3 research outputs found
Ion stopping in dense plasma target for high energy density physics
- Author
- Bimbot René
- Chabot Marin
- Couillaud Christophe
- Della-Negra Serge
- Deutsch Claude
- Fertman Alexander
- Fleurier Claude
- Fortov Vladimir E.
- Gardes Daniel
- Golubev Alexey A.
- Hasegawa Jun
- Hoffmann Dieter H. H.
- Jacoby Joachim
- Maynard Gilles
- Mintsev Victor
- Ogawa Masao
- Oguri Yoshiyuki
- Rivet Marie-France
- Rosmej Olga N.
- Sharkov Boris Y.
- Tahir Naeem Ahmad
- Wahl H.
- Weyrich Karin
- Publication venue
- Publication date
- 01/01/2010
- Field of study
The basic physics of nonrelativistic and electromagnetic ion stopping in hot and ionized plasma targets is thoroughly updated. Corresponding projectile-target interactions involve enhanced projectile ionization and coupling with target free electrons leading to significantly larger energy losses in hot targets when contrasted to their cold homologues. Standard stoppping formalism is framed around the most economical extrapolation of high velocity stopping in cold matter. Further elaborations pay attention to target electron coupling and nonlinearities due to enhanced projectile charge state, as well. Scaling rules are then used to optimize the enhanced stopping of MeV/amu ions in plasmas with electron linear densities nel ~ 10 18 -10 20 cm -2 . The synchronous firing of dense and strongly ionized plasmas with the time structure of bunched and energetic multicharged ion beam then allow to probe, for the first time, the long searched enhanced plasma stopping and projectile charge at target exit. Laser ablated plasmas (SPQR1) and dense linear plasma columns (SPQR2) show up as targets of choice in providing accurate and on line measurements of plasma parameters. Corresponding stopping results are of a central significance in asserting the validity of intense ion beam scenarios for driving thermonuclear pellets. Other applications of note feature thorium induced fission, novel ion sources and specific material processing through low energy ion beams. Last but not least, the given ion beam-plasma target interaction physics is likely to pave a way to the production and diagnostics of warm dense matter (WDM)
Midrapidity antiproton-to-proton ratio in pp collisons root s=0.9 and 7 TeV measured by the ALICE experiment
- Author
- Aamodt Kenneth
- Abel N
- Abeysekara U
- Abramyan A
- Adamová D
- Aggarwal MM
- Agocs AG
- Ahammed Z
- Ahmad A
- Ahmad N
- Ahn SU
- Akimoto R
- Akindinov A
- Aleksandrov D
- Alessandro B
- Alici A
- Alme Johan
- Alt T.
- Altini V
- Altinpinar S
- Andrei C
- Andronic A
- Anelli G
- Angelov V
- Anson C
- Anticic T
- Antinori F
- Antinori S
- Antipin K
- Antonczyk D
- Antonioli P
- Anzo A
- Aphecetche L
- Appelshauser SA
- Arcelli S
- Arceo R
- Arend A
- Armesto N
- Arnaldi R
- Aronsson T
- Arsene Ionut Christian
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
- Bablok Sebastian Robert
- Bach M
- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisser A
- Baldit A
- Ban J
- Barbera R
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VC
- Bartke J
- Basile M
- Basmanov V
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann C
- Bearden IG
- Becker B
- Belikov I
- Bellwied R
- Belmont-Moreno E
- Belogianni A
- Benhabib L
- Beole S
- Berceanu I
- Bercuci A
- Berdermann E
- Berdnikov Y
- Betev L
- Bhasin A
- Bhati AK
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- Bielcikova J
- Bilandzic A
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- Biolcati E
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- Boggild H
- Bogolyubsky M
- Bohm J
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- Borel H
- Borisov A
- Bortolin C
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- Bossu F
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- Bottger S
- Bourdaud G
- Boyer B
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- Braun-Munzinger P
- Bravina Larissa
- Bregant M
- Breitner T
- Bruckner G
- Brun R
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Buncic P
- Busch O
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- Capitani GP
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- Cherney M
- Cheshkov C
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- Chiavassa E
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- Chinellato DD
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- Hasegan D
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- Hutter D
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- Ilkiv I
- Inaba M
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- Ippolitov M
- Irfan M
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- Tsilis E
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- Tveter Trine Spedstad
- Tydesjo H
- Tywoniuk Konrad
- Ulery J
- Ullaland Kjetil
- Uras A
- Urban J
- Urciuoli GM
- Usai GL
- Vacchi A
- Vala M
- Vallero S
- van der Kolk N
- van Leeuwen M
- Vannucci L
- Vargas A
- Vargas HL
- Varma R
- Vasileiou M
- Vasiliev A
- Vasquez MAS
- Vassiliev I
- Vechernin V
- Velasquez AO
- Venaruzzo M
- Vercellin E
- Vergara S
- Vernet R
- Verweij M
- Vetlitskiy I
- Vickovic L
- Viesti G
- Vikhlyantsev O
- Vilakazi Z
- Vinogradov A
- Vyvre PV
- Wagner Boris
- Wikne Jon Christopher
- Zabrodin Evgeny
- Zetina LM
- Øvrebekk Gaute
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 09/10/2017
- Field of study
The ratio of the yields of antiprotons to protons in pp collisions has been measured by the ALICE experiment at root s = 0.9 and 7 TeV during the initial running periods of the Large Hadron Collider. The measurement covers the transverse momentum interval 0.45 < p(t) < 1.05 GeV/c and rapidity vertical bar y vertical bar < 0.5. The ratio is measured to be R-vertical bar y vertical bar<0.5 = 0.957 +/- 0.006(stat) +/- 0.0014(syst) at 0.9 Tev and R-vertical bar y vertical bar<0.5 = 0.991 +/- 0.005 +/- 0.014(syst) at 7 TeV and it is independent of both rapidity and transverse momentum. The results are consistent with the conventional model of baryon-number transport and set stringent limits on any additional contributions to baryon-number transfer over very large rapidity intervals in pp collisions
Transverse momentum spectra of charged particles in proton–proton collisions at √s=900 GeV with ALICE at the LHC
- Author
- Aamodt Kenneth
- Abel N.
- Abeysekara U.
- Abrahantes Quintana A.
- Abramyan A.
- Adamová Dagmar
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agocs A.G.
- Aguilar Salazar S.
- Ahammed Zubayer
- Ahmad A.
- Ahmad Nazeer
- Ahn Sang Un
- Akimoto R.
- Akindinov Alexander
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfaro Molina Jose Ruben
- Alici Andrea
- Almaráz Aviña E.
- Alme Johan
- Alt Torsten
- Altini V.
- Altinpinar Sedat
- Andrei Cristian
- Andronic Anton
- Anelli G.
- Angelov V.
- Anson Christopher Daniel
- Antinori Federico
- Antinori S.
- Antipin K.
- Antičić Tome
- Antonioli Pietro
- Antończyk Dariusz
- Anzo A.
- Aphecetche Laurent Bernard
- Appelshäuser Harald
- Arcelli Silvia
- Arceo R.
- Arend A.
- Armesto Néstor
- Arnaldi Roberta
- Aronsson Tomas Robert
- Arsene Ionut Cristian
- Asryan A.
- Augustinus Andre
- Averbeck Ralf Peter
- Awes T.C.
- Azmi Mohd Danish
- Bablok Sebastian
- Bach Matthias
- Badalà Angela
- Baek Yong Wook
- Bagnasco Stefano
- Bailhache Raphaëlle
- Bala Remu
- Baldisseri Alberto
- Baldit A.
- Barbera Roberto
- Barile Francesco
- Barnaföldi Gergely Gábor
- Barnby L.
- Barret Valerie
- Bartke Jerzy
- Basile Maurizio
- Basmanov V.
- Bastid Nicole
- Bathen Bastian
- Batigne Guillaume
- Batyunya Boris
- Baumann C.
- Bearden Ian Gardner
- Becker B.
- Belikov Iouri
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- Zycháček V.
- Zynovyev M.
- Závada Petr
- Äystö J.
- Österman L.
- Øvrebekk G.
- Šafařík Karel
- Šumbera Michal
- Šuša Tatjana
- Šándor Ladislav
- Publication venue
- Publication date
- 20/08/2010
- Field of study
The inclusive charged particle transverse momentum distribution is measured in proton–proton collisions at s=900 GeV at the LHC using the ALICE detector. The measurement is performed in the central pseudorapidity region (|η|<0.8) over the transverse momentum range 0.15<pT<10 GeV/c. The correlation between transverse momentum and particle multiplicity is also studied. Results are presented for inelastic (INEL) and non-single-diffractive (NSD) events. The average transverse momentum for |η|<0.8 is 〈pT〉INEL=0.483±0.001 (stat.)±0.007 (syst.) GeV/c and 〈pT〉NSD=0.489±0.001 (stat.)±0.007 (syst.) GeV/c, respectively. The data exhibit a slightly larger 〈pT〉 than measurements in wider pseudorapidity intervals. The results are compared to simulations with the Monte Carlo event generators PYTHIA and PHOJET