phywe-tess-phy-lex-advoptik-en

ADVANCED OPTICSAND LASER PHYSICS

Laserphysik_07 12.12.2006 12:38 Uhr Seite 1

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About Phywe

Founded in Göttingen, Germany in 1913 by Dr. Gotthelf Leimbach, Phywe Systeme GmbH & Co. KG quickly advanced

to one of the leading manufacturers of scientific equipment.

Over this period of more than 90 years Phywe has been putting quality and innovation into its products as a

fundamental requirement.

As a well known international supplier in the fields of science and engineering we have made a significant impact on

the market through high quality equipment.

Phywe products are made in Germany and in use throughout the world in the fields of education und research, from

primary schools right through to university level.

Up-to-date educational systems, planning and commissioning of scientific and engineering laboratories to meet

specific requirements are our daily business.

As a supplier of complete, fully developed and established systems, Phywe provides teaching and learning systems

for students as well as teacher demonstration experiments. The system ranges from simple, easy to operate

equipment intended for student use up to coverage of highly sophisticated and specialised university equipment

demands.

Phywe Systeme GmbH & Co. KG has achieved a very high standard based on research and technology and through

exchange of experiences with universities and high schools as well as with professors and teachers.

As experienced and competent manufacturer, we would gladly assist you in the

selection of the "right" experiments for your particular curricula.


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Advanced Optics and Laser Physics

Page

Laser Physics

Helium-Neon-laser (P2260700) 6

CO2-laser (P2260400) 7

Nd-YAG-laser (P2260900) 8

Advanced Optics

Diffraction of light through a double slit or by a grid (P1216800) 9

Diffraction of lightthrough a slit and stripes, Babinet’s theorem (P1216900) 10

Michelson interferometer (P1217100) 11

Newton’s rings (P1217200) 12

Polarisation through �/4 plates (P1217400) 13

Kerr effect (P1217600) 14

Faraday effect (P1217700) 15

Determination of the index of refractionof CO2 with Michelson’s interferometer (P1218000) 16

Michelson interferometer – High Resolution (P1306700) 17

Doppler effect with the Michelson interferometer (P1307000) 18

Magnetostriction with the Michelson interferometer (P1307100) 19

Determination of the refraction indexof air with the Mach-Zehnder interferometer (P1307500) 20

Fabry-Perot interferometer – Determination of the laser light’s wavelength (P1307700) 21

Fabry-Perot interferometer – optical resonator modes (P1307800) 22

Fourier optics – optical filtration – 4f Arrangement (P2261200) 23

LDA – Laser Doppler Anemometry (P1308000) 24

White light hologram with expansion system (P1290200) 25

Transmission hologram with expansion system (P1290400) 26

Transfer hologram from a master hologram (P1290500) 27

Real time procedure I (bending of a plate) (P1290900) 28

Student System “Advanced Optics” and Laser Physics 29

Equipment Holders 30

Optical Components 31

Further equipment and components 32

Lasers and Accessories 34

Index 35

How to order 36

Order form 37

ContentsThe Experimental Conceptin a short overview:

The customersThe Phywe Educational System for “AdvancedOptics and Laser Physics” is intended for physicslaboratory courses at universities, colleges andsimilar institutions and also for advancedcourses in highschools.

The specific fieldsThe experimental system allows many importantexperiments in:

1. Geometrical optics

2. Wave optics

3. Holography

4. Interferometry

5. Fourier optics

6. Applied optics

7. Laser Physics

The equipment systemTo investigate these experimental topics weoffer a large didactical equipment set with:

1. high-quality light sources (different types of lasers)

2. easy and stable placeable magnetic opticalequipment

Furthermore three didactic Laser Systems areavailable to investigate the fundamentalworking principles and characteristics of lasers

The experimental literatureWe support your experimentation with 3 hand-books containing 45 accurately described experi-ments incl. theoretical backround information,drawings, safety and maintenance remarks.


4 PHYWE Systeme GmbH & Co. KG · D-37070 GöttingenAdvanced Optics and Laser Physics

Experimental Literature

Laser Physics I – Experiments with coherent light 01179.02

Please ask for a complete equipmentlist Ref. No. 227021 Diffraction of lightLP 1.1 (12166)Diffraction of light through a slit and atan edge.LP 1.2 (12167)Diffraction through a slit andHeisenberg’s uncertainty principle.LP 1.3* (12168)Diffraction of light through a double slitor by a grid. LP 1.4* (12169)Diffraction of light through a slit andstripes, Babinet’s theorem

2 Interference of lightLP 2.1 (12170)Fresnel mirror and biprismLP 2.2* (12171)Michelson interferometerLP 2.3* (12172)Newton’s rings

3 Polarisation of lightLP 3.1 (12173)Fresnel’s law, theory of reflectionLP 3.2* (12174)Polarisation through λ/4 platesLP 3.3 (12175)Half shadow polarimeter, rotation of pola-risation through an optically active mediumLP 3.4* (12176)Kerr effectLP 3.5* (12177)Faraday effect

4 Refraction of lightLP 4.1 (12178)Index of refraction n of a flint glassprismLP 4.2 (12179)Determination of the index of refractionof air with Michelson’s interferometerLP 4.3* (12180)Determination of the index of refractionof CO2 with Michelson’s interferometer

5 Law of radiationLP 5.1 (12181)Lambert’s law of radiation

Laser Physics IIHolography 01400.02

Please ask for a complete equipmentlist Ref. No. 22703LH 1 (12900)Fresnel zone plate

LH 2 (12901)White light hologram

LH 3* (12902)White light hologram with expansion system

LH 4 (12903)Transmission hologram

LH 5* (12904)Transmission hologram with expansion system

LH 6* (12905)Transfer hologram from a master hologram.

LH 7 (12906)Double exposure procedure

LH 8 (12907)Time-averaging procedure I (with tuning fork).

LH 9 (12908)Time-averaging procedure II (with loudspeaker).

LH 10* (12909)Real time procedure I (bending of a plate).

LH 11 (12910)Real time procedure II (oscillating plate).

Laser Physics IIIInterferometry 01401.02

Please ask for a complete equipmentlist Ref. No. 22704LI 1 (13066)Michelson interferometerLI 2* (13067)Michelson interferometer – high resolutionLI 3 (13068)Mach - Zehnder interferometerLI 4 (13069)Sagnac interferometerLI 5* (13070)Doppler-Effect with Michelson interferom.LI 6* (13071)Magnetostriction with Michelson interferometerLI 7 (13072)Thermal expansion of solids with Michelson interferometerLI 8 (13073)Refraction index of CO2-gas withMichelson interferometerLI 9 (13074)Refraction index of air with Michelson interferometerLI 10* (13075)Refraction index of air with Mach-Zehnder interferometerLI 11 (13076)Refraction index of of CO2-gas withMach-Zehnder interferometerLI 12* (13077)Fabry - Perot interferometer – determi-nation of the wavelength of laserlightLI 13* (13078)Fabry - Perot interferometer – optical resonator modesLI 14 (22611)Fourier optics –2 f arrangementLI 15* (22612)Fourier optics – 4 f arrangement, filteringand reconstructionLI 16 (13079)Optical determination of the velocity ofultrasound in liquids – phasemodulationof laserlight by ultrasonic wavesLI 17* (13080)LDA – Laser Doppler AnemometryLI 18 (13081)Twyman-Green interferometer

Laboratory ExperimentsPhysics 16502.12

230 experiments in the field of:

1. Mechanics64 experiments

2. Optics34 experiments

incl. the three didactical laser

experiments with:

1. He-Ne laser*2. Nd-YAG laser*3. CO2 laser*

3. Thermodynamics21 experiments

4. Electricity45 experiments

5. Physical Stucture of Matter66 experiments

incl. 20 experiments for the

Phywe X-Ray Unit

LABORATORY EXPERIMENTS

PHYSICS

1650

2.12

Laboratory Experiments

Klaus Hermbecker

Ludolf von Alvensleben

Regina Butt

Andreas Grünemaier

Robin Sandvoß

This volume which has been developed by Phywe presents an assortment of 23 experiments in “Advanced Optics and Laser Physics”. In this brochure these experiments are shown in a short form.

The three Laser Physics manuals below-mentioned include extensive descriptions of 45 experiments. In addition, they provide safetyinformation concerning the use of lasers as well as information on handling and maintaining optical components.

In our Laboratory Experiments Physics manual you can find experiments related to our three didactic laser systems and a wide rangeof other highly interesting experiments on other subjects.

*These experimentsare shown

in a short form inthis brochure


5PHYWE Systeme GmbH & Co. KG · D-37070 Göttingen Advanced Optics and Laser Physics

Advanced Optics and Laser Physics

Equipment List guarantee time-savingand easy conducting of the experiment.

Set-up and procedure with a lot ofinformation for an easy, quick andcomfortable experimental set-up.

All experiments are uniformly built-up and contain references such asRelated terms, Principle and Objectiveto introduce the subject.

Experimental literatureHandbook Laserphysics 1“Experiments with Coherent Light” 01179.02

Handbook Laserphysics 2“Holography” 01400.02

Handbook Laserphysics 3“Interferometry, Fourier-Optics, etc.” 01401.02

The experiments in the PHYWE Publication Series “Advanced Optics and Laser Physics” are intended for

physics laboratory courses at universities, colleges and similar institutions and also for advanced courses in

high schools.

Drawing for an easy, quick andsafe experimental set-up.

Theoretical backround information and remarks onsafety and maintenance oflaser, equipment and opticalcomponents.



Advanced Optics and Laser Physics LEP

P2260700 Helium-Neon-laser

Principle:The difference between spontaneousand stimulated emission of light isdemonstrated. The beam propagationwithin the resonator cavity of a He-Ne-laser and its divergence aredetermined, its stability criterion ischecked and the relative outputpower of the laser is measured as afunction of the tube’s position insidethe resonator and of the tube current.

