Antiprotons for plasma heating
Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiproto...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Huber, Felix M. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1997 |
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| Schlagwörter: |
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| Anmerkung: |
© Kluwer Academic Publishers 1997 |
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| Übergeordnetes Werk: |
Enthalten in: Hyperfine interactions - Kluwer Academic Publishers, 1975, 109(1997), 1-4 vom: Aug., Seite 323-330 |
|---|---|
| Übergeordnetes Werk: |
volume:109 ; year:1997 ; number:1-4 ; month:08 ; pages:323-330 |
| Links: |
|---|
| DOI / URN: |
10.1023/A:1012630106392 |
|---|
| Katalog-ID: |
OLC2076388990 |
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| 520 | |a Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. | ||
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10.1023/A:1012630106392 doi (DE-627)OLC2076388990 (DE-He213)A:1012630106392-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Huber, Felix M. verfasserin aut Antiprotons for plasma heating 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Energy Deposit Density Change Reaction Chamber Antihydrogen Plasma Heating Messerschmid, Ernst W. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 109(1997), 1-4 vom: Aug., Seite 323-330 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:109 year:1997 number:1-4 month:08 pages:323-330 https://doi.org/10.1023/A:1012630106392 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 109 1997 1-4 08 323-330 |
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10.1023/A:1012630106392 doi (DE-627)OLC2076388990 (DE-He213)A:1012630106392-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Huber, Felix M. verfasserin aut Antiprotons for plasma heating 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Energy Deposit Density Change Reaction Chamber Antihydrogen Plasma Heating Messerschmid, Ernst W. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 109(1997), 1-4 vom: Aug., Seite 323-330 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:109 year:1997 number:1-4 month:08 pages:323-330 https://doi.org/10.1023/A:1012630106392 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 109 1997 1-4 08 323-330 |
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10.1023/A:1012630106392 doi (DE-627)OLC2076388990 (DE-He213)A:1012630106392-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Huber, Felix M. verfasserin aut Antiprotons for plasma heating 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Energy Deposit Density Change Reaction Chamber Antihydrogen Plasma Heating Messerschmid, Ernst W. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 109(1997), 1-4 vom: Aug., Seite 323-330 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:109 year:1997 number:1-4 month:08 pages:323-330 https://doi.org/10.1023/A:1012630106392 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 109 1997 1-4 08 323-330 |
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10.1023/A:1012630106392 doi (DE-627)OLC2076388990 (DE-He213)A:1012630106392-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Huber, Felix M. verfasserin aut Antiprotons for plasma heating 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Energy Deposit Density Change Reaction Chamber Antihydrogen Plasma Heating Messerschmid, Ernst W. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 109(1997), 1-4 vom: Aug., Seite 323-330 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:109 year:1997 number:1-4 month:08 pages:323-330 https://doi.org/10.1023/A:1012630106392 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 109 1997 1-4 08 323-330 |
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10.1023/A:1012630106392 doi (DE-627)OLC2076388990 (DE-He213)A:1012630106392-p DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Huber, Felix M. verfasserin aut Antiprotons for plasma heating 1997 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Kluwer Academic Publishers 1997 Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Energy Deposit Density Change Reaction Chamber Antihydrogen Plasma Heating Messerschmid, Ernst W. aut Enthalten in Hyperfine interactions Kluwer Academic Publishers, 1975 109(1997), 1-4 vom: Aug., Seite 323-330 (DE-627)129438685 (DE-600)194471-X (DE-576)014809028 0304-3843 nnns volume:109 year:1997 number:1-4 month:08 pages:323-330 https://doi.org/10.1023/A:1012630106392 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_20 GBV_ILN_22 GBV_ILN_40 GBV_ILN_70 GBV_ILN_2279 GBV_ILN_4307 33.00 VZ AR 109 1997 1-4 08 323-330 |
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Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. © Kluwer Academic Publishers 1997 |
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Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. © Kluwer Academic Publishers 1997 |
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Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. © Kluwer Academic Publishers 1997 |
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