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Thanks, those links lead me to this page on prisms: http://www.nitto-optical.co.jp/english/products/basic_prism/index.html
Edit: I'm going to edit in something I was looking at today, that's the perceived brightness of 660nm compared to 638nm, using RHD's online calculator, found in my signature, I'm seeing 1.4 watts of 638nm is just as bright to the eye as 5 watts of 660nm. Due to this, I'm looking for a higher power single beam output 638nm diode, but only finding a 700mw rated Oclaro diode right now, but the good thing is they are cheap. I could combine them together using a cube to give close to 1.4 watts, if pushed hard. This would give me the same amount of brilliance as the more expensive 5 watt 660nm but at the cost of simplicity.
Here's a RHD comparison of the brightness:
If you look at the way Mateusz Szymański of Opt Lasers or ebay/tomorrowssystem combines two relatively inexpensive 700mw 638nm red diodes, this is how complex it gets, below. Although when you consider the cost of the extra optics & diode holder, the price isn't so cheap.
I see he uses a rotator for the output of one and places the diode holders at different distances, still trying to understand why he did that when you could just turn the diode to adjust polarity for one (there must be more to it than that) and for the distance question, I am clueless.
Another edit: Mateusz got back to me with a answer to my question about the wave rotator, if you don't use it, you have a cross shape, this rotates the shape of the laser diode output. Here was his answer:
"If you don't use it the output beam will be in cross shape. If you use it joined beams can be in the same position for example horizontal. So you do not have cross effect."
I guess the wave rotator not only corrects the orientation of the beam, but rotates the polarity at the same time? The only reason I am questioning this is I thought I once saw a wave rotator which only changed the polarity leaving the beam the same shape.
This is a an idea which might be something I can do, maybe I should find dicro's which will allow me to combine 638nm and 660nm together so I can get higher power red without needing a cube which has more loss? I'm wondering if there are dicro's which are "tuned" to such specific frequencies to allow one to pass through and the other to reflect, maybe these two wavelengths are just too close together to do that. I wouldn't use a 5 watt 660nm and a 700mw 638nm diode this way, just looking at this as a method of using a less expensive 660nm diode together with a cheap 638nm diode to allow me to throw out the losses a cube would produce, only draw back is a lower power 660nm diode just doesn't add as much brilliance to the eye which puts me right back to using a cube, either that or using the high power 5 watt diode to make up for it, arrggg! I'm lost in the wilds walking in a circle
Edit: I'm going to edit in something I was looking at today, that's the perceived brightness of 660nm compared to 638nm, using RHD's online calculator, found in my signature, I'm seeing 1.4 watts of 638nm is just as bright to the eye as 5 watts of 660nm. Due to this, I'm looking for a higher power single beam output 638nm diode, but only finding a 700mw rated Oclaro diode right now, but the good thing is they are cheap. I could combine them together using a cube to give close to 1.4 watts, if pushed hard. This would give me the same amount of brilliance as the more expensive 5 watt 660nm but at the cost of simplicity.
Here's a RHD comparison of the brightness:
If you look at the way Mateusz Szymański of Opt Lasers or ebay/tomorrowssystem combines two relatively inexpensive 700mw 638nm red diodes, this is how complex it gets, below. Although when you consider the cost of the extra optics & diode holder, the price isn't so cheap.
I see he uses a rotator for the output of one and places the diode holders at different distances, still trying to understand why he did that when you could just turn the diode to adjust polarity for one (there must be more to it than that) and for the distance question, I am clueless.
Another edit: Mateusz got back to me with a answer to my question about the wave rotator, if you don't use it, you have a cross shape, this rotates the shape of the laser diode output. Here was his answer:
"If you don't use it the output beam will be in cross shape. If you use it joined beams can be in the same position for example horizontal. So you do not have cross effect."
I guess the wave rotator not only corrects the orientation of the beam, but rotates the polarity at the same time? The only reason I am questioning this is I thought I once saw a wave rotator which only changed the polarity leaving the beam the same shape.
This is a an idea which might be something I can do, maybe I should find dicro's which will allow me to combine 638nm and 660nm together so I can get higher power red without needing a cube which has more loss? I'm wondering if there are dicro's which are "tuned" to such specific frequencies to allow one to pass through and the other to reflect, maybe these two wavelengths are just too close together to do that. I wouldn't use a 5 watt 660nm and a 700mw 638nm diode this way, just looking at this as a method of using a less expensive 660nm diode together with a cheap 638nm diode to allow me to throw out the losses a cube would produce, only draw back is a lower power 660nm diode just doesn't add as much brilliance to the eye which puts me right back to using a cube, either that or using the high power 5 watt diode to make up for it, arrggg! I'm lost in the wilds walking in a circle
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