The following items can be realizedwith advanced set 08656.02.By means of a birefringent tuner anda Littrow prism different wave-lengths can be selected and quanti-tatively determined if a monochro-mator is available.

Finally you can demonstrate the ex-istence of longitudinal modes andthe gain profile of the He-Ne-laserprovided an analysing Fabry Perotsystem is at your disposal.

Tasks:1. Set up the He-Ne-laser. Adjust the

resonator mirrors by use of the pilotlaser. (left mirror: VIS, HR, plane;right mirror: VIS, HR, R = 700 mm)

2. Check on the stability condition ofa hemispherical resonator.

Relative output power as a function of mirror spacing.

3. Measure the integral relative out-put power as a function of thelaser tube’s position within thehemispherical resonator.

4. Measure the beam diameter with-in the hemispherical resonatorright and left of the laser tube.

5. Determine the divergence of thelaser beam.

6. Measure the integral relative out-put power as a function of thetube current.

The He-Ne-laser can be tuned usinga BFT or a LTP. Longitudinal modescan be observed by use of a FabryPerot Etalon of low finesse. Remark:These points can only be coveredquantitatively if a monochromatorand an analysing Fabry Perot systemare available.

Experiment set He-Ne-laser, basic set 08656.01 1

Optical bench on carrier rail 08599.01 1

Diaphragm for adjustment of laser 08608.00 2

Photoelement, silicon 08734.00 1

Digital multimeter 07134.00 1

Screen, white, 150�150 mm 09826.00 1

Danger sign -LASER- 06542.00 1

Barrel base –PASS- 02006.55 1

Vernier caliper 03010.00 1

Measuring tape, l = 2 m 09936.00 1

Protective glasses for the He-Ne-laser 08581.10 1

Cleaning set for laser 08582.00 1

Option:

Experiment set He-Ne-laser, advanced set 08656.02 1

consisting of:

• Birefringent tuner (Lyot Plate, BFT) with holder and rider (08656.10) •Littrow prism with x/y-holder and rider (08656.20) • Fabry Perot Etalon inx/y-holder and rider (08656.30)

What you need:

Helium-Neon-laser, basic set P2260701

What you can learn about

� Spontaneous and stimulatedlight emission

� Inversion� Collision of second type� Gas discharge tube� Resonator cavity� Transverse and longitudinal

resonator modes� Birefraction� Brewster angle� Littrow prism� Fabry Perot

Helium-Neon-laser, advanced set P2260705

Class 3B Laser



LEP Advanced Optics and Laser Physics

Nd-YAG-laser P2260900

25

20

15

10

5

50 100 150

PNd-YAGmW

Pump powermW

From graphic:Threshold power = 57 mW

From graphic:Slope efficiency: 30%

Principle:The rate equation model for an opti-cally pumped four-level laser systemis determined. As lasing medium, aNd-YAG (Neodymium-Yttrium Alu-minium Garnet) rod has been select-ed which is pumped by means of asemiconductor diode laser.

The IR-power output of the Nd-YAGlaser is measured as a function of theoptical power input and the slope ef-ficiency as well as the thresholdpower are determined.

Finally, a KTP-crystal is inserted intothe laser cavity and frequency dou-bling is demonstrated. The quadraticrelationship between the power ofthe fundamental wave and the beampower for the second harmonic isthen evident.

Nd-YAG laser power output as a function of the pump power l = 808.4 nm.

Tasks:1. Set up the Nd-YAG laser and opti-

mize its power output.

2. The IR-power output of the Nd-YAG laser is to be measured as afunction of the pump power. Theslope efficiency and the thresholdpower are to be determined.

3. Verify the quadratic relationshipbetween the power of the funda-mental wave, with l = 1064 nm,and the beam power of the secondharmonic with l = 532 nm.

Basic set optical pumping 08590.93 1

Sensor for measurement of beam power 08595.00 1

Nd-YAG laser cavity mirror/holder 08591.01 1

Laser cavity mirror frequency doubling 08591.02 1

Frequency doubling crystal in holder 08593.00 1

Filter plate, short pass type 08594.00 1


Oscilloscope, 30 MHZ, 2 channels 11459.95 1

Screened cable, BNC, l 750 mm 07542.11 3

Protective glasses for the Nd-YAG-Laser 08581.20 1

Cleaning set for laser 08582.00 1

Optional equipment for setup and storage:

Optical base plate in experiment case 08700.01 1

What you need:

Nd-YAG-laser P2260900


� Optical pumping� Spontaeous emission� Induced emission� Inversion� Relaxation� Optical resonator� Resonator modes� Polarization� Frequency doubling

4. Determine the power output ofthe semiconductor laser as a func-tion of the injection current.

5. Trace the fluorescent spectrum ofthe Nd:YAG rod pumped by thediode laser and verify the mainabsorption lines of neodymium.

6. Measure the mean life time of the4F3/2-level of the Nd-atoms.

7. Extend laser cavity by KTP-crystalfor frequency doubling. Finalizealignment testimate output powerof second harmonic line.

Class 4 Laser



P2260400 CO2-laser

Principle:Among molecular lasers, the CO2-laser is of greatest practical impor-tance. The high level of efficiencywith which laser radiation can begenerated in continuous wave (cw)and pulse operation is its most fasci-nating feature.

The experimental equipment set isan open CO2-didactic laser system oftyp. 5 W power output. All compo-nents of the system can be handledindividually and the influence ofeach procedure on the output powercan be studied. One target in learn-ing is the alignment of the CO2-laser.

Tasks:1. Align the CO2-laser and optimize

its power output.

2. Check the influence of the Brew-ster windows position on thepower output.

3. Determine the power output as afunction of the electric powerinput and gasflow.

4. Evaluate the efficiency as a func-tion of the electric power input.

Laser power as a function of the angle of inclination of the brewster windownormal N.

5. If the gas-mixing unit is suppliedthe influence of the differentcomponents of the laser gas (CO2,He, N2) to the output efficiency ofthe CO2-laser are analyzed.

6. Measurement of temperaturesdifferences for the laser gas(input/output) for study of con-version efficiency.

CO2-laser tube, detachable, typ 5 W 08596.00 1Module box for CO2-laser tube 08597.00 1Set of laser mirrors, ZnSe and Si with x/y holder/rider 08598.00 1Optical bench on steel rail l = 1.3 m 08599.00 1HV-power supply 5 kV/50 mA DC 08600.93 1Ballast resistor unit incl. 3 HV cables 08601.00 1Cooling water unit, portable 08602.93 1Vacuum pump, two-stage 02751.93 1Gas filter/buffer unit 08605.00 1He-Ne-laser/adjusting device 08607.93 1Diaphragm for adjusting CO2-laser 08608.00 2Screen translucent, 250�250 mm 08064.00 1Right angle clamp –PASS- 02040.55 1Powermeter 30 mW/10 Watt 08579.93 1Support for power probe 08580.00 1Protecting glasses, 10.6 micro-m 08581.00 1Cleaning set for laser 08582.00 1ZnSe biconvex lens, d = 24 mm, f = 150 mm 08609.00 1Digital thermometer, 2 channels, NiCr-Ni 08583.00 1HV-isolated temperature probe 08584.00 1Control panel with support, 1 gas* 08606.00 1Pressure control valve 200/3bar* 08604.00 1Laser gas in bottle, 50 l/200 bar* 08603.00 1

*Alternative:Laser gas mixing unit, 3 gases (see picture) 08606.88 1He-, N2- and CO2-gas

Option:Experiment set for laser beam analysis 08610.10 1

1. estimation of wavelength by diffraction grating and2. distribution of power by diaphragm

IR conversion plate for observation of CO2-laserinfrared radiation 08611.10 1

What you need:

CO2-laser P2260400

Advanced Optics and Laser Physics LEP


� Molecular vibration, excitation� Electric discharge� Vibration/Rotation niveau� Inversion/

Optical amplification� Induced/Spontaneous emission� Spectrum of emission� Polarization� Brewster angle� Optical resonator

Class 4 Laser



LP 1.3 Advanced Optics and Laser Physics

Diffraction of light through a double slit or by a grid P1216800

Principle:The coherent monochromatic light of a laser is directed to a diaphragmwith a varying number of slits. Theresulting interference patterns arestudied using a photoelement.

Qualitative intensity distribution of diffraction through 2 and 4 slits, thedistance x being normalised to �/s. The intensity distribution of the simpleslit has been represented with exaggerated height to give a clearer view.

� Fraunhofer diffraction� Huygens’ principle� Interference� Coherence

Tasks:The intensity distribution of diffrac-tion patterns formed by multiple slitsis measured using a photoelement.The dependence of this distributionfrom the slit widths the number ofslits and the grid constant is investi-gated. The obtained curves are com-pared to the theoretical values.

Optical base plate with rubber feet 08700.00 1

He-Ne-laser, 5 mW with holder* 08701.00 1

Power supply for laser head 5 mW* 08702.93 1

Adjusting support 35�35 mm 08711.00 1

Surface mirror 30�30 mm 08711.01 1

Magnetic foot for optical base plate 08710.00 3

Diaphragm holder for optical base plate 08724.00 1

Diaphragm, 4 double slits 08523.00 1

Diaphragm, 4 multiple slits 08526.00 1

Photoelement for optical base plate** 08734.00 1

Sliding device, horizontal 08713.00 1

Universal measuring amplifier** 13626.93 1

Voltmeter, 0.3-300 VDC, 10-300 VAC 07035.00 1

Connecting cord, l = 500 mm, red** 07361.01 2

*Alternative to laser 5 mW, power supply and shutter:

Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

or

Diodelaser 0.2/1 mW; 635 nm 08760.99 1

**Alternative:

Si-Photodetector with amplifier 08735.00 1

Control Unit for Si-Photodetector 08735.99 1

Screened cable, BNC, l = 750 mm 07542.11 1

Adapter, BNC-socket/4mm plug pair 07542.27 1

What you need:

Diffraction of light through a double slit or by a grid P1216800


Intensity distribution of the corresponding simple slit



P1216900 Diffraction of light through a slit and stripes, Babinet’s theorem

Principle:Babinet's Principle states that thediffraction pattern for an aperture isthe same as the pattern for anopaque object of the same shape il-luminated in the same manner. Thatis the pattern produced by a diffract-ing opening of arbitrary shape is thesame as a conjugate of the openingwould produce.

