Numerical studies on capillary discharges as focusing elements for electron beams
Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowi...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Brentegani, E. [verfasserIn] Anania, M.P. [verfasserIn] Atzeni, S. [verfasserIn] Biagioni, A. [verfasserIn] Chiadroni, E. [verfasserIn] Croia, M. [verfasserIn] Ferrario, M. [verfasserIn] Filippi, F. [verfasserIn] Marocchino, A. [verfasserIn] Mostacci, A. [verfasserIn] Pompili, R. [verfasserIn] Romeo, S. [verfasserIn] Schiavi, A. [verfasserIn] Zigler, A. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2018 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Nuclear instruments & methods in physics research / A - Amsterdam : North-Holland Publ. Co., 1984, 909, Seite 404-407 |
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| Übergeordnetes Werk: |
volume:909 ; pages:404-407 |
| DOI / URN: |
10.1016/j.nima.2018.03.012 |
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| Katalog-ID: |
ELV001178342 |
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| 245 | 1 | 0 | |a Numerical studies on capillary discharges as focusing elements for electron beams |
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| 520 | |a Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowing in the lens causes beam emittance growth and increases the minimum achievable spot size. To study the physics of the capillary discharge processes employed as active plasma lenses, we developed a 2-D hydrodynamic computational model. Here, we present preliminary simulation results and we compare the computed magnetic field profile with one from literature, which has been experimentally inferred. The result of the comparison is discussed. | ||
| 650 | 4 | |a Active plasma lens | |
| 650 | 4 | |a Plasma lens | |
| 650 | 4 | |a Plasma hydrodynamics | |
| 650 | 4 | |a Hydrogen discharge | |
| 650 | 4 | |a Gas filled capillary | |
| 650 | 4 | |a Capillary discharge simulation | |
| 700 | 1 | |a Anania, M.P. |e verfasserin |4 aut | |
| 700 | 1 | |a Atzeni, S. |e verfasserin |4 aut | |
| 700 | 1 | |a Biagioni, A. |e verfasserin |4 aut | |
| 700 | 1 | |a Chiadroni, E. |e verfasserin |4 aut | |
| 700 | 1 | |a Croia, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Ferrario, M. |e verfasserin |4 aut | |
| 700 | 1 | |a Filippi, F. |e verfasserin |4 aut | |
| 700 | 1 | |a Marocchino, A. |e verfasserin |4 aut | |
| 700 | 1 | |a Mostacci, A. |e verfasserin |4 aut | |
| 700 | 1 | |a Pompili, R. |e verfasserin |4 aut | |
| 700 | 1 | |a Romeo, S. |e verfasserin |4 aut | |
| 700 | 1 | |a Schiavi, A. |e verfasserin |4 aut | |
| 700 | 1 | |a Zigler, A. |e verfasserin |4 aut | |
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10.1016/j.nima.2018.03.012 doi (DE-627)ELV001178342 (ELSEVIER)S0168-9002(18)30341-3 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Brentegani, E. verfasserin aut Numerical studies on capillary discharges as focusing elements for electron beams 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowing in the lens causes beam emittance growth and increases the minimum achievable spot size. To study the physics of the capillary discharge processes employed as active plasma lenses, we developed a 2-D hydrodynamic computational model. Here, we present preliminary simulation results and we compare the computed magnetic field profile with one from literature, which has been experimentally inferred. The result of the comparison is discussed. Active plasma lens Plasma lens Plasma hydrodynamics Hydrogen discharge Gas filled capillary Capillary discharge simulation Anania, M.P. verfasserin aut Atzeni, S. verfasserin aut Biagioni, A. verfasserin aut Chiadroni, E. verfasserin aut Croia, M. verfasserin aut Ferrario, M. verfasserin aut Filippi, F. verfasserin aut Marocchino, A. verfasserin aut Mostacci, A. verfasserin aut Pompili, R. verfasserin aut Romeo, S. verfasserin aut Schiavi, A. verfasserin aut Zigler, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 909, Seite 404-407 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:909 pages:404-407 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 909 404-407 |
| spelling |
10.1016/j.nima.2018.03.012 doi (DE-627)ELV001178342 (ELSEVIER)S0168-9002(18)30341-3 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Brentegani, E. verfasserin aut Numerical studies on capillary discharges as focusing elements for electron beams 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowing in the lens causes beam emittance growth and increases the minimum achievable spot size. To study the physics of the capillary discharge processes employed as active plasma lenses, we developed a 2-D hydrodynamic computational model. Here, we present preliminary simulation results and we compare the computed magnetic field profile with one from literature, which has been experimentally inferred. The result of the comparison is discussed. Active plasma lens Plasma lens Plasma hydrodynamics Hydrogen discharge Gas filled capillary Capillary discharge simulation Anania, M.P. verfasserin aut Atzeni, S. verfasserin aut Biagioni, A. verfasserin aut Chiadroni, E. verfasserin aut Croia, M. verfasserin aut Ferrario, M. verfasserin aut Filippi, F. verfasserin aut Marocchino, A. verfasserin aut Mostacci, A. verfasserin aut Pompili, R. verfasserin aut Romeo, S. verfasserin aut Schiavi, A. verfasserin aut Zigler, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 909, Seite 404-407 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:909 pages:404-407 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 909 404-407 |
| allfields_unstemmed |
10.1016/j.nima.2018.03.012 doi (DE-627)ELV001178342 (ELSEVIER)S0168-9002(18)30341-3 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Brentegani, E. verfasserin aut Numerical studies on capillary discharges as focusing elements for electron beams 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowing in the lens causes beam emittance growth and increases the minimum achievable spot size. To study the physics of the capillary discharge processes employed as active plasma lenses, we developed a 2-D hydrodynamic computational model. Here, we present preliminary simulation results and we compare the computed magnetic field profile with one from literature, which has been experimentally inferred. The result of the comparison is discussed. Active plasma lens Plasma lens Plasma hydrodynamics Hydrogen discharge Gas filled capillary Capillary discharge simulation Anania, M.P. verfasserin aut Atzeni, S. verfasserin aut Biagioni, A. verfasserin aut Chiadroni, E. verfasserin aut Croia, M. verfasserin aut Ferrario, M. verfasserin aut Filippi, F. verfasserin aut Marocchino, A. verfasserin aut Mostacci, A. verfasserin aut Pompili, R. verfasserin aut Romeo, S. verfasserin aut Schiavi, A. verfasserin aut Zigler, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 909, Seite 404-407 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:909 pages:404-407 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 909 404-407 |
| allfieldsGer |
10.1016/j.nima.2018.03.012 doi (DE-627)ELV001178342 (ELSEVIER)S0168-9002(18)30341-3 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Brentegani, E. verfasserin aut Numerical studies on capillary discharges as focusing elements for electron beams 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowing in the lens causes beam emittance growth and increases the minimum achievable spot size. To study the physics of the capillary discharge processes employed as active plasma lenses, we developed a 2-D hydrodynamic computational model. Here, we present preliminary simulation results and we compare the computed magnetic field profile with one from literature, which has been experimentally inferred. The result of the comparison is discussed. Active plasma lens Plasma lens Plasma hydrodynamics Hydrogen discharge Gas filled capillary Capillary discharge simulation Anania, M.P. verfasserin aut Atzeni, S. verfasserin aut Biagioni, A. verfasserin aut Chiadroni, E. verfasserin aut Croia, M. verfasserin aut Ferrario, M. verfasserin aut Filippi, F. verfasserin aut Marocchino, A. verfasserin aut Mostacci, A. verfasserin aut Pompili, R. verfasserin aut Romeo, S. verfasserin aut Schiavi, A. verfasserin aut Zigler, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 909, Seite 404-407 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:909 pages:404-407 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 909 404-407 |
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10.1016/j.nima.2018.03.012 doi (DE-627)ELV001178342 (ELSEVIER)S0168-9002(18)30341-3 DE-627 ger DE-627 rda eng 530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Brentegani, E. verfasserin aut Numerical studies on capillary discharges as focusing elements for electron beams 2018 nicht spezifiziert zzz rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowing in the lens causes beam emittance growth and increases the minimum achievable spot size. To study the physics of the capillary discharge processes employed as active plasma lenses, we developed a 2-D hydrodynamic computational model. Here, we present preliminary simulation results and we compare the computed magnetic field profile with one from literature, which has been experimentally inferred. The result of the comparison is discussed. Active plasma lens Plasma lens Plasma hydrodynamics Hydrogen discharge Gas filled capillary Capillary discharge simulation Anania, M.P. verfasserin aut Atzeni, S. verfasserin aut Biagioni, A. verfasserin aut Chiadroni, E. verfasserin aut Croia, M. verfasserin aut Ferrario, M. verfasserin aut Filippi, F. verfasserin aut Marocchino, A. verfasserin aut Mostacci, A. verfasserin aut Pompili, R. verfasserin aut Romeo, S. verfasserin aut Schiavi, A. verfasserin aut Zigler, A. verfasserin aut Enthalten in Nuclear instruments & methods in physics research / A Amsterdam : North-Holland Publ. Co., 1984 909, Seite 404-407 Online-Ressource (DE-627)266014666 (DE-600)1466532-3 (DE-576)074959743 0168-9002 nnns volume:909 pages:404-407 GBV_USEFLAG_U GBV_ELV SYSFLAG_U GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_224 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2027 GBV_ILN_2034 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2056 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2190 GBV_ILN_2336 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4242 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4313 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4393 33.05 Experimentalphysik VZ 33.07 Spektroskopie VZ 33.40 Kernphysik VZ AR 909 404-407 |
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English |
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Enthalten in Nuclear instruments & methods in physics research / A 909, Seite 404-407 volume:909 pages:404-407 |
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Enthalten in Nuclear instruments & methods in physics research / A 909, Seite 404-407 volume:909 pages:404-407 |
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Experimentalphysik Spektroskopie Kernphysik |
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Active plasma lens Plasma lens Plasma hydrodynamics Hydrogen discharge Gas filled capillary Capillary discharge simulation |
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Nuclear instruments & methods in physics research / A |
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Brentegani, E. @@aut@@ Anania, M.P. @@aut@@ Atzeni, S. @@aut@@ Biagioni, A. @@aut@@ Chiadroni, E. @@aut@@ Croia, M. @@aut@@ Ferrario, M. @@aut@@ Filippi, F. @@aut@@ Marocchino, A. @@aut@@ Mostacci, A. @@aut@@ Pompili, R. @@aut@@ Romeo, S. @@aut@@ Schiavi, A. @@aut@@ Zigler, A. @@aut@@ |
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2018-01-01T00:00:00Z |
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Brentegani, E. ddc 530 bkl 33.05 bkl 33.07 bkl 33.40 misc Active plasma lens misc Plasma lens misc Plasma hydrodynamics misc Hydrogen discharge misc Gas filled capillary misc Capillary discharge simulation Numerical studies on capillary discharges as focusing elements for electron beams |
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530 VZ 33.05 bkl 33.07 bkl 33.40 bkl Numerical studies on capillary discharges as focusing elements for electron beams Active plasma lens Plasma lens Plasma hydrodynamics Hydrogen discharge Gas filled capillary Capillary discharge simulation |
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Brentegani, E. Anania, M.P. Atzeni, S. Biagioni, A. Chiadroni, E. Croia, M. Ferrario, M. Filippi, F. Marocchino, A. Mostacci, A. Pompili, R. Romeo, S. Schiavi, A. Zigler, A. |
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Numerical studies on capillary discharges as focusing elements for electron beams |
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Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowing in the lens causes beam emittance growth and increases the minimum achievable spot size. To study the physics of the capillary discharge processes employed as active plasma lenses, we developed a 2-D hydrodynamic computational model. Here, we present preliminary simulation results and we compare the computed magnetic field profile with one from literature, which has been experimentally inferred. The result of the comparison is discussed. |
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Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowing in the lens causes beam emittance growth and increases the minimum achievable spot size. To study the physics of the capillary discharge processes employed as active plasma lenses, we developed a 2-D hydrodynamic computational model. Here, we present preliminary simulation results and we compare the computed magnetic field profile with one from literature, which has been experimentally inferred. The result of the comparison is discussed. |
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Active plasma lenses are promising technologies for the focusing of high brightness electron beams due to their radially symmetric focusing and their high field gradients (up to several kT/m). However, in a number of experimental situations, the transverse non-uniformity of the current density flowing in the lens causes beam emittance growth and increases the minimum achievable spot size. To study the physics of the capillary discharge processes employed as active plasma lenses, we developed a 2-D hydrodynamic computational model. Here, we present preliminary simulation results and we compare the computed magnetic field profile with one from literature, which has been experimentally inferred. The result of the comparison is discussed. |
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| score |
7.3991594 |