The pseudorapidity density and multiplicity distribution of charged particles produced in proton-proton collisions at the LHC, at a centre-of-mass energy root s = 7 TeV, were measured in the central pseudorapidity region vertical bar eta vertical bar < 1. Comparisons are made with previous measurements at root s = 0.9 TeV and 2.36 TeV. At root s = 7 TeV, for events with at least one charged particle in |eta vertical bar| < 1, we obtain dN(ch)/d eta = 6.01 +/- 0.01(stat.)(-0.12)(+0.20) (syst.). This corresponds to an increase of 57.6%+/-0.4%(stat.)(-1.8%)(+3.6) (syst.) relative to collisions at 0.9 TeV, significantly higher than calculations from commonly used models. The multiplicity distribution at 7 TeV is described fairly well by the negative binomial distribution.
Charged-particle multiplicity measurement in proton-proton collisions at root s=7 TeV with ALICE at LHC / Aamodt, K; Abel, N; Abeysekara, U; ABRAHANTES QUINTANA, A; Abramyan, A; Adamova, D; Aggarwal, M; AGLIERI RINELLA, G; Agocs, A; AGUILAR SALAZAR, S; Ahammed, Z; Ahmad, A; Ahmad, N; Ahn, S; Akimoto, R; Akindinov, A; Aleksandrov, D; Alessandro, B; ALFARO MOLINA, R; Alici, A; ALMARAZ AVIA, E; Alme, J; 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, H; Arcelli, S; Arceo, R; Arend, A; Armesto, N; Arnaldi, R; Aronsson, T; Arsene, I; Asryan, A; Augustinus, A; Averbeck, R; Awes, T; Aysto, J; Azmi, M; Bablok, S; Bach, M; Badalia, A; Baek, Y; Bagnasco, S; Bailhache, R; Bala, R; Baldisseri, A; Baldit, A; Ban, J; Barbera, R; Barnafoldi, G; Barnby, L; Barret, V; Bartke, J; Barile, F; Basile, M; Basmanov, V; Bastid, N; Bathen, B; Batigne, G; 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C, PARTICLES AND FIELDS. - ISSN 1434-6044. - STAMPA. - 68:3(2010), pp. 345-354. [10.1140/epjc/s10052-010-1350-2]
Charged-particle multiplicity measurement in proton-proton collisions at root s=7 TeV with ALICE at LHC
AAMODT K; ABEL N; ABEYSEKARA U; ABRAHANTES QUINTANA A; ABRAMYAN A; ADAMOVA D; AGGARWAL M; AGLIERI RINELLA G; AGOCS A; AGUILAR SALAZAR S; AHAMMED Z; AHMAD A; AHMAD N; AHN S; AKIMOTO R; AKINDINOV A; ALEKSANDROV D; ALESSANDRO B; ALFARO MOLINA R; ALICI A; ALMARAZ AVIA E; ALME J; 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 H; ARCELLI S; ARCEO R; AREND A; ARMESTO N; ARNALDI R; ARONSSON T; ARSENE I; ASRYAN A; AUGUSTINUS A; AVERBECK R; AWES T; AYSTO J; AZMI M; BABLOK S; BACH M; BADALIA A; BAEK Y; BAGNASCO S; BAILHACHE R; BALA R; BALDISSERI A; BALDIT A; BAN J; BARBERA R; BARNAFOLDI G