Principle of set up for diffraction through a slit and qualitative distribution onintensities � (�) �0 in the detector plane LD.

Tasks:Babinet’s theorem is verified by thediffraction pattern of monochromat-ic light directed through a slit and anopaque stripe complementary to thelatter. The experiment is also per-formed with a circular aperture andan opaque obstacle conjugate to thisopening.





Surface mirror 30�mm 08711.01 1



Screen, with diffracting elements 08577.02 1







Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

or

Diodelaser 0.2/1 mW; 635 nm 08760.99 1

**Alternative:





What you need:

Diffraction of light through a slit and stripes,Babinet’s theorem P1216900

Advanced Optics and Laser Physics LP 1.4


� Fraunhofer interference� Huygens’ principle� Multiple beam interference� Babinet’s theorem� Coherence

LD




Michelson interferometer P1217100

Principle:In a Michelson interferometer, a lightbeam is split into two partial beamsby a semi transparent glass plate(amplitude splitting). These beamsare reflected by two mirrors andbrought to interference after theypassed through the glass plate asecond time.

Formation of interference rings.

Tasks:The wavelength of the used laserlight is determined through the ob-servation of the change in the inter-ference pattern upon changing thelength of one of the interferometerarms.







Michelson interferometer 08557.00 1

Achromatic objective 20� N.A. 0.45 62174.20 1

Pinhole 30 micron 08743.00 1


xy shifting device 08714.00 2

Adapter ring device 08714.01 1

Screen, white, 150�150 mm 09826.00 1


Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

or

Diodelaser 0.2/1 mW; 635 nm 08760.99 1

What you need:

Michelson interferometerP1217100


� Interference� Wavelength� Refraction index� Light velocity� Phase� Virtual light source� Coherence



P1217200 Newton’s rings

Principle:The air wedge formed between aslightly convex lens and a plane glassplate (Newton's colour glass) is usedto cause interference of monochro-matic light. The wavelength is deter-mined from the radii of the interfer-ence rings.

Generation of Newton’s rings.

Tasks:The diameters of interference ringsproduced by Newton’s colour glassare measured and these are used to:

1. determine the wavelength for agiven radius of curvature of thelens,

2. determine the radius of curvaturefor a given wavelength.












Newton colourglass for optical base plate 08730.02 1

Lensholder for optical base plate 08723.00 1

Lens, mounted, f = +50 mm 08020.01 1

Screen, transparent with holder for optical base plate 08732.00 1



Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

or

Diodelaser 0.2/1 mW; 635 nm 08760.99 1

What you need:

Newton’s ringsP1217200



� Coherent light� Phase relation� Path difference� Interference at thin layers� Newton's colour glass




Polarisation through �/4 plates P1217400

Principle:Monochromatic light impinges on amica plate, perpendicularly to its op-tical axis. If the thickness of theplate is adequate (l/4 plate), a phaseshift of 90° occurs between the ordi-nary and the extraordinary beamwhen the latter leaves the crystal.The polarisation of exiting light isexamined for different angles be-tween the optical axis of the l/4plate and the direction of polarisa-tion of incident light.

Tasks:1. Measurement of the intensity of

linearly polarised light as a func-tion of the analyser’s position(Malus’ law)

2. Measurement of the light intensi-ty behind the analyser as a func-

Intensity distribution of polarised light for different angles of the �/4 plate,as a function of the analyser position.

tion of the angle between the op-tical axis of the l/4 plate and theanalyser.

3. Carrying out experiment (2) withtwo successive l/4 plates.








Lens, mounted, f = +20 mm 08018.01 1


Polarizing filter for optical base plate 08730.00 2

Polarization specimen, mica 08664.00 2






Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

or

Diodelaser 0.2/1 mW; 635 nm 08760.99 1

**Alternative:





What you need:

Polarisation through l/4 platesP1217400


� Linearly, circularly andelliptically polarised light

� Polarizer� Analyser� Plane of polarisation� Malus' law� Double refraction� Optical axis� Ordinary and extraordinary

beam



P1217600 Kerr effect

Principle:Monochromatic light, which is po-larised vertical impinges on a PLZTelement (lead-lanthanum-zirconi-um-titanium preparation) rotated inits support by 45° against the verti-cal.

An electric field is applied to thePLZT element (Kerr cell) and causesthe latter to become double refract-ing. The phase difference betweenthe ordinary and the extraordinarybeams after the PLZT element isrecorded as a function of the appliedvoltage. It is shown that the differ-ence of phase is proportional to thesquare of the electric field intensity,due to the applied voltage.

Tasks:1. The phase difference between the

ordinary and the extraordinarylight beam is recorded for diffe-rent voltages applied to the PLZTelement, that is, for different fieldintensities. The half wavelengthvoltages U(l/2) must be deter-mined.

2. By plotting the square of the ap-plied voltage against the phasedifference between the ordinaryand the extraordinary beam, it isshown that the relation betweenboth magnitudes is approximatelylinear. The Kerr constant is calcu-lated from the slope of thestraight line.

Relative light intensity I/I0 after analyser A as a function of the voltage Uapplied to the Kerr cell and of phase shift � between the ordinary and theextraordinary beams.

Optical base plate with rubber feet 08700.00 1He-Ne-laser, 5 mW with holder* 08701.00 1Power supply for laser head 5 mW* 08702.93 1Adjusting support 35�35 mm 08711.00 1Surface mirror 30�30 mm 08711.01 1Magnetic foot for optical base plate 08710.00 5Kerr cell PLTZ for optical base plate 08731.00 1High voltage supply unit, 0–10 kV 13670.93 1Loudspeaker, 8 �/5 k� 13765.00 1Polarizing filter for optical base plate 08730.00 2Photoelement for optical base plate*** 08734.00 1Universal measuring amplifier*** 13626.93 1Voltmeter, 0.3-300 VDC, 10-300 VAC 07035.00 1Digital multimeter 07134.00 1Flat cell battery, 9 V 07496.10 1Power frequency generator 1MHz** 13650.93 1Screened cable, BNC, l = 750 mm 07542.11 1Adapter, BNC-socket/4 mm plug pair 07542.27 1Connecting cord, l = 500 mm, yellow 07361.02 1Connecting cord, l = 750 mm, red*** 07362.01 3Connecting cord, l = 750 mm, blue 07362.04 3

*Alternative to laser 5 mW, power supply and shutter:Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1orDiodelaser 0.2/1 mW; 635 nm 08760.99 1

**Alternative:Radio and adapter plug 1

***Alternative:Si-Photodetector with amplifier 08735.00 1Control Unit for Si-Photodetector 08735.99 1Screened cable, BNC, l = 750 mm 07542.11 1Adapter, BNC-socket/4mm plug pair 07542.27 1Connecting cord, l = 500 mm red 07362.01 1

What you need:

Kerr effect P1217600



� Polarisation of light� Double refraction� Optical anisotropy� Modulation of light� Electro-optical modulator

3. Superimposing an alternate volt-age to the constant electric HVfield, the PLZT element is trans-formed to an electro optical mod-ulator. Its function is demonstrat-ed by means of alternate voltagesof variable frequency in the audi-ble range.

Phase shift

Voltage for peaksand minima




Faraday effect P1217700

Principle:The angle of rotation of the plane ofpolarisation of a linearly polarisedlight wave in a rod of flint glass ap-pears to be a linear function of theaverage magnetic flow density andof the length of optical mediumtravelled through by the wave. Thefactor of proportionality is a mediumspecific constant and is calledVerdet’s constant.

Experimental set up (* only required for 5 mW laser)

� Interaction ofelectromagnetic fields

� Electronic oscillation� Electromagnetism� Polarisation� Verdet’s constant� Malus’ law

Tasks:Qualitative investigation of the Fara-day effect through observation ofthe electro optical modulation of thepolarised laser light with frequenciesin the acoustic range.

Optical base plate with rubber feet 08700.00 1He-Ne-laser, 5 mW with holder* 08701.00 1Power supply for laser head 5 mW* 08702.93 1Adjusting support 35�35 mm 08711.00 1Surface mirror 30�30 mm 08711.01 1Magnetic foot for optical base plate 08710.00 5Polarizing filter for optical base plate 08730.00 2Faraday modulator for optical base plate 08733.00 1Power frequency generator 1 MHz** 13650.93 1Ammeter, 1 mA - 3 A DC/AC 07036.00 1Photoelement for optical base plate*** 08734.00 1Universal measuring amplifier*** 13626.93 1Loudspeaker, 8 �/5 k� 13765.00 1Screen, transparent with holder for optical base plate 08732.00 1Connecting cord, l = 500 mm, red 07361.01 3Connecting cord, l = 500 mm, blue 07361.04 2

*Alternative to laser 5 mW, power supply and shutter:Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1orDiodelaser 0.2/1 mW; 635 nm 08760.99 1

**Alternative:Radio and adapter plug 1orLow frequency amplifier 13625.93 1Function generator 13652.93 1Connecting cord, l = 500 mm, red 07361.01 1Connecting cord, l = 500 mm, blue 07361.04 1

*** Alternative:Si-Photodetector with amplifier 08735.00 1Control Unit for Si-Photodetector 08735.99 1Screened cable, BNC, l = 750 mm 07542.11 1Adapter, BNC-socket/4mm plug pair 07542.27 1

What you need:

Faraday Effect P1217700




P1218000 Determination of the index of refraction of CO2 with Michelson’s interferometer

Principle:Light is caused to interfere by meansof a beam splitter and two mirrorsaccording to Michelson’s set up.Substituting the air in a measure-ment cuvette located in one of theinterferometer arms by CO2 gass al-lows to determine the index of re-fraction of CO2.

