Metallic and non-metallic coatings for inertial confinement fusion targets
Some fusion targets designed to be driven by 0.35-1 microm laser light are glass spheres coated with layers of various materials such as hydrocarbons, fluorocarbons, beryllium, copper, gold, platinum etc. The glass shell, which is filled with gas, liquid or solid deuterium-tritium fuel, must have re...
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| Autor*in: |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
1981 |
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| Reproduktion: |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
|---|---|
| Übergeordnetes Werk: |
in: Thin Solid Films - Amsterdam : Elsevier, 83(1981), 1, Seite 61-72 |
| Übergeordnetes Werk: |
volume:83 ; year:1981 ; number:1 ; pages:61-72 |
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| 520 | |a Some fusion targets designed to be driven by 0.35-1 microm laser light are glass spheres coated with layers of various materials such as hydrocarbons, fluorocarbons, beryllium, copper, gold, platinum etc. The glass shell, which is filled with gas, liquid or solid deuterium-tritium fuel, must have remarkably good surface and wall thickness uniformity. To avoid the development of Rayleigh-Taylor instabilities which reduce the effectiveness of the implosion in achieving both the high density and the high temperature necessary for efficient thermonuclear deuterium-tritium interactions, the surface irregularities should be of the order of 100 Å or less and wall thickness variations should be limited to 1% or less of the thickness. It is further required that irregularities of the surface should be small enough (or absent) to avoid nucleating variations in coatings as they are deposited. Each layer applied must conform to the same uniformity requirements. Methods for depositing the various materials will be discussed. They include plasma polymerization, electrodeposition, sputtering and evaporation. Many of the difficulties encountered in the coating processes are the result of coating on free spheres with very small radii (35-500 microm). Several means of overcoming the problems are described and experimental results are presented. | ||
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(DE-627)NLEJ178986429 (DE-599)GBVNLZ178986429 DE-627 ger DE-627 rakwb eng Metallic and non-metallic coatings for inertial confinement fusion targets 1981 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Some fusion targets designed to be driven by 0.35-1 microm laser light are glass spheres coated with layers of various materials such as hydrocarbons, fluorocarbons, beryllium, copper, gold, platinum etc. The glass shell, which is filled with gas, liquid or solid deuterium-tritium fuel, must have remarkably good surface and wall thickness uniformity. To avoid the development of Rayleigh-Taylor instabilities which reduce the effectiveness of the implosion in achieving both the high density and the high temperature necessary for efficient thermonuclear deuterium-tritium interactions, the surface irregularities should be of the order of 100 Å or less and wall thickness variations should be limited to 1% or less of the thickness. It is further required that irregularities of the surface should be small enough (or absent) to avoid nucleating variations in coatings as they are deposited. Each layer applied must conform to the same uniformity requirements. Methods for depositing the various materials will be discussed. They include plasma polymerization, electrodeposition, sputtering and evaporation. Many of the difficulties encountered in the coating processes are the result of coating on free spheres with very small radii (35-500 microm). Several means of overcoming the problems are described and experimental results are presented. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Hendricks, C.D. oth Crane, J.K. oth Hsieh, E.J. oth Meyer, S.F. oth in Thin Solid Films Amsterdam : Elsevier 83(1981), 1, Seite 61-72 (DE-627)NLEJ177331380 (DE-600)1482896-0 0040-6090 nnns volume:83 year:1981 number:1 pages:61-72 http://linkinghub.elsevier.com/retrieve/pii/0040-6090(81)90587-3 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 83 1981 1 61-72 |
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Metallic and non-metallic coatings for inertial confinement fusion targets |
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Some fusion targets designed to be driven by 0.35-1 microm laser light are glass spheres coated with layers of various materials such as hydrocarbons, fluorocarbons, beryllium, copper, gold, platinum etc. The glass shell, which is filled with gas, liquid or solid deuterium-tritium fuel, must have remarkably good surface and wall thickness uniformity. To avoid the development of Rayleigh-Taylor instabilities which reduce the effectiveness of the implosion in achieving both the high density and the high temperature necessary for efficient thermonuclear deuterium-tritium interactions, the surface irregularities should be of the order of 100 Å or less and wall thickness variations should be limited to 1% or less of the thickness. It is further required that irregularities of the surface should be small enough (or absent) to avoid nucleating variations in coatings as they are deposited. Each layer applied must conform to the same uniformity requirements. Methods for depositing the various materials will be discussed. They include plasma polymerization, electrodeposition, sputtering and evaporation. Many of the difficulties encountered in the coating processes are the result of coating on free spheres with very small radii (35-500 microm). Several means of overcoming the problems are described and experimental results are presented. |
