite Pulse Train,A finite train of identical pulses can be written:,where g(t) is a finite-width envelope over the pulse train.,Use the fact that the Fourier transform of a product is a convolution.,A lasers frequencies are oft

26、en called longitudinal modes.Theyre separated by 1/T = c/2L, where L is the length of the laser.Which modes lase depends on the gain and loss profiles.,Frequency,Intensity,Here, additional narrowband filtering has yielded a single mode.,Actual Laser Modes,Mode-locked vs. non-mode-locked light,Mode-l

27、ocked pulse train:,Non-mode-locked pulse train:,Random phase for each mode,A train of short pulses,A mess,Generating short pulses = Mode-locking,Locking vs. not locking the phases of the laser modes (frequencies),Intensity vs. time,Intensity vs. time,Locked modes,Intensities,Numerical simulation of

28、mode-locking,Ultrafast lasers often have thousands of modes.,A generic ultrashort-pulse laser,A generic ultrafast laser has a broadband gain medium, a pulse-shortening device, and two mirrors (among other stuff):,Many pulse-shortening devices have been proposed and used.,Output pulse,R = 100%,R 100%

29、,Laser medium,Pump power,Pulse-shortening device,Pulsed pumping: ms pulses,Long and potentially complex pulse,Pumping a laser medium with a short-pulse flash lamp yields a fairly short pulse. Flash lamp pulses as short as 1 s exist.Unfortunately, this yields a pulse as long as the excited-state life

30、time of the laser medium, which can be considerably longer than the pump pulse.Since solid-state laser media have lifetimes in the microsecond range, it yields pulses microseconds to milliseconds long.,I(t),Q-switching: ns pulses,Q-switching involves:Preventing the laser from lasing (by adding massi

31、ve loss) until the flash lamp is finished flashing, andAbruptly allowing the laser to lase.,The pulse length is limited by how fast we can switch and the round-trip time of the laser and yields pulses 10 - 100 ns long.,100%,0%,Time,Cavity Loss,Cavity Gain,Output pulse intensity,Gain saturation,Q-Swi

32、tching,How do we Q-switch a laser? Q-switching involves preventing lasing until were ready.A Pockels cell switches (in a few nanoseconds) from a quarter-wave plate to nothing.,Before switching,After switching,Pockels cell as wave plate w/ axes at 45,0 Polarizer,Mirror,Pockels cell as an isotropic me

33、dium,0 Polarizer,Mirror,Polarization becomes circular on the first pass and then horizontal on the next and is then rejected by the polarizer.,Polarization is unaffected by the Pockels cell and hence is passed by the polarizer.,The saturable absorber,Like a sponge, an absorbing medium can only absor

34、b so much. High-intensity spikes burn through; low-intensity light is absorbed. The absorption coefficient vs. input intensity:,0,where:,for a 2-level system,The Effect of a Saturable Absorber,First, imagine raster-scanning the pulse vs. time like this, where k indicates the round-trip number:,After

35、 many round trips, even a slightly saturable absorber can yield a very short pulse.,Intensity,Round trips (k),Notice that the weak pulses are suppressed, and the strongest one is amplified (by the laser gain).,And the strong pulse shortens!,Alas, most absorbers recover slowly,T,Passive mode-locking

36、with a slow saturable absorber,What if the absorber responds slowly (more slowly than the pulse)?Then only the leading edge will experience pulse shortening.,This is the most common situation, unless the pulse is many ps long.,Gain saturation shortens the pulse trailing edge.,The intense spike uses

37、up the laser gain-medium energy, reducing the gain available for the trailing edge of the pulse (and for later pulses).,The gain saturates, too. This is good.,While saturable absorption shortens the leading edge, of the price, saturable gain shortens the trailing edge.,Amplifying the pulse uses up t

38、he stored energy and hence reduces the gain.,Initial unsaturated loss,gain loss,gain loss,gain loss,Initial unsaturated gain,time,Laser pulse intensity,Saturated gain and loss,The Passively Mode-locked Dye Laser,Passively mode-locked dye lasers yield pulses as short as a few hundred fs.Theyre limite