Michelson’s set up for interference.

Tasks:A Michelson Interferometer is set upand adjusted so that interferencerings can be observed. CO2 gas isfilled into a measurement cuvettethat was filled before with air. Fromchanges in the interference patternthe difference of the refraction indexbetween air and CO2 is determined.







Michelson interferometer 08557.00 1






Screen, white, 150�150 mm 09826.00 1

Glass cell, diameter 21.5 mm 08625.00 1

Compressed gas, CO2, 21 g 41772.06 1

Pipette, with rubber bulb 64701.00 1

Universal clamp with joint 37716.00 1

Silicone tubing, d = 5 mm 39297.00 1


Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

or

Diodelaser 0.2/1 mW; 635 nm 08760.99 1

What you need:

Determination of the index of refraction of CO2with Michelson’s interferometer P1218000



� Interference� Wavelength� Index of refraction� Light velocity� Phase� Virtual light source� Coherence


17PHYWE Systeme GmbH · D-37070 Göttingen Advanced Optics and Laser Physics

LI 2 Advanced Optics and Laser Physics

Michelson interferometer – High Resolution P1306700

Principle:With the aid of two mirrors in aMichelson arrangement, light isbrought to interference. While mov-ing one of the mirrors, the alterationin the interference pattern is ob-served and the wavelength of thelaser light determined.


� Interference� Wavelength� Diffraction index� Speed of light� Phase� Virtual light source

Experimentally determined contrast function in comparison to the theoreticalcontrast function K of a 2-mode laser.

Tasks:1. Construction of a Michelson inter-

ferometer using separate compo-nents.

2. The interferometer is used to de-termine the wavelength of thelaser light.

3. The contrast function K is quali-tatively recorded in order to deter-mine the coherence length with it.







Holder for diaphragm/beam splitter 08719.00 1

Beam splitter 1/1, non polarizing 08741.00 1

Lens, mounted, f = +20 mm 08018.01 1


Screen, white, 150�150 mm 09826.00 1

Interferometer plate with precision drive 08715.00 1

Photoelement for optical base plate 08734.00 1


Flat cell battery, 9 V 07496.10 1



Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

What you need:

Michelson interferometer – High ResolutionP1306700



P1307000 Doppler effect with the Michelson interferometer

Principle:With the aid of two mirrors in aMichelson arrangement, light isbrought to interference. While mov-ing one of the mirrors, the alterationin the interference pattern is ob-served and the modulation frequen-cy is measured using the Doppler ef-fect.

Sample measurement with the y-t recorder.


ferometer using separate compo-nents.

2. Measurement of the Doppler ef-fect via uniform displacement ofone of the mirrors.

Optical base plate with rubber feet 08700.00 1He-Ne-laser, 5 mW with holder* 08701.00 1Power supply for laser head 5 mW* 08702.93 1Interferometer plate with precision drive 08715.00 1Light barrier with counter 11207.30 1Power supply 5 VDC/2.4 A 11076.99 1Support 09906.00 1Motor with gearing and cord pulley 08738.00 1Perforated disk with driving belt 08738.01 1Recorder, tY, 2 channel** 11415.95 1Perforated disk with driving belt 08738.01 1Connecting cord, l = 500 mm, red** 07361.01 2Connecting cord, l = 500 mm, blue** 07361.04 2Photoelement for optical base plate** 08734.00 1Power supply 0-12 V DC/6 V,12 V AC 13505.93 1Adjusting support 35�35 mm 08711.00 4Surface mirror 30�30 mm 08711.01 4Magnetic foot for optical base plate 08710.00 8Support rod, stainless steel, 100 mm 02030.00 1Holder for diaphragm/beam splitter 08719.00 1Right angle clamp -PASS- 02040.55 1Beam splitter 1/1, non polarizing 08741.00 1Lens, mounted, f = +20 mm 08018.01 1Lensholder for optical base plate 08723.00 1Screen, white, 150�150 mm 09826.00 1

*Alternative to laser 5 mW, power supply and shutter:Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

**Alternative:Stop watch 03071.01 1

What you need:

Doppler effect with the Michelson interferometer P1370000


� Interference� Wavelength� Diffraction index� Speed of light� Phase� Virtual light source� Temporal coherence� Special relativity theory� Lorentz transformation

Advanced Optics and Laser Physics LI 5




Magnetostriction with the Michelson interferometer P1307100

Principle:With the aid of two mirrors in aMichelson arrangement, light isbrought to interference. Due to themagnetostrictive effect, one of themirrors is shifted by variation in themagnetic field applied to a sample,and the change in the interferencepattern is observed.

Measuring results of the magnetostriction of nickel with the relative changein length �l/l plotted against applied field strength H


ferometer using separate opticalcomponents.

2. Testing various ferromagnetic ma-terials (iron and nickel) as well asa non-ferromagnetic material,copper, with regard to their mag-netostrictive properties.









Lens, mounted, f = +20 mm 08018.01 1


Screen, white, 150�150mm 09826.00 1

Faraday modulator for optical base plate 08733.00 1

Rods for magnetostriction, set 08733.01 1

Power supply, universal 13500.93 1


Connecting cord, l = 500 mm, blue 07361.04 1

Flat cell battery, 9 V 07496.10 1


Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

What you need:

Magnetostriction with the Michelson interferometerP1307100


� Interference� Wavelength� Diffraction index� Speed of light� Phase� Virtual light source� Ferromagnetic material� Weiss molecular magnetic

fields� Spin-orbit coupling



P1307500 Determination of the refraction index of air with the Mach-Zehnder interferometer

Principle:Light is brought to interference bytwo mirrors and two beam splittersin the Mach-Zehnder arrangement.By changing the pressure in a mea-suring cell located in the beam path,one can deduce the refraction indexof air.

Schematic representation of the cell with normal pressure (a) and nearlyabsolute vacuum (b)

Tasks:1. Construction of a Mach-Zehnder

interferometer using individualoptical components.

2. Measurement of the refractionindex n of air by lowering the airpressure in a measuring cell.










Pin hole 30 micron 08743.00 1




Screen, white, 150�150 mm 09826.00 1

Glass cell, diameter 21.5 mm 08625.00 1

Manual vacuum pump with manometer 08745.00 1

Universal clamp with joint 37716.00 1

Tubing connector, T-shape, ID 8-9 mm 47519.03 1

Tubing adaptor, ID 3-6/7-11 mm 47517.01 1

Vacuum hose, di = 6 mm 39286.00 1

Silicone tubing, di = 3mm 39292.00 1

Glass cell holder on rod 08706.00 1


Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

What you need:

Determination of the refraction index of airwith the Mach-Zehnder interferometer P1307500



� Interference� Wavelength� Diffraction index� Speed of light� Phase� Virtual light source




Fabry-Perot interferometer – Determination of the laser light’s wavelength P1307700

Principle:Two mirrors are assembled to form aFabry-Perot interferometer. Usingthem, the multibeam interference ofa laser’s light beam is investigated.By moving one of the mirrors, thechange in the interference pattern isstudied and the wavelength of thelaser’s light determined.

Multibeam interferometer after Fabry and Perot. Illustration of the principlefor deriving the individual amplitudes.

Tasks:1. Construction of a Fabry-Perot in-

terferometer using separate opti-cal components.

2. The interferometer is used to de-termine the wavelength of thelaser light.










Beam splitter T = 30, R = 70, with holder 08741.01 1

Lens, mounted, f = +20 mm 08018.01 1


Screen, white, 150�150 mm 09826.00 1


Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

What you need:

Fabry-Perot interferometer – Determinationof the laser lights’s wavelength P1307700


� Interference� Wavelength� Diffraction index� Speed of light� Phase� Virtual light source� Multibeam interferometer


P1307800 Fabry-Perot interferometer – optical resonator modes

Principle:Two mirrors are assembled to form aFabry-Perot Interferometer. Usingthem, the multibeam interference ofa laser’s light beam is investigated.On moving one of the mirrors, thechange in the intensity distributionof the interference pattern is stud-ied. This is a qualitative experiment,to study the shape of different lasermodes and compare it with somephotos given in this description.

Intensity distribution of the Hermitian-Gaussian resonator modes.

Tasks:1. Construction of a Fabry-Perot in-

terferometer using separate opti-cal components.

2. The interferometer is used to ob-serve different resonator modeswithin the interferometer.







Concave mirror OC; r = 1.4 m, T = 1.7%, mounted 08711.03 1

Plane mirror HR >99%, mounted 08711.02 1


Lens, mounted, f = +20 mm 08018.01 1


Screen, white, 150�150 mm 09826.00 1

What you need:

Fabry-Perot interferometer –optical resonator modes P1307800


� Interference� Wavelength� Diffraction index� Speed of light� Phase� Virtual light source� Two-beam interferometer






Fourier optics – optical filtration – 4f Arrangement P2261200

Principle:The electric field distribution of lightin a specific plane (object plane) isFourier transformed into the 4fconfiguration by 2 lenses and opti-cally filtered with appropriate dia-phragms.

Principle of the set-up for coherent optical filtration.

Tasks:1. Optical filtration of diffraction

objects in 4f set-up.

