Using low and high prepulses to enhance the J=0-1 transition at 19.6 nm in the Ne-like germanium XUV laser
We report a study of the effect of prepulses on XUV lasing of Ne-like germanium for an irradiation geometry where ≈20 mm long germanium slab targets were irradiated at ≈1.6 × 1013 W cm-2 using ≈0.7 ns (1.06 μm) pulses from the VULCAN glass laser. Prepulses were generated at fractional power levels o...
| Auteurs principaux: | , , , , , , , , , , , , |
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| Format: | Journal article |
| Langue: | English |
| Publié: |
1996
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| _version_ | 1826257013678538752 |
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| author | Cairns, G Lewis, C Lamb, M MacPhee, A Neely, D Norreys, P Key, M Healy, S Holden, P Pert, G Plowes, J Tallents, G Demir, A |
| author_facet | Cairns, G Lewis, C Lamb, M MacPhee, A Neely, D Norreys, P Key, M Healy, S Holden, P Pert, G Plowes, J Tallents, G Demir, A |
| author_sort | Cairns, G |
| collection | OXFORD |
| description | We report a study of the effect of prepulses on XUV lasing of Ne-like germanium for an irradiation geometry where ≈20 mm long germanium slab targets were irradiated at ≈1.6 × 1013 W cm-2 using ≈0.7 ns (1.06 μm) pulses from the VULCAN glass laser. Prepulses were generated at fractional power levels of ≈2 × 10-4 (low) and ≈2 × 10-2 (high) and arrived on target 5 and 3.2 ns respectively in advance of the main heating pulse. For both the low and high prepulses the output of the 3p-3s, J=0-1, line at 19.6 nm was enhanced such that the peak radiant density (J/st) for this line became greater than that for the normally stronger J=2-1 lines at 23.2 and 23.6 nm. The 7=0-1 line, whose FWHM duration was reduced from ≈450 ps to ≈100 ps, delivered ≈6X more power (W) than the average for the combined J=2-1 lines, whose FWHM duration was ≈500 ps for both levels of prepulse. The higher prepulse was more effective, yielding ≈2X more radiant density and ≈7X more power on both the J=0-1 and J=2-1 transitions compared to the low prepulse case. The most dramatic observation overall was the ≈40X increase of power in the J=0-1 line for the high prepulse (≈2%) case compared with the zero prepulse case. These observations, coupled with measurements of beam divergence and beam deviation through refractive bending, as well as general agreement with modelling, lead us to conclude that, for germanium, the main influence of the prepulse is (a) to increase the energy absorbed from the main pulse, (b) to increase the volume of the gain zone and (c) to relax the plasma density gradients, particularly in the J=0-1 gain zone. |
| first_indexed | 2024-03-06T18:11:24Z |
| format | Journal article |
| id | oxford-uuid:032a8e10-c632-4ce3-b25b-f1237a2d3ef4 |
| institution | University of Oxford |
| language | English |
| last_indexed | 2024-03-06T18:11:24Z |
| publishDate | 1996 |
| record_format | dspace |
| spelling | oxford-uuid:032a8e10-c632-4ce3-b25b-f1237a2d3ef42022-03-26T08:44:26ZUsing low and high prepulses to enhance the J=0-1 transition at 19.6 nm in the Ne-like germanium XUV laserJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:032a8e10-c632-4ce3-b25b-f1237a2d3ef4EnglishSymplectic Elements at Oxford1996Cairns, GLewis, CLamb, MMacPhee, ANeely, DNorreys, PKey, MHealy, SHolden, PPert, GPlowes, JTallents, GDemir, AWe report a study of the effect of prepulses on XUV lasing of Ne-like germanium for an irradiation geometry where ≈20 mm long germanium slab targets were irradiated at ≈1.6 × 1013 W cm-2 using ≈0.7 ns (1.06 μm) pulses from the VULCAN glass laser. Prepulses were generated at fractional power levels of ≈2 × 10-4 (low) and ≈2 × 10-2 (high) and arrived on target 5 and 3.2 ns respectively in advance of the main heating pulse. For both the low and high prepulses the output of the 3p-3s, J=0-1, line at 19.6 nm was enhanced such that the peak radiant density (J/st) for this line became greater than that for the normally stronger J=2-1 lines at 23.2 and 23.6 nm. The 7=0-1 line, whose FWHM duration was reduced from ≈450 ps to ≈100 ps, delivered ≈6X more power (W) than the average for the combined J=2-1 lines, whose FWHM duration was ≈500 ps for both levels of prepulse. The higher prepulse was more effective, yielding ≈2X more radiant density and ≈7X more power on both the J=0-1 and J=2-1 transitions compared to the low prepulse case. The most dramatic observation overall was the ≈40X increase of power in the J=0-1 line for the high prepulse (≈2%) case compared with the zero prepulse case. These observations, coupled with measurements of beam divergence and beam deviation through refractive bending, as well as general agreement with modelling, lead us to conclude that, for germanium, the main influence of the prepulse is (a) to increase the energy absorbed from the main pulse, (b) to increase the volume of the gain zone and (c) to relax the plasma density gradients, particularly in the J=0-1 gain zone. |
| spellingShingle | Cairns, G Lewis, C Lamb, M MacPhee, A Neely, D Norreys, P Key, M Healy, S Holden, P Pert, G Plowes, J Tallents, G Demir, A Using low and high prepulses to enhance the J=0-1 transition at 19.6 nm in the Ne-like germanium XUV laser |
| title | Using low and high prepulses to enhance the J=0-1 transition at 19.6 nm in the Ne-like germanium XUV laser |
| title_full | Using low and high prepulses to enhance the J=0-1 transition at 19.6 nm in the Ne-like germanium XUV laser |
| title_fullStr | Using low and high prepulses to enhance the J=0-1 transition at 19.6 nm in the Ne-like germanium XUV laser |
| title_full_unstemmed | Using low and high prepulses to enhance the J=0-1 transition at 19.6 nm in the Ne-like germanium XUV laser |
| title_short | Using low and high prepulses to enhance the J=0-1 transition at 19.6 nm in the Ne-like germanium XUV laser |
| title_sort | using low and high prepulses to enhance the j 0 1 transition at 19 6 nm in the ne like germanium xuv laser |
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