I have also used a single set of 6X Cylindricals to correct the NDG7475/NUBM07E diode combination with very good results.
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It does not matter what LD you rotate the polarization/EM field on...Pick one.
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OK..to get the best match up...the best Beam-on-Beam ( BoB)....the nearfield geometry of both beams..... must enter the PBS cube with the fast axis being perpendicular to your optical base plate/plane.
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This means that the geometry that you need to see on the entry surface of the PBS cube is....
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a small vertical bar...going up/down on one (1) entry side.....Let us call this the " Main Beam " and....
a small vertical bar...going up/down on another entry side... which is right next to the " Main Beam " side.....Let us call this the " Secondary Beam " . These entry sides are at a 90 degree relationship to one another.
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You will see a plane within the PBS cube...This is where the two prism's that make up the PBS cube are joined. On this internal plane....both beam geometries....( The Main Beam and the Secondary beam) must be over layed ...or...in a Beam -on- Beam state to accomplish optimal beam combination / alignment. BUT.....but...
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For the PBS cube to be able to combine the beams...the polarization of one (1) beam must be at 90 degree to the other beam. Well....to rotate the polarization....you only have two (2) options; 1) Physically...rotate the LD, 2) Leave the LD alone....and use a waveplate filter to optically rotate the polarization field by 90 degree.
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You cannot rotate the LD....for that would cause you to lose the BoB condition/state.....SOoooo....you place a Waveplate optic in the beam bath of one of your diodes...again....it does not matter which one....Green or Blue.....the photons do not care ...HAHAHA
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Now....with the waveplate in place.....you must rotate this waveplate in an radial fashion...rotating the optic about it's central axis to locate the best radial position. This best position is determined by using a Power Meter and rotating the optic. The position at which you achieve the greatest optical power of your Secondary beam as it propagates out of the PBS cube.....is the where you want to lock down your waveplate optic.
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When the waveplate is in the best position....you have rotated a single beam Polarization by 90 degree....but have not changed the beam nearfield geometry....and this is what you want.....SOooo....now....both beams enter the PBS cube.....with the fast axis perpendicular to your optical plane ( " l " bar shape going up/down )....and...because you've rotated the Electromagnetic Polarization field with the wavelate....the PBS can now combine your beams.
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Now....as the combined beams exit the PBS cube....they then prop into the Cylindrical Lens set. AND...a big AND...both beams are in the correct orientation for the Cylinderical lens set to expand the slow axis....so...This " l " becomes this " # "... and the C-Set corrects the astigmatic beam geometry. Out pops two (2) corrected beams....with a close to 1:1 aspect ratio....closer to a circle...again...not a perfect Gaussian circle....but....for our purposes....very good for projector application.
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Hmmm...Do I get paid by the word ???? I hope all the above makes sense....if not...refer to Beam Axiom #2
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Happy New Year...to all you "Photon Phanitics"
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CDBEAM
Last edited by CDBEAM; 12-27-2016 at 17:36.
Reason: Corrected explaination of PBS operation and added more explaination blah, blah
Beam Axiom #1 ~The Quantum well is DEEP ! Photons for ALL !!
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Beam Axiom #2 ~Yes...As a matter of fact...I DO wear tinfoil on my head !!
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Beam Axiom #3 ~Whe'n dout...Po ah Donk awn et !!
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Beam Axiom #4 ~A Chicken in every Pot, and a Laser Lumia in every Livingroom !!
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Beam Axiom #5 ~"Abstract Photonic Expressionism"....is "Abstractonimical" !!
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Beam Axiom #6 ~ "A Posse ad Essea" ~ From being possible to being actual ...is the beam target !