2. Reconstruction of a filtered image.

Optical base plate with rubber feet 08700.00 1He-Ne-laser, 5 mW with holder* 08701.00 1Power supply for laser head 5 mW* 08702.93 1Adjusting support 35�35 mm 08711.00 2Surface mirror 30�30 mm 08711.01 2Magnetic foot for optical base plate 08710.00 9Holder for diaphragm/beam splitter 08719.00 2Lens, mounted, f = +100 mm 08021.01 3Lensholder for optical base plate 08723.00 3Screen, white, 150�150 mm 09826.00 1Slide -Emperor Maximilian- 82140.00 1Screen, with arrow slit 08133.01 1Diffraction grating, 4 lines/mm 08532.00 1Diffraction grating, 50 lines/mm 08543.00 1Diaphragms, d = 1, 2, 3, 5 mm 09815.00 1Screen, with diffracting elements 08577.02 1Sliding device, horizontal 08713.00 1xy shifting device 08714.00 2Achromatic objective 20� N.A. 0.45 62174.20 1Adapter ring device 08714.01 1Pin hole 30 micron 08743.00 1Ruler, plastic, 200 mm 09937.01 1Ultrasonic generator 11744.93 1Glass cell, 150�55�100 mm 03504.00 1Table with stem 09824.00 2Support rod, stainless steel, 250 mm 02031.00 1Bosshead 02043.00 1Universal clamp 37715.00 1

*Alternative to laser 5 mW, power supply and shutter:Laser, He-Ne 0.2/1.0 mW, 220 V AC 08180.93 1

What you need:


� Fourier transform� Lenses� Fraunhofer diffraction� Index of refraction� Huygens’ principle� Debye-Sears-effect

filter

half plane

Fourier plane P2lens L1object plane P1 lens L2 observationplane SC

Fouriert optics – optical filtration –4 f Arrangement P2261200


P1308011 LDA – Laser Doppler Anemometry with Cobra3

Principle:Small particles in a current passthrough the LDA measuring volumeand scatter the light whose frequen-cy is shifted by the Doppler effectdue to the particle movement. The frequency change of the scat-tered light is detected and convertedinto a particle or flow velocity.

Tasks:1. Measurement of the light-fre-

quency change of individual lightbeams which are reflected bymoving particles.

Measurement of the signal spectrum with a signal peak.

2. Determination of the flow veloci-ties.

Optical base plate with rubber feet 08700.00 1He-Ne-laser, 5 mW with holder 08701.00 1Power supply for laser head 5 mW 08702.93 1Adjusting support 35�35 mm 08711.00 2Surface mirror 30�30 mm 08711.01 2Magnetic foot for optical base plate 08710.00 8Holder for diaphragm/beam splitter 08719.00 1Lens, mounted, f = +100 mm 08021.01 1Lens, mounted, f = +50 mm 08020.01 1Lens, mounted, f = +20 mm 08018.01 1Iris diaphragm 08045.00 1Beam splitter 1/1, non polarizing 08741.00 1Si-Photodetector with Amplifier 08735.00 1Control Unit for Si-Photodetector 08735.99 1Adapter, BNC-socket/4 mm plug pair 07542.27 1Screened cable, BNC, l = 750 mm 07542.11 1Prism table with holder for optical base plate 08725.00 1Lensholder for optical base plate 08723.00 3Screen, white, 150�150 mm 09826.00 1xy shifting device 08714.00 1Pin hole 30 micron 08743.00 1Sliding device, horizontal 08713.00 1LDA-Accessory-Set 08740.00 1Support rod -PASS-, square, l = 630 mm 02027.55 2Right angle clamp -PASS- 02040.55 2Universal clamp 37715.00 2Support base -PASS- 02005.55 1Aspirator bottle, clear glass 1000 ml 34175.00 2Pinchcock, width 10 mm 43631.10 3Glass tubes, straight, 80 mm 36701.65 1Rubber stopper, d = 32/26 mm, 1 hole 39258.01 2Rubber stopper, d = 22/17 mm, 1 hole 39255.01 2Measuring tape, l = 2 m 09936.00 1Spatula, double blade, 150 mm 33460.00 1

What you need:


� Interference� Doppler effect� Scattering of light by small

particles (Mie scattering)� High- and low-pass filters� Sampling theorem� Spectral power density� Turbulence



Silicone tubing di = 7 mm 39296.00 4Glass beaker, short, 150 ml 36012.00 1COBRA3-Basic-Unit 12150.00 1Power supply 12 V/2 A 12151.99 1Data cable, plug/socket, 9 pole 14602.00 1Software Cobra3-Frequency Analyzer 14514.61 1PC, Windows® 95 or higher

LDA – Laser Doppler Anemometrywith Cobra3 P1308011



LH 3 Advanced Optics and Laser Physics

White light hologram with expansion system P1290200

Principle:White light holograms are preparedby allowing the coherent referenceand object waves to strike the holo-gram plate from two different sidesduring image-capture. Interferencelayers are generated in the photo-sensitive material. If the developedhologram is illuminated with whitelight, those layers act as interferencefilters. According to the condition forBragg reflection constructive inter-ference for a specific wavelength can

occur only at certain angles of ob-servation.

Principle of the white light hologram. Image-capture geometry and Braggreflection.

Tasks:Prepare a hologram which can alsobe reconstructed with white light ofa punctiform lightsource (e.g. thesun)


He-Ne-laser, 5 mW with holder 08701.00 1

Power supply for laser head 5 mW 08702.93 1










Object for holography 08749.00 1

Holographic plates, 20 pieces* 08746.00 1

Darkroom equipment for holography 08747.88 1

consisting of:

Plastic trays, 4 pcs. • Laboratory gloves, medium, 100 pcs. • Tray

thermometer, offset, +40°C • Roller squeegee • Clamps, 2 pcs. • Film

tongs, 2 pcs. • Darkroom lamp with green filter • Light bulb 230 V/15 W •

Funnel • Narrow-necked bottles, 4 pcs.

Set of photographic chemicals 08746.88 1

consisting of: Holographic developer • Stop bath • Wetting agent •

Laminate • Paint

Bleaching chemicals:

Potassium dichromate, 250 g 30102.25 1

Sulphuric acid, 95-98%, 500 ml 30219.50 1

What you need:


� Bragg reflection� Object beam� Reference beam� Real and virtual image� Phase holograms� Amplitude holograms� Interference� Diffraction� Developing of film

*Alternative:

Holographic sheet film 08746.01 1

Glass plate, 120�120�2 mm 64819.00 2

White light hologram with expansion systemP1290200



P1290400 Transmission hologram with expansion system

Principle:In contrast to normal photography ahologram can store informationabout the three-dimensionality of anobject. To capture the three-dimen-sionality of an object, the film storesnot only the amplitude but also thephase of the light rays. To achievethis, a coherent light beam (laserlight) is split into an object and a ref-erence beam by being passedthrough a beam splitter. These beamsinterfere in the plane of the holo-graphic film. The hologram is recon-

structed with the reference beamwhich was also used to record thehologram.

Experimental set-up for the image-capture of a transmission hologram usingthe optical expansion system.

Tasks:1. Capture the holographic image of

an object.

2. Perform the development andbleaching of this phase hologram.

3. Reconstruct the transmissionhologram (reconstruction beam isthe reference beam during imagecapture).













Surface mirror, large, d = 80 mm 08712.00 1





consisting of:







Laminate • Paint




What you need:

Transmission hologram with expansion systemP1290400

Advanced Optics and Laser Physics LH 5


� Object beam� Reference beam� Real and virtual image� Phase holograms� Amplitude holograms� Interference� Diffraction� Coherence�Developing of film

*Alternative:


Glass plate, 120�120�2 mm 64819.00 2



LH 6 Advanced Optics and Laser Physics

Transfer hologram from a master hologram P1290500

Principle:After preparing a transmission holo-gram (master hologram) of an object,the reconstructed real image is usedto illuminate a second holographicplate. Thereby a transfer hologram isprepared.

Tasks:Image-capture and reconstructionof a transmission hologram, whichis also termed the master hologram.Reconstruction of the master holo-gram with the phase conjugated

Correct selection of the object position so that the image-capture of a trans-fer hologram is possible.

reference wave R* and image-cap-ture of the transfer hologram,whereby an image-plane hologramshould be generated.













Surface mirror, large, d = 80 mm 08712.00 1





consisting of:







Laminate • Paint




What you need:

Transfer hologram from a master hologramP1290500


� Coherence of light� Object/Reference beam� Real and virtual image� Phase conjugation� Phase/Amplitude holograms� Interference diffraction� Developing of film

*Alternative:


Glass plate, 120�120�2 mm 64819.00 4


Advanced Optics and Laser Physics LH 10


Principle:– In real time procedures, alter-

ations of an object are directly ob-served. A hologram is recordedunder the initial object conditionsand remains in exactly the sameposition (at exactly the sameplace) where it was located duringthe image-capture procedurewhile it is being developed.

– The hologram is reconstructedwith the reference beam and theobject is illuminated with the ob-ject beam (both waves are un-changed with respect to the cap-tured image). The light scatteredby the object interferes with thereconstructed light wave of thehologram.

– During the occurrence of minoralterations (e.g. bending) of theobject, interference fringes be-come visible on observing thehologram.

Experimental set-up for real-time procedures as a holographic interferometerfor a bending plate.

Tasks:Image-capture and reconstructionof a hologram of a plate which iscovered with different masses dur-ing the reconstruction.

