半导体激光器本科毕业论文文献翻译.doc

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1、毕 业 设 计（论 文）英文翻译姓 名 学 号 0811122121 所在学院 理 学 院 专业班级 2008级光信1班 指导教师 日 期 2012年4月20 日 英文原文1.5 Experimental SetupDue to the many concepts and variations involved in performing the experiments in this project and also because of their introductory nature, Project 1 will very likely be the most time consum

2、ing project in this kit. This project may require as much as 9 hours to complete. We recommend that you perform the experiments in two or more laboratory sessions. For example, power and astigmatic distance characteristics may be examined in the first session and the last two experiments (frequency

3、and amplitude characteristics) may be performed in the second session. A Note of CautionAll of the above comments refer to single-mode operation of the laser which is a very fragile device with respect to reflections and operating point. One must ensure that before performing measurements the laser

4、is indeed operating single-mode. This can be realized if a single, broad fringe pattern is obtained or equivalently a good sinusoidal output is obtained from the Michelson interferometer as the path imbalance is scanned. If this is not the case, the laser is probably operating multimode and its curr

5、ent should be adjusted. If single-mode operation cannot be achieved by adjusting the current, then reflections may be driving the laser multimode, in which case the setup should be adjusted to minimize reflections. If still not operating single-mode, the laser diode may have been damaged and may nee

6、d to be replaced.WarningThe lasers provided in this project kit emit invisible radiation that can damage the human eye. It is essential that you avoid direct eye exposure to the laser beam. We recommend the use of protective eyewear designed for use at the laser wavelength of 780 nm. Read the Safety

7、 sections in the Laser Diode Driver Operating Manual and in the laser diode section of Component Handling and Assembly (Appendix A) before proceeding.1.5.1 Semiconductor Diode Laser Power Characteristics1. Assemble the laser mount assembly (LMA-I) and connect the laser to its power supply. We will f

8、irst collimate the light beam. Connect the laser beam to a video monitor and image the laser beam on a white sheet of paper held about two to ten centimeters from the laser assembly. Slowly increase the drive current to the laser and observe the spot on the white card. The threshold drive current ra

9、ting of the laser is supplied with each laser. Increase the current to about 10-20 mA over the threshold value. With the infrared imager or infrared sensor card, observe the spot on the card and adjust the collimator lens position in the laser assembly LMA-I to obtain a bright spot on the card. Move

10、 the card to about 30 to 60 centimeters from the lens and adjust the lens position relative to the laser to obtain a spot where size does not vary strongly with the position of the white card. When the spot size remains roughly constant as the card is moved closer or further from the laser, the outp

11、ut can be considered collimated. Alternatively, the laser beam may be collimated by focusing it at a distance as far away as possible. Protect fellow co-workers from accidental exposure to the laser beam.2. Place an 818-SL detector on a post mount (assembly M818) and adjust its position so that its

12、active area is in the center of the beam. There should be adequate optical power falling on the detector to get a strong signal. Connect the photodetector to the power meter (815). Reduce the background lighting (room lights) so that the signal being detected is only from the laser. Reduce the drive

13、 current to a few milliamperes below threshold and, again, check to see that room light is not the dominant signal at the detector by blocking the laser light.3. Increase the current and record the output of the detector as a function of laser drive current. You should obtain a curve similar to Figu

14、re 1.2. If desired, the diode temperature may also be varied to observe the effects of temperature on threshold current. When examining laser diode temperature characteristics, the laser diode driver should be operated in the constant current mode as a safeguard against excessive currents that damag

15、e the diode laser. Note that as the diode temperature is reduced, the threshold decreases. Start all measurements with the diode current off to prevent damage to the laser by preventing drive currents too high above threshold. To prevent destruction of the laser, do not exceed the stated maximum dri

16、ve current of the laser.1.5.2 Astigmatic Distance CharacteristicsThe laser diode astigmatic distance is determined as follows. A lens is used to focus the laser beam at a convenient distance. A razor blade is, then, incrementally moved across the beam to obtain data for total optical power passing t

