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okay were going to talk more particularly about narrow bandpass filters we saw earlier this morning if I have a high index quarter wave and then a half wave and a half wave everythings going to go as though there was no coating if I get a high index like germanium now Im going to have a high reflection in here but again at the half wave nothing so the since were only talking numbers here we dont have to talk about real materials we can imagine an index of 8 or 16 or 32 but theyre not real materials in our spectral region at least but its only numbers we can do anything put in a computer dont have to make it yet but the interesting thing is if I turn that chart upside down all of a sudden what Ive got is a filter which passes this narrow band so this is the basis of the narrow bandpass filter so what do we have here if I have a slab of very high index that happens to be a half-wave thick because this is a very high index in air this is a very high reflector and similar to this