Optical base plate in experiment case 08700.01 1He-Ne-laser, 5 mW with holder 08701.00 1Power supply for laser head 5 mW 08702.93 1Magnetic foot for optical base plate 08710.00 7Holder for diaphragm/beam splitter 08719.00 2Sliding device, horizontal 08713.00 1xy shifting device 08714.00 2Adapter ring device 08714.01 1Achromatic objective 20� N.A. 0.45 62174.20 1Pin hole 30 micron 08743.00 1Adjusting support 35�35 mm 08711.00 2Surface mirror 30�30 mm 08711.01 2Surface mirror, large, d = 80 mm 08712.00 1Beam splitter 1/1, non polarizing 08741.00 2Screen, white, 150�150 mm 09826.00 1Slotted weight, 50 g, black 02206.01 2Right angle clamp -PASS- 02040.55 4Cell with magnetic base 08748.00 1Hose clip, diam. 8-12mm 40996.01 2Filter funnel, PP, d = 75 mm 46895.00 1Retort stand, h = 500 mm 37692.00 1Pinchcock, width 15 mm 43631.15 1Ballon flask, HDPE, 10 l 47477.00 1Universal clamp 37715.00 4Holographic sheet film* 08746.01 1Insert for cell 08748.00 for films* 08748.02 1Rubber tubing, vacuum i. d. 6 mm 39286.00 2Gas wash bottle, w/o frit, 250 ml 35834.05 1Manual vacuum pump with manometer* 08745.00 1Silicone grease, 50 g 31863.00 1Silicone tubing, di = 8 mm 47531.00 1

Darkroom equipment for holography 08747.88 1consisting of:Plastic trays, 4 pcs. • Laboratory gloves, medium, 100 pcs. • Traythermometer, offset, +40°C • Roller squeegee • Clamps, 2 pcs. • Filmtongs, 2 pcs. • Darkroom lamp with green filter • Light bulb 230 V/15 W •Funnel • Narrow-necked bottles, 4 pcs.

What you need:

Real time procedure I(bending of a plate) P1290900


� Interference� Optical path length� Refraction index� Phase difference

P1290900 Real time procedure I (bending of a plate)

Set of photographic chemicals 08746.88 1consisting of: Holographic developer • Stop bath • Wetting agent •Laminate • Paint

Bleaching chemicals:Potassium dichromate, 250 g 30102.25 1Sulphuric acid, 95-98%, 500 ml 30219.50 1

*Alternative:Holographic plates, 20 pieces 08746.00 1Insert for cell 08748.00 for plates 08748.01 1



Student System “Advanced Optics” and Laser Physics

Experimental System “Advanced Optics”

This experimental system allows many important experiments in

● Geometrical optics ● Holography● Wave optics ● Interferometry● Applied optics ● Fourier optics

to be performed.

All experiments are supported by corresponding handbooks, which containdetailed descriptions of experimental set-ups and procedures, as well asresults of measurements.

By use of a base plate and magnetically held adjustment devices, which canbe positioned jerkfree, 1 and 2 dimensional measuring set-ups with laser lightsources can be quickly and dependably realized. By deflecting the light path,experiments with larger focal lengths can also be carried out on the baseplate.

The high inherent stiffness and vibration damping of the base plate enablessensitive interferometer arrangements to be set up.Experimental set up for transmission hologram (LH5 – P1290400)

Optical base plate 08700.00For setting up magnetically adheringoptical components. Rigid and vibra-tion-damped working base made ofsteel plate. With corrosion protection,NEXTEL® plastic coating and im-printed grid (5×5) cm. Three fixedadapter sleeves for laser and lasershutter. With rubber feet for non-slipworking. Base plate size (mm) 590×430×24Mass 7 kg

Optical base plate in experimental case 08700.01Design as for base plate 08700.00,however with vibration-dampedstorage in the base of a case. Bottomclamp screws. When carrying out theexperiments, the base plate remainsin the bottom of the case. Separatecase hood with lock.Case dimensions (mm) 620×460×280Mass 13 kg

The practical system enables all im-portant experiments in • Geometric optics• Wave optics (diffraction, interfer-

ence, polarisation and refraction,Kerr and Faraday effect)

• Holography ( white light, transmis-sion and transfer holograms, aver-age time and real time holography)

• Interferometry (Michelson, Mach-Zehnder, Fabry-Perot, Sagnac,Twyman-Green interferometer, aswell as the insert for producingnon-optical phenomena such ase.g. measurement of magnetostric-tions).

• Fourier optics, diffusion of light,optical Doppler effect and laserDoppler anemometry to be carriedout.

With the aid of a base plate and mag-netic adhering holders, which can bepositioned jolt-free, 1 and 2 dimen-sional measuring arrangements canbe quickly and reliably realised usinglaser light sources. By folding thelight paths experiments with largerfocal distances can also be carriedout on the working base. The high stiffness and vibrationdamping of the base plate allowssensitive interferometer arrange-ments to be set up. The base platewith hooded case 08700.01 is rec-ommended for the use of particular-ly vibration-sensitive applications,which is accommodated with partic-ular vibration-damping in the bot-tom of a transport case.

Complete set of interferometer experiments 08700.88

Under the order-no. 08700.88 we offer a complete equipment set to realizethe following 5 types of interferometers: (Please see also page 4 in thisbrochure: Handbook Laser Physics III)

Michelson interferometer (LI 1) Experiment-no. P1306600Sagnac interferometer (LI 4) Experiment-no. P1306900Mach-Zehnder interferometer (LI 10) Experiment-no. P1307500Fabry-Perot interferometer (LI 12) Experiment-no. P1307700Twyman-Green interferometer (LI 18) Experiment-no. P1308100



Equipment Holders

� Magnetic foot for optical base plate 08710.00

Due to internal three-point guide way,stable and highly accurate work hold-ing device for optical componentswith round stems (∅ 10 mm…13 mm).Magnetic base with sliding and attri-tion-free plastic coating for jolt-freepositioning of the optical compo-nents on the base plate. Base height 55 mm

� Adjusting support 35�35 mm 08711.00

For holding optical components (e.g.front surface mirrors). With sensitiveadjustment screws for setting thex,y-position of the optical compo-nents. With round stem l = 75 mmand d = 10 mm.

� Holder for diaphragm/beam plitter 08719.00

Rubber-covered clamping jaws withknurled screws for clamping andholding glass plates, beam splitters,etc. With two round unscrewablestems l = 50 mm and l = 68 mm andd = 10 mm.

� Sliding device, horizontal08713.00

For precise and reproducible linearshift of optical components.Two edge resistant holes for holdingoptical components and a central,linearly adjustable adjustment withspindle drive and scaled, clampableadjustment knob. With round steml = 50 mm and d = 10 mm.Shift range 40 mmAdjustment accuracy 0.1 mm

� XY-shifting device 08714.00For holding and fine positioning op-tical components for extendingbeams (microscope objectives) andspatial filtering (pinhole/apertureplate). With three point bearing andadjusting facility in two mutuallyperpendicular directions, as well asperpendicular to the optical axis inone plane. With clamping pegs forsliding device, horizontal 08713.00.Incl. adjustable aperture plate. x,y-adjustment path max. ± 2 mm

� Adapter ring device08714.01

with internal thread for holding micro-scope objectives (e.g. objective 20×,62174.20) in xy-shifting device08714.00

� Pin hole 30 micron 08743.00For suppressing interference in thelaser light (spatial filter) in connec-tion with microscope objectives. Inframe ∅ = 25 mm.

Adjusting ring 25 � 10 �13 mm 08710.01

For placing and clamping on roundstem optical components, to placethem with a fixed height in magnet-ic feet.

Rot. guide rail with angularscale 08717.00

For reproducible angle adjustment ofoptical components about a freelypositionable pivot. With fixed hold ofcomponents with round stem in thepivot. Swivel rotating track for hold-ing magnet feet for additional com-ponents.Rotating range 360 °Divisions 5 °

� Holder for coaxial laser 08705.00

Holder with three-point bearing forlaser tube ∅ = 30…55 mm. On steml = 65 mm.

� Interferometer plate withprecision drive 08715.00

For precise and reproducible linearshift of optical components e. g. ininterferometer set ups. Suppression of tilting effects due totraverse construction. Position ad-justment through lever device withmicrometer screw. Stiff steel baseplate with NEXTEL®-Plastic coating.Set up on base plate.Shift path max. 0.25 mmResolution 500 nmDimensions (mm) 320×200 ×14Mass 5 kg

� Lens holder for opt. base plate 08723.00

for holding of framed lenses. Designas 08012.00 (s. Page 288), howeverwith short stem l = 35 mm.

� Diaphragm holder 08724.00Design as 08040.00, however withshort stem l = 35 mm.

� Holder for direct vision prismfor opt. base plate 08726.00

Design as 08255.00, however withshort stem l = 50 mm.

� Slit, adjust for opt. baseplate 08727.00


� Prism table for opt. baseplate 08725.00


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Optical Components

� Cell with magnetic base08748.00

For holding holography plates/ filmsfor experiments on real time hologra-phy. Cuvette made of streak-freeglass plates. With 2 hose connec-tions.Dimensions (mm) 200×150×60

� Insert for holographic plates08748.01

Corrosion-proof stainless steel hold-er for standard plates (102×127) mmor even for half-size in cuvette withmagnetic feet 08748.00.Dimensions (mm) 170×130×40

� Insert for holographic films08748.02

Corrosion-proof plexiglass holder forholography films (80×60, 80×100 or127×102) mm. Can be used in cu-vette with magnetic feet 08748.00.The plane film fixing is achieved byproducing low air pressure with theaid of a hand-held vacuum pumpwith manometer 08745.00.Dimensions (mm) 170×130×40

� Object for holography08749.00

Three dimensional model body onmagnetic foot. Total height 17 cm.