17、he razor edge vs. the razor blade position. A plot of this data produces an integrated power profile of the laser beam (Figure 1.9a) which through differentiation exposes the actual power profile (Figure 1.9b) which, in turn, permits determination of the beam diameter (W). A beam diameter profile is

18、 obtained by measuring the beam diameter while varying the laser position. Figure 1.9c illustrates the two beam diameter profiles of interest: one for razor edge travel in the direction perpendicular to the laser diode junction plane and the other for travel in the direction parallel to the junction

19、 plane. The astigmatic distance for a laser diode is the displacement between the minima of these two profiles. This method is known as the knife edge technique.1. Assemble the components shown in Figure 1.8 with the collimator lens (LC), in the rotational stage assembly (RSA-I), placed roughly 1 ce

20、ntimeter away from the laser. The beam should travel along the optic axis of the lens. This is the same lens used in collimating the laser in the previous setup. The approximate placement of all the components are shown in the figure. Make sure that the plane of the diode junction (xz plane in Figur

21、e 1.1) is parallel with the table surface.2. Due to the asymmetric divergence of the light, the cross-section of the beam leaving the laser and, further, past the spherical lens is elliptical. The beam, thus, has two distinct focal points, one in the plane parallel and the other in the plane perpend

22、icular to the laser diode junction. There is a point between the two focal points where the beam cross-section is circular. With the infrared imager and a white card, roughly determine the position where the beam cross-section is circular.Figure 1.9 Procedure for finding astigmatic distance.3. Adjus

23、t the laser diode to lens distance such that the razor blades are located in the xy plane where the beam cross-section is circular.4. Move the laser diode away from the lens until minimum beam waist is reached at the plane of razor blades. Now, move the laser diode about 200 m further away from the

24、lens.5. Move razor blade 1 in the x direction across the beam through the beam spread x and record the x position and detected intensity at each increment (100 m increments). The expected output is shown in Figure 1.9. The derivative of this curve yields the intensity profile of the beam in the x di

25、rection from which the beam diameter is determined.6. Repeat with razor blade 2 for y in the y direction.7. Move the laser closer to the lens in increments (50 m) through a total of at least than 500m. Repeat Steps 5 and 6 at each z increment, recording the z position.8. Using the collected data, de

26、termine the beam intensity profiles in the x and y directions as a function of the lens position z. This is done by differentiating each data set with respect to position. Then, calculate the beam diameter and plot as a function of z. The difference in z for the minimum in x and y is the astigmatic

27、distance of the laser diode. Use of computer software, especially in differentiating the data, is highly recommended.If the laser junction is not parallel to the table surface, then for each measurement above, you will obtain an admixture of the two beam divergences and the measurement will become i

28、mprecise. If the laser is oriented at 45 to the surface of the table, the astigmatic distance will be zero.Different laser structures will have different angular beam divergences and, thus, different astigmatic distances. If you have access to several different laser types (gain guided, index guided

29、), it may be instructive to characterize their astigmatic distances.1.5.3 Frequency Characteristics of Diode LasersIn order to study frequency characteristics of a diode laser, we will employ a Michelson interferometer to convert frequency variations into intensity variations. An experimental setup

30、for examining frequency and, also, amplitude characteristics of a laser source is illustrated in Figure 1.10.1. In this experiment, it is very possible that light may be coupled back into the laser, thereby, destabilizing it. An optical isolator, therefore, will be required to minimize feedback into

31、 the laser. A simple isolator will be constructed using a polarizing beam splitter cube and a quarterwave plate. We orient the quarterwave plate such that the linearly polarized light from the polarizer is incident at 45 to the principal axes of the quarterwave plate so that light emerging from the

32、quarterwave plate is circularly polarized. Reflections change left-circular polarized light into right-circular or vice versa so that reflected light returning through the quarterwave plate will be linearly polarized and 90 rotated with respect to the polarizer transmission axis. The polarizer, then

33、, greatly attenuates the return beam. In assembling the isolator, make sure that the laser junction (xz plane in Figure 1.1) is parallel to the surface of the table (the notch on the laser diode case points upward) and the beam is collimated by the lens. The laser beam should be parallel to the surf