39、d by our ability to saturate the absorber.,Some common dyes and their corresponding saturable absorbers,Colliding pulses have a higher peak intensity.,And higher intensity in the saturable absorber generates shorter pulses. This is called Colliding-Pulse Mode-locking (CPM).,The colliding-pulse mode-

40、locked (CPM) laser,A Sagnac interferometer is ideal for creating colliding pulses.,CPM dye lasers produce even shorter pulses: 30 fs.,Passive Mode-Locking Using a Mediums Nonlinear Refractive Index,Just as absorption varies with intensity (a a0 a2I ), a mediums other optical characteristic, the refr

41、active index, n, will also change with intensity:,This is called the optical Kerr effect.The nonlinear refractive index can be made to act like a saturable absorber.,L(x),A Lens and a Lens,A lens is a lens because the phase delay seen by a beam varies quadratically with x:,Now let L be constant, but

42、 let n vary quadratically with x:,n(x),In both cases, a quadratic variation of the phase with x yields a lens.,Laser beam,f(x) = n k L(x),f(x) = n(x) k L,Here, the lens thickness varies quadratically with x.,L(x) L0 (1- x2/a2),n(x) n0 (1- x2/a2),Kerr-Lensing,A laser beam has an approximately quadrat

43、ic intensity near its center, so an intense beam can induce a lens via the nonlinear refractive index.,Solid,Low intensity:,High intensity:,I0 exp(- x2/w2) I0 (1- x2/w2),f(x) = n(x) k L n0 + n2 I0 (1- x2/w2) k L,Nothing happens.,Beam focuses!,Kerr-Lens Mode-Locking,Kerr-lensing is the mode-locking m

44、echanism of the Titanium:Sapphire (Ti:Sapph) laser. Ti:Sapph not only lases, but it has a large n2!,Losses are zero for a high-intensity fs pulse.,Large n2,Placing an aperture at the focus favors a short pulse:,Losses are too high for a low-intensity pulse to lase.,Large n2,Low intensity:,High inten

45、sity:,Large n2,Modeling Kerr-lens mode-locking,The gain region acts as the aperture.,We align the laser for the extra focusing due to the Kerr effect at high intensity, so a high-intensity pulse will have better overlap with the gain medium than a low-intensity pulse.,High-intensity pulse,Low-intens

46、ity pulse,Ti:Sapph,Kerr-lensing is thus equivalent to saturable absorption!The Ti:Sapph crystal acts as the gain medium, the Kerr lens, and the aperture!,Titanium Sapphire (Ti:Sapphire),Ti:Sapphire has high gain and a very high n2.As a result, it acts both as the gain medium and the mode-locker.It i

47、s currently the workhorse laser of the ultrafast community, emitting pulses as short as a few fs and average power in excess of a Watt.,Titanium Sapphire,It can be pumped with a (continuous) Argon laser (450-515 nm) or a doubled-Nd laser (532 nm).,Upper level lifetime: 3.2 msec,Ti:Sapphire lases fro

48、m 700 nm to 1000 nm.,Mechanisms that limit pulse shortening,Gain narrowing: G(w) = exp(-aw2), then after N passes, the spectrum will narrow by GN(w) = exp(-Naw2), which is narrower by N1/2.Etalon effects:This yields multiple pulses, spreading the energy over time, weakening the pulses.Group-velocity

49、 dispersion:GVD spreads the pulse in time. And everything has GVDAll fs lasers incorporate dispersion-compensating components. Well spend several lectures discussing GVD!,The universe conspires to lengthen pulses.,Phase and Group Velocities,The phase velocity, vf, is that of the high-frequency oscil

50、lations. The group velocity, vg, is that of the pulse envelope.,Dispersion is critical in ultrafast optics.,Dispersion, the dependence of the refractive index on wavelength, has two effects on a pulse, one in space and the other in time.,Both effects play major roles in ultrafast optics.,Group-veloc