�

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�

�

� Surface mirror 08711.01High-quality front-surface planemirror with SiO2- protective coat; onaluminium holder with protectiveedge. Can be used in adjustmentholder 08711.00 Mirror area (mm) 30×30Plan evenness λ/8

� Surface mirror, large 08712.00

High-quality front-surface planemirror with SiO2- protective coat.On holder with round stem l = 76mm. Rear adjustment screws for ad-justing inclination of the mirror inx,y direction.Mirror diameter (mm) 80Plane evenness λ/10

� Concave mirror f = 5 mm, with holder 08720.00

Front-surface mirror ∅ = 10 mm onmagnetic adhering ball joint, mount-ed on round stem l = 110 mm.

� Fresnel mirror for opt. base plate 08728.00

Design as for 08560.00, however withshort stem l = 50 mm.

� Newton colour glass for opt. base plate 08730.02


� Polarisation filter for baseplate 08730.00


� Polarizing filter halfshadefor opt. base plate 08730.01


Kerr cell, PLZT for opt. base plate 08731.00


Photoelement for opt. base plate 08734.00

For determining light intensities.With replaceable holders l = 110 mmand l = 250 mm. Incl. attachableaperture slit d = 0.3 mm.Spectral range 400…1100 nm

Screen, transparent for opt. base plate 08732.00Area (mm) 150×150

� Beam splitter 1/1, non polarizing 08741.00

Semi transparent, non-polarizingglass mirror for separating lightbeam intensity into 50% transmis-sion and 50% reflection. Designedfor wavelength λ = 633 nm.Plate dimensions (mm) 50×30×3.2

� Beam splitter T = 30, R =70, with holder 08741.01

Semi-transparent glass plate for sep-arating light beam intensity into 30 %transmission and 70 % reflection.E.g. for Fabry-Perot interferometer.Mounted on a metal frame.Plate dimensions (mm) 30×20×1.7Frame (mm) 50×30×4

Faraday modulator for opt. base plate 08733.00

Copper coil on temperature-stable alu-minium winder with insert for holdingglass rods (SF58) for Faraday effect(included). With round stem, clampscrews and fixed connection cable l = 1 m with 4-mm jacks.Number of windings 1200Inductivity 6,3 mHOhm’s resistance 4 ΩInternal diameter 14 mmMax. current 5 A (1min)

Rods for magnetotriction, set of 3 08733.01 Ni-, Fe- and Cu-rod with single-sidedM6 thread and silicon hose cover forvibration damping. Can be fixed incoil for magnetostriction 08733.00.Each l = 150 mm, ∅ = 8 mm.

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Special components for holography



Further equipment and components

Holographic plates, 25 pcs. 08746.00Photo plates with extremely high resolution (approx. 6000 Lines/mm). Sensitive for He-Ne-laser light(633 nm). Plate format (127×102) mm.

Holographic sheet films, 50 pcs. 08746.01With extremely high resolution (approx. 6000 Lines/mm). Sensitive for He-Ne-laser light (633 nm).Extent of delivery: 30 pcs (100×80) mm, 50 pcs (80×60) mm.

Set of photographic chemicals 08746.88Consisting of: Developer, stop bath, wetting agent, white paint and laminate.

Dark room equipment for holography 08747.88Consisting of: 4 plastic dishes, darkroom light with green filter and lamp, shell thermometer, roller squeegee,2 clips, 2 photo pincettes, laboratory gloves 100 pcs., funnel and 4 narrow-necked flasks 1000 ml, cleaningset for optical components.

Equipment set for CO2-laser beam analysis 08610.10

With this equipment the experiment P2260400 “CO2-laser” (p. 8) can be extended to:

1. estimating the wavelength by a diffraction grating and2. measuring the distribution of power with the help of a diaphragm

Consists of: (1) Diffraction grating, metal, slit width 0.2 mm, distance of slit centers 0.4 mm, aper-ture diameter: 12 mm, thermal stable up to a power of 8 W/3 mm beam diameter

(2) Diaphragm for powermeter 08579.93 (included in the experiment P2260400), aluminium, black anodised, slit width/diaphragm diameter: 1 mm, thermal loadtolerance: 10 W at 3 mm beam diameter

(3) Sliding device, horizontal, for powermeter sensor, linear adjustment with spindledrive, shift range ±20 mm, with slide mount that goes with the optical benchsupplied with P2260400

(4) Slide mount to hold diffraction grating (1)

IR conversion plate for observation of infrared CO2-laser radiation 08611.10

Using this Thermal Image Plate it is possible to see IR laser beams in real time and with high res-olution. The conversion plate displays IR laser beams through the use of thermal sensitive phos-phors. When illuminated by a long wavelength ultraviolet light (source supplied) these phosphorsfluoresce. The intensity of fluorescence decreases with increasing temperature. When an IR laserbeam strikes the thermal-sensitive surface, the absorbed energy raises the surface temperatureand produces a corresponding thermal image.

Laser beam profiler 08587.00

Consisting of: – CMOS 1,3 mega pixel USB 2.0 camera– Set of neutral density filters– Software for acquisition and analysis of image data

Although special consideration was given to the requirements and problems of laser beam profil-ing during its development, the set is not limited to this function. The software provides tools for2D- as well as 3D-visualization, beam cross section analysis but also for studying e.g. the imageof diffraction patterns. The beam profiler is made for analysing laser beams in the UV, VIS and NIRwavelength range.

Sensor 1 1/8” CMOSPixel Size 6 x 6 µmDynamics 8 bitMax. frame rate 18 fpsSize 34 mm x 32 mm x 27.4 mmThe filters have an optical density of: OD 0.9, OD 1.8, OD 3.0 and OD 4.0 respectively



Further equipment and components

� Helium-Neon-laser 5 mW,with holder 08701.00

Wavelength 632.8 nmTEM00 Modesselection 99%Degree of polarisation 1: 500Beam diameter 0.81 mmBeam divergence 1 mradmax. power drift 2.5 %/8hService life approx. 15000 hCoaxial cylinder casing � = 44.2 mm,

l = 400 mm

With fixed connection cable with HVjack for laser power pack 08702.93Incl. 2 holders with three-point bear-ing 08705.00 and 2 setting collars08710.00

Lasers are ideal, highly monochromatic light sources with excellent coherence and very low beam divergence.

They are particularly suited as light sources for interference, diffraction and holography experiments.

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�

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� Power supply for laser head 5 mW 08702.93

HV supply for laser 08701.00. Withprogrammable timer for selectablehologram light exposure times of0.1s…99 s with the aid of a control-lable shutter. Digital display for pre-selected and expired shutter times.Shutter control via time selection,restart, stop and permanent switch-ing.Plasticcasing (mm) 184×140×130Incl. Shutter � with fixed connec-tion cable with appliance plug; inupright ∅ = 10 mm

Si-Photodetector with amplifier � 08735.00

This silicon photodiode with a built in transconductance amplifier is designed for precision, linearphotometric measurements over 6 decades at high interference levels. It works in connection withthe control unit 08735.99 �.The diode is supplied with a front lens which can be partly covered by a screw-on slit diaphragmfor measurements with a higher local resolution. A second diaphragm, that slides onto the firstone, can be used to alter the entrance aperture in a variable fashion. Thereby it is possible to measure high light intensities without reaching the saturation level of the amplifier.

Spectral range 390 nm…1150 nmMaximum sensitivity at 900 nmBand width DC...65 kHzDiameter of lens aperture approx. 8mmDiaphragm slit aperture max.0.3 mm x 10 mm; min. 0.3 mm x 0.3mm

Control unit for Si-Photodetector � 08735.99

In connection with the Si-Photodetector 08735.00 it serves for photometric measurements of lowdirect- or alternating light signals. It is especially useful for photometric measurements in LDA andfibre optics experiments.It supplies the working voltage for the Si- Photodetector 08735.00. As outputs it offers a monitorsignal, a variable gain output for alternating light signals and an output that is filtered via a band-pass filter (200 Hz…10kHz). The latter output is recommended when low frequency noise (e.g.fluorescent lamps) as well as noise of high frequency has to be suppressed in the light signal.

Input terminal for: Si-Photodetector 08735.00Output, 1 DC…60 kHz, amplification 1 (monitor)Output, 2 AC; 10Hz…60 kHz, amplification 1…10Output, 3 AC; 200Hz…10 kHz, amplification 1…10External power supply 110 VAC…240 VAC, 50/60 Hz

Universal power supply for He-Ne-laser 08701.99

This power supply is suited for He-Ne-laser tubes in the output power range of 0.5…10 mW. Theoutput current of this unit can be varied continuously from 3…10 mA. The value of this current isshown on a digital display. The connection to the laser tubes is made via a high voltage connector.

Power supply 100 V…240 V, AC, 50/60 HzIgnition voltage max. 12 kVWorking voltage max. 4 kVCurrrent output continuous, 3…10 mA

Laser and Accessories

�

�

Class 3B Laser



Laser and Accessories

Danger sign “Laser” 06542.00glass fibre reinforced plastic, 315×220 mm, on a stem, d = 10 mm

Recommended accessories:»PASS« barrel base 02006.55

Protection glasses, 10.6 micrometer (CO2-laser) � 08581.00Protection glasses for He-Ne-laser � 08581.10He-Ne-laser alignment glasses (no picture) 08581.11Protection glasses for Nd:YAG-laser � 08581.20

These laser goggles protect the eyes of the user against scattered light and diffuse reflection of alaser beam. All persons staying in the danger zone of laser radiation must have an appropriate eyeprotection. Before using the goggles you always have to make sure that the laser goggle is suitablefor the intended laser radiation.

Diode Laser 0.2/1.0 mW 08760.99

The PHYWE diode laser is particulary suitable as a light source for interference and diffraction ex-periments. Apart from its compact design it is distinguished by its unbeatable price which makesit a cost-effective alternative to traditional He-Ne-gas lasers.

The diode laser complies which the technical requirements of DIN 60825-1, laser class 2. It isequipped with a key switch, an indicator diode indicating the operating status and an electronicshutter to limit the laser output. It is therefore approved for being used at schools. It comes sup-plied with a support rod (length 180 mm, diameter 10 mm), a power supply unit, an instructionmanual and several test records.

Laser, helium-neon, 0.2/1.0 mW 08180.93linearly polarised light source, very short design. Welded glass tube assures a very long lifetime >18 000 operating hours. Key switch and integrated grey filter to reduce radiation power to 0.2 mW. Screw-in release to deactivate the grey filter.

Anodised aluminium casing with integrated mains power supply, screw-in holding stem, signal lightand required warnings printed on both sides. Fixed mains connecting cable 140 cm.

wavelength 632.8 nmoptical output power

without filter 1.0 mWwith filter 0.2 mW

beam diameter 0.5 mmbeam divergence < 2 mrad.minimum polarisation 500:1max. drift over 8 hours ± 2.5%oscillating mode TEM00lifetime > 18000 hpower requirements 35 VAconnecting voltage 230 V, 50…60 HzFurther connecting voltages on request dimensions (mm) 210×80×40stem diameter 10 mmdistance between middle of beam 180 mmand end of stem

Laser, helium-neon, 1.0 mW 08181.93same design as 08180.93, but without grey filter.

Green Laser 0.2/1 mW; 532 nm 08762.99

Diode-pumped frequency-doubled yttrium vanadate solid-state laser (Nd:YVO4)

Since the human eye is particular sensitive to green light, the beam of this laser is a lot better vis-ible than a red laser with the same output power. Dimensions and the other features correspondto the Diode Laser 08760.99

Laser Class 2Wavelength 532 nmPower output 1 mW/0.2 mWDimensions length 15 cm/∅ 3,5 cm

Including power supply (110 - 230) VACTwo holding rods length 15 cm/8.5 cm, ∅ 10 mm

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Class 2 Laser

Class 2 Laser

Class 2 Laser



Index

AAmplitude holograms 25, 26

Analyser 13

BBabinet’s theorem 10

Birefraction 6

Bragg reflection 25

Brewster angle 6, 7

CCO2-laser 8

Coherence of light 27

Coherence 9, 10, 11, 16, 26

Coherent light 12

Collision of second type 6

DDebye-Sears-effect 23

Developing of film 25, 26, 27

Diffraction index 17, 18, 19, 2021, 22

Diffraction 9, 10, 25, 26

Doppler effect 18, 24

Double refraction 13, 14

EElectric discharge 7

Electromagnetism 15

Electronic oscillation 15

Electro-optical modulator 14

FFabry Perot 6, 21, 22

Faraday effect 15

Ferromagnetic material 19

Fourier optics 23

Fourier transform 23

Fraunhofer diffraction 9

Fraunhofer diffraction 23

Fraunhofer interference 10

Frequency doubling 8

GGas discharge tube 6

HHe-Ne-laser 6

High- and low-pass filters 24

Hologram 25, 26, 27, 28

Huygens’ principle 9. 10, 23

IIndex of refraction 16, 23

Induced emission 8

Induced/Spontaneous emission 7

Interaction of electromagneticfields 15

Interference at thin layers 12

Interference diffraction 9, 11, 22

Interference 16, 25, 26, 28, 17, 1819, 20, 21, 22, 24

Inversion 6, 8

Inversion/Optical amplification 7

KKerr effect 14

LLaser Doppler Anemometry 24

Lenses 23

Light velocity 11, 16

Linearly, circularly and elliptically polarised light 13

Littrow prism 6

Lorentz transformation 18

MMach-Zehnder-Interferometer 20

Magnetostriction 19

Malus' law 13, 15

Michelson Interferometer 11, 1617, 18, 19

Modulation of light 14

Molecular vibration, excitation 7

Multibeam interferometer 21

Multiple beam interference 10

NNd-YAG-laser 7

Newton's colour glass 12

Newton’s rings 12

OObject beam 25, 26

Object/Reference beam 27

Optical anisotropy 14

Optical axis 13

Optical path length 28

Optical pumping 8

Optical resonator 7, 8

Ordinary and extraordinarybeam 13

PPath difference 12

Phase conjugation 22

Phase difference 23

Phase holograms 25, 26

Phase relation 12

Phase 11, 16, 17, 18, 19, 2021, 22

Phase/Amplitude holograms 27

Plane of polarisation 13

Polarisation of light 14

Polarisation 7, 8, 13, 15

Polarizer 13

RReal and virtual image 25, 26, 27

Reference beam 25, 26

Refraction index 11, 16, 28

Relaxation 8

Resonator cavity 6

Resonator modes 8

SSampling theorem 24

Scattering of light bysmallparticles (Mie scattering) 24

Special relativity theory 18

Spectral power density 24

Spectrum of emission 7

Speed of light 17, 18, 19, 2021, 22

Spin-orbit coupling 19

Spontaeous emission 8

Spontaneous andstimulated light emission 6

TTemporal coherence 18

Transverse and longitudinalresonator modes 6

Turbulence 24

Two-beam interferometer 22

VVerdet’s constant 15

Vibration/Rotation niveau 7

Virtual light source 11, 16, 17, 1819, 20, 21, 22

WWavelength 11, 16, 17, 18, 19

20, 21, 22

Weiss molecular magneticfields 19



How to order

Quantity

Order No.

Please specify thisOrder No. if you wouldlike to order the completeexperiment.

The experiments can be offered or ordered completely or partially, if desired, in accordance with the

comprehensive equipment lists. On request, we will gladly send you detailed experimental descriptions.

You can order the experiments as follows:

� Didactically adap-ted descriptions ofexperiments – easy,direct preparationby the students ispossible

� Comprehensive experiments – cover the entire range of classicaland modern optics

� Developed and proven bypracticians – unproblematical andreliable performance

� Complete equipment offeringmodular experimental set-up –multiple use of individual devices,cost effective and flexible

� Excellent measurement accuracy – results agree with theory

� Computer-assisted experiments –simple, rapid assessement of theresults

Optical base plate in exp. case 08700.01 1He-Ne-laser, 5 mW with holder 08701.00 1Power supply for laser head 5 mW 08702.93 1Magnetic foot for optical base plate 08710.00 6Holder for diaphragm/beam splitter 08719.00 2Sliding device, horizontal 08713.00 1xy shifting device 08714.00 2Adapter ring device 08714.01 1Achromatic objective 20� N.A. 0.45 62174.20 1Pin hole 30 micron 08743.00 1Adjusting support 35�35 mm 08711.00 2Surface mirror 30�30 mm 08711.01 2Surface mirror, large, d = 80 mm 08712.00 1Beam splitter 1/1, non polarizing 08741.00 1Object for holography 08749.00 1Holographic plates, 20 pieces* 08746.00 1

Darkroom equipment for holography 08747.88 1consisting of:Plastic trays, 4 pcs. • Laboratory gloves, medium, 100 pcs. • Traythermometer, offset, +40°C • Roller squeegee • Clamps, 2 pcs. • Filmtongs, 2 pcs. • Darkroom lamp with green filter • Light bulb 230 V/15 W •Funnel • Narrow-necked bottles, 4 pcs.

Set of photographic chemicals 08746.88 1consisting of: Holographic developer • Stop bath •Wetting agent • Laminate • Paint

Bleaching chemicals:Potassium dichromate, 250 g 30102.25 1Sulphuric acid, 95-98%, 500 ml 30219.50 1

*Alternative:Holographic sheet film 08746.01 1Glass plate, 120�120�2mm 64819.00 2

What you need:

Transmission hologram with expansion system P1290400

All additional nessecaryitems are mentioned (e.g. spare parts).

Where applicablealternatives are alsomentioned.


37

Send to Fax No. (00 49) 5 51 60 41 15or by postor contact our local representative

PHYWE Systeme GmbH & Co. KG

D-37070 GöttingenFederal Republic of Germany

Address of institution

Telephone Fax

Date Signature

Please circle the corresponding experiment numbers

Information / Quotation

Please send detailed descriptions, free of charge

Please send an offer for the following experiments

P2260700 P2260400 P2260900 P1216800 P1216900

P1217100 P1217200 P1217400 P1217600 P1217700

P1218000 P1290200 P1290400 P1290500 P1290900

P1306700 P1307000 P1307100 P1307500 P1307700

P1307800 P2261200 P1308000


38

Send to Fax No. (00 49) 5 51 60 41 15or by postor contact our local representative

PHYWE Systeme GmbH & Co. KG

D-37070 GöttingenFederal Republic of Germany

Address of institution

Telephone Fax

Date Signature

Equipment Article-No. Quantity

Information / Quotation

Please send an offer for the following equipment


PHYSICS – CHEMISTRY – BIOLOGY

The comprehensive catalogue for physics, chemistry

and biology. Additionally you can find a large number of

laboratory materials and an insight in our particularly

successful teaching systems TESS, Cobra3 and

Natural Sciences on the board.

Available in English and Spanish.

Laboratory Experiments

The experiments in the Phywe publication series “Laboratory Experiments”

are intended for the heads of laboratories,

colleges of advanced technology, technical

colleges and similar institutions and also

for advanced courses in high schools.

Laboratory Experiments is

also available on CD-ROM.

Available in English.

Special brochures

Additionally there are special brochu-

res for our particularly successful

teaching systems TESS (available in

German, English, French and Spanish),

Cobra3 (available in German, English)

and Natural Sciences on the board

(available in German, English).

– catalogues, brochures and more…

PHYSICS · CHEMISTRY · BIOLOGY


12.06.05 Order No. 00117.02

PHYWE SYSTEME GmbH & Co. KGRobert-Bosch-Breite 10

D-37079 GöttingenGermany

phone: ++49/551/604-0fax: ++49/551/604-115

int.sales@ phywe.comwww.phywe.com


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