34、ace of the optical table. Set the polarizer and quarterwave (/4) plate in place. Place a mirror after the /4 plate and rotate the /4 plate so that maximum rejected signal is obtained from the rejection port of the polarizing beam splitter cube as shown in Figure 1.11. When this signal is maximized,

35、the feedback to the laser should be at a minimum.2. Construct the Michelson interferometer as shown in Figure 1.12. Place the beam steering assembly (BSA-II) on the optical table and use the reflected beam from the mirror to adjust the quarterwave plate orientation. Set the cube mount (CM) on the op

36、tical breadboard, place a double sided piece of adhesive tape on the mount, and put the nonpolarizing beam splitter cube (05BC16NP.6) on the adhesive tape. Next, place the other beam steering assembly (BSA-I) and the detector mount (M818BB) in location and adjust the mirrors so that the beams reflec

37、ted from the two mirrors overlap at the detector. When long path length measurements are made, the interferometer signal will decrease or disappear if the laser coherence length is less than the two way interferometer path imbalance. If this is the case, shorten the interferometer until the signal r

38、eappears. If this does not work, then check the laser for single-mode operation by looking for the fringe pattern on a card or by scanning the piezoelectric transducer block (PZB)in BSA-II and monitoring the detector output which should be sinusoidal with PZB scan distance. If the laser does not app

39、ear to be operating single-mode, realign the isolator and/or change the laser operating point by varying the bias current. Additionally, to ensure single-mode operation, the laser should be DC biased above threshold before applying AC modulation. Overdriving the laser can also force it into multimod

40、e operation.3. The Michelson interferometer has the property that depending on the position of the mirrors, light may strongly couple back toward the laser input port. In order to further reduce the feed-back, slightly tilt the mirrors as illustrated in Figure 1.13. If still unable to obtain single-

41、mode operation, replace the laser diode.4. Place a white card in front of the detector and observe the fringe pattern with the infrared imager. Slightly adjust the mirrors to obtain the best fringe pattern. Try to obtain one broad fringe.5. Position the detector at the center of the fringe pattern s

42、o that it intercepts no more than a portion of the centered peak.6. By applying a voltage to the piezoelectric transducer block attached to the mirror (part PZB) in one arm of the interferometer (i.e. BSA-II), maximize the output intensity. The output should be stable over a time period of a minute

43、or so. If it is not, verify that all components are rigidly mounted. If they are, then room air currents may be destabilizing the setup. In this case, place a box (cardboard will do) over the setup to prevent air currents from disturbing the interferometer setup.7. Place the interferometer in quadra

44、ture (point of maximum sensitivity between maximum and minimum outputs of the interferometer) by varying the voltage on the PZB.8. The output signal of the interferometer due to frequency shifting of the laser is given by I = 2/c L where L is the difference in path length between the two arms of the

45、 interferometer and is the frequency sweep of the laser that is induced by applying a current modulation. Remember that in a Michelson interferometer L is twice the physical difference in length between the arms since light traverses this length difference in both directions. L values of 3-20 cm rep

46、resent convenient length differences with the larger L yielding higher output signals. Before we apply a current modulation to the laser, note that the interferometer output signal, I, should be made larger than the detector or laser noise levels by proper choice of L and current modulation amplitud

47、e di. Also recall from Section 1.3 that when the diode current is modulated so is the laser intensity as well as its frequency. We can measure the laser intensity modulation by blocking one arm of the interferometer. This eliminates interference and enables measurement of the intensity modulation de

48、pth. We, then, subtract this value from the total interferometer output to determine the true dI/di due to frequency modulation. Apply a low frequency, small current modulation to the laser diode. Note that when the proper range is being observedand for the amplitude change only.Recalling ,orwhere K is a detector response constant determined by varying L.9. With the interferometer and detection system properly adjusted, vary the drive frequency of the laser and obtain the frequency response of the laser (Figure 1.4 or 1.10a).You will need to record two sets of data: (i)