text stringlengths 0 205 |
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align:start position:0% |
also |
align:start position:0% |
also |
tune |
align:start position:0% |
align:start position:0% |
across the gain curve |
align:start position:0% |
align:start position:0% |
of the cavity I |
align:start position:0% |
of the cavity I |
align:start position:0% |
of the cavity I |
mean I gain curve of the of the medium |
align:start position:0% |
mean I gain curve of the of the medium |
align:start position:0% |
mean I gain curve of the of the medium |
of the of the laser |
align:start position:0% |
align:start position:0% |
so in in summary then we've seen that |
align:start position:0% |
so in in summary then we've seen that |
align:start position:0% |
so in in summary then we've seen that |
for this laser here that's about 22 |
align:start position:0% |
for this laser here that's about 22 |
align:start position:0% |
for this laser here that's about 22 |
centimeters apart that we get |
align:start position:0% |
centimeters apart that we get |
align:start position:0% |
centimeters apart that we get |
longitudinal modes of 680 megahertz |
align:start position:0% |
longitudinal modes of 680 megahertz |
align:start position:0% |
longitudinal modes of 680 megahertz |
apart and |
align:start position:0% |
apart and |
align:start position:0% |
apart and |
the polarization of each mode is is |
align:start position:0% |
the polarization of each mode is is |
align:start position:0% |
the polarization of each mode is is |
different in fact they have adjacent |
align:start position:0% |
different in fact they have adjacent |
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