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Positronium for Antihydrogen Production in the AEGIS Experiment
The primary goal of the Antihydrogen Experiment: Gravity, Interferometry, Spectroscopy (AEGIS) collaboration is to measure for the first time precisely the gravitational acceleration of antihydrogen, H¯ , a fundamental issue of contemporary physics, using a beam of antiatoms. Indeed, although indire...
Autores principales: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2017
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.12693/APhysPolA.132.1443 http://cds.cern.ch/record/2312278 |
_version_ | 1780958009343606784 |
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author | Consolati, G Aghion, S Amsler, C Bonomi, G Brusa, R S Caccia, M Caravita, R Castelli, F Cerchiari, G Comparat, D Demetrio, A Di Noto, L Doser, M Evans, C Fanì, M Ferragut, R Fesel, J Fontana, A Gerber, S Giammarchi, M Gligorova, A Guatieri, F Haider, S Hinterberger, A Holmestad, H Kellerbauer, A Khalidova, O Krasnicky, D Lagomarsino, V Lansonneur, P Lebrun, P Malbrunot, C Mariazzi, S Marton, J Matveev, V Mazzotta, Z Müller, S R Nebbia, G Nedelec, P Oberthaler, M Pacifico, N Pagano, D Penasa, L Petracek, V Prelz, F Prevedelli, M Ravelli, L Rienaecker, B Robert, J Røhne, O M Rotondi, A Sandaker, H Santoro, R Smestad, L Sorrentino, F Testera, G Tietje, I C Widmann, E Yzombard, P Zimmer, C Zmeskal, J Zurlo, N |
author_facet | Consolati, G Aghion, S Amsler, C Bonomi, G Brusa, R S Caccia, M Caravita, R Castelli, F Cerchiari, G Comparat, D Demetrio, A Di Noto, L Doser, M Evans, C Fanì, M Ferragut, R Fesel, J Fontana, A Gerber, S Giammarchi, M Gligorova, A Guatieri, F Haider, S Hinterberger, A Holmestad, H Kellerbauer, A Khalidova, O Krasnicky, D Lagomarsino, V Lansonneur, P Lebrun, P Malbrunot, C Mariazzi, S Marton, J Matveev, V Mazzotta, Z Müller, S R Nebbia, G Nedelec, P Oberthaler, M Pacifico, N Pagano, D Penasa, L Petracek, V Prelz, F Prevedelli, M Ravelli, L Rienaecker, B Robert, J Røhne, O M Rotondi, A Sandaker, H Santoro, R Smestad, L Sorrentino, F Testera, G Tietje, I C Widmann, E Yzombard, P Zimmer, C Zmeskal, J Zurlo, N |
author_sort | Consolati, G |
collection | CERN |
description | The primary goal of the Antihydrogen Experiment: Gravity, Interferometry, Spectroscopy (AEGIS) collaboration is to measure for the first time precisely the gravitational acceleration of antihydrogen, H¯ , a fundamental issue of contemporary physics, using a beam of antiatoms. Indeed, although indirect arguments have been raised against a different acceleration of antimatter with respect to matter, nevertheless some attempts to formulate quantum theories of gravity, or to unify gravity with the other forces, consider the possibility of a non-identical gravitational interaction between matter and antimatter. We plan to generate H¯ through a charge-exchange reaction between excited Ps and antiprotons coming from the Antiproton Decelerator facility at CERN. It offers the advantage to produce sufficiently cold antihydrogen to make feasible a measurement of gravitational acceleration with reasonable uncertainty (of the order of a few percent). Since the cross-section of the above reaction increases with n 4 , n being the principal quantum number of Ps, it is essential to generate Ps in a highly excited (Rydberg) state. This will occur by means of two laser excitations of Ps emitted from a nanoporous silica target: a first UV laser (at 205 nm) will bring Ps from the ground to the n = 3 state; a second laser pulse (tunable in the range 1650–1700 nm) will further excite Ps to the Rydberg state. |
id | oai-inspirehep.net-1643356 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2017 |
record_format | invenio |
spelling | oai-inspirehep.net-16433562019-09-30T06:29:59Zdoi:10.12693/APhysPolA.132.1443http://cds.cern.ch/record/2312278engConsolati, GAghion, SAmsler, CBonomi, GBrusa, R SCaccia, MCaravita, RCastelli, FCerchiari, GComparat, DDemetrio, ADi Noto, LDoser, MEvans, CFanì, MFerragut, RFesel, JFontana, AGerber, SGiammarchi, MGligorova, AGuatieri, FHaider, SHinterberger, AHolmestad, HKellerbauer, AKhalidova, OKrasnicky, DLagomarsino, VLansonneur, PLebrun, PMalbrunot, CMariazzi, SMarton, JMatveev, VMazzotta, ZMüller, S RNebbia, GNedelec, POberthaler, MPacifico, NPagano, DPenasa, LPetracek, VPrelz, FPrevedelli, MRavelli, LRienaecker, BRobert, JRøhne, O MRotondi, ASandaker, HSantoro, RSmestad, LSorrentino, FTestera, GTietje, I CWidmann, EYzombard, PZimmer, CZmeskal, JZurlo, NPositronium for Antihydrogen Production in the AEGIS ExperimentParticle Physics - ExperimentThe primary goal of the Antihydrogen Experiment: Gravity, Interferometry, Spectroscopy (AEGIS) collaboration is to measure for the first time precisely the gravitational acceleration of antihydrogen, H¯ , a fundamental issue of contemporary physics, using a beam of antiatoms. Indeed, although indirect arguments have been raised against a different acceleration of antimatter with respect to matter, nevertheless some attempts to formulate quantum theories of gravity, or to unify gravity with the other forces, consider the possibility of a non-identical gravitational interaction between matter and antimatter. We plan to generate H¯ through a charge-exchange reaction between excited Ps and antiprotons coming from the Antiproton Decelerator facility at CERN. It offers the advantage to produce sufficiently cold antihydrogen to make feasible a measurement of gravitational acceleration with reasonable uncertainty (of the order of a few percent). Since the cross-section of the above reaction increases with n 4 , n being the principal quantum number of Ps, it is essential to generate Ps in a highly excited (Rydberg) state. This will occur by means of two laser excitations of Ps emitted from a nanoporous silica target: a first UV laser (at 205 nm) will bring Ps from the ground to the n = 3 state; a second laser pulse (tunable in the range 1650–1700 nm) will further excite Ps to the Rydberg state.oai:inspirehep.net:16433562017 |
spellingShingle | Particle Physics - Experiment Consolati, G Aghion, S Amsler, C Bonomi, G Brusa, R S Caccia, M Caravita, R Castelli, F Cerchiari, G Comparat, D Demetrio, A Di Noto, L Doser, M Evans, C Fanì, M Ferragut, R Fesel, J Fontana, A Gerber, S Giammarchi, M Gligorova, A Guatieri, F Haider, S Hinterberger, A Holmestad, H Kellerbauer, A Khalidova, O Krasnicky, D Lagomarsino, V Lansonneur, P Lebrun, P Malbrunot, C Mariazzi, S Marton, J Matveev, V Mazzotta, Z Müller, S R Nebbia, G Nedelec, P Oberthaler, M Pacifico, N Pagano, D Penasa, L Petracek, V Prelz, F Prevedelli, M Ravelli, L Rienaecker, B Robert, J Røhne, O M Rotondi, A Sandaker, H Santoro, R Smestad, L Sorrentino, F Testera, G Tietje, I C Widmann, E Yzombard, P Zimmer, C Zmeskal, J Zurlo, N Positronium for Antihydrogen Production in the AEGIS Experiment |
title | Positronium for Antihydrogen Production in the AEGIS Experiment |
title_full | Positronium for Antihydrogen Production in the AEGIS Experiment |
title_fullStr | Positronium for Antihydrogen Production in the AEGIS Experiment |
title_full_unstemmed | Positronium for Antihydrogen Production in the AEGIS Experiment |
title_short | Positronium for Antihydrogen Production in the AEGIS Experiment |
title_sort | positronium for antihydrogen production in the aegis experiment |
topic | Particle Physics - Experiment |
url | https://dx.doi.org/10.12693/APhysPolA.132.1443 http://cds.cern.ch/record/2312278 |
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