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Some fusion targets designed to be driven by 0.35-1 microm laser light are glass spheres coated with layers of various materials such as hydrocarbons, fluorocarbons, beryllium, copper, gold, platinum etc. The glass shell, which is filled with gas, liquid or solid deuterium-tritium fuel, must have remarkably good surface and wall thickness uniformity. To avoid the development of Rayleigh-Taylor instabilities which reduce the effectiveness of the implosion in achieving both the high density and the high temperature necessary for efficient thermonuclear deuterium-tritium interactions, the surface irregularities should be of the order of 100 Å or less and wall thickness variations should be limited to 1% or less of the thickness. It is further required that irregularities of the surface should be small enough (or absent) to avoid nucleating variations in coatings as they are deposited. Each layer applied must conform to the same uniformity requirements. Methods for depositing the various materials will be discussed. They include plasma polymerization, electrodeposition, sputtering and evaporation. Many of the difficulties encountered in the coating processes are the result of coating on free spheres with very small radii (35-500 microm). Several means of overcoming the problems are described and experimental results are presented. |
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Some fusion targets designed to be driven by 0.35-1 microm laser light are glass spheres coated with layers of various materials such as hydrocarbons, fluorocarbons, beryllium, copper, gold, platinum etc. The glass shell, which is filled with gas, liquid or solid deuterium-tritium fuel, must have remarkably good surface and wall thickness uniformity. To avoid the development of Rayleigh-Taylor instabilities which reduce the effectiveness of the implosion in achieving both the high density and the high temperature necessary for efficient thermonuclear deuterium-tritium interactions, the surface irregularities should be of the order of 100 Å or less and wall thickness variations should be limited to 1% or less of the thickness. It is further required that irregularities of the surface should be small enough (or absent) to avoid nucleating variations in coatings as they are deposited. Each layer applied must conform to the same uniformity requirements. Methods for depositing the various materials will be discussed. They include plasma polymerization, electrodeposition, sputtering and evaporation. Many of the difficulties encountered in the coating processes are the result of coating on free spheres with very small radii (35-500 microm). Several means of overcoming the problems are described and experimental results are presented. |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">NLEJ178986429</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706090812.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1981 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ178986429</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ178986429</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Metallic and non-metallic coatings for inertial confinement fusion targets</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1981</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Some fusion targets designed to be driven by 0.35-1 microm laser light are glass spheres coated with layers of various materials such as hydrocarbons, fluorocarbons, beryllium, copper, gold, platinum etc. The glass shell, which is filled with gas, liquid or solid deuterium-tritium fuel, must have remarkably good surface and wall thickness uniformity. To avoid the development of Rayleigh-Taylor instabilities which reduce the effectiveness of the implosion in achieving both the high density and the high temperature necessary for efficient thermonuclear deuterium-tritium interactions, the surface irregularities should be of the order of 100 Å or less and wall thickness variations should be limited to 1% or less of the thickness. It is further required that irregularities of the surface should be small enough (or absent) to avoid nucleating variations in coatings as they are deposited. Each layer applied must conform to the same uniformity requirements. Methods for depositing the various materials will be discussed. They include plasma polymerization, electrodeposition, sputtering and evaporation. Many of the difficulties encountered in the coating processes are the result of coating on free spheres with very small radii (35-500 microm). Several means of overcoming the problems are described and experimental results are presented.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Elsevier Journal Backfiles on ScienceDirect 1907 - 2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Hendricks, C.D.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Crane, J.K.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Hsieh, E.J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Meyer, S.F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Thin Solid Films</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">83(1981), 1, Seite 61-72</subfield><subfield code="w">(DE-627)NLEJ177331380</subfield><subfield code="w">(DE-600)1482896-0</subfield><subfield code="x">0040-6090</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:83</subfield><subfield code="g">year:1981</subfield><subfield code="g">number:1</subfield><subfield code="g">pages:61-72</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0040-6090(81)90587-3</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_H</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SDJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">83</subfield><subfield code="j">1981</subfield><subfield code="e">1</subfield><subfield code="h">61-72</subfield></datafield></record></collection>
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