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
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Englisch |
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1997 |
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8 |
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Springer Online Journal Archives 1860-2002 |
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Übergeordnetes Werk: |
in: Hyperfine interactions - 1975, 109(1997) vom: Jan./Apr., Seite 323-330 |
Übergeordnetes Werk: |
volume:109 ; year:1997 ; month:01/04 ; pages:323-330 ; extent:8 |
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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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(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier 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. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
spelling |
(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier 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. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
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(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier 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. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
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(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier 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. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
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(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier 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. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
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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. |
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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. |
abstract_unstemmed |
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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