Science: v.1-v.219Moses King, 1965 |
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Page 839
... optical sys- tems without violating the well - known brightness laws of optics . This brings us to a fourth important property , the intensity or brightness which can be achieved by maser tech- niques . As indicated initially , once one ...
... optical sys- tems without violating the well - known brightness laws of optics . This brings us to a fourth important property , the intensity or brightness which can be achieved by maser tech- niques . As indicated initially , once one ...
Page 1360
... optical systems , standard optical instru- ments , optical systems specially suited for laboratory use , experimental de- termination of properties of optical systems , and effects of misalignment of optical components . The tuition is ...
... optical systems , standard optical instru- ments , optical systems specially suited for laboratory use , experimental de- termination of properties of optical systems , and effects of misalignment of optical components . The tuition is ...
Page 1381
... optical - density peak is at 19S . The radioactive peaks are at 16S , 12S , and 4S from left to right along the gradient . DENSITY 280 my OPTICAL Q.2- 28 A 0.14 QD . 0.2- 0.1- 0.2- Q11 C 10 20 30 10 30 20 30 FRACTION NUMBER -300 F200 ...
... optical - density peak is at 19S . The radioactive peaks are at 16S , 12S , and 4S from left to right along the gradient . DENSITY 280 my OPTICAL Q.2- 28 A 0.14 QD . 0.2- 0.1- 0.2- Q11 C 10 20 30 10 30 20 30 FRACTION NUMBER -300 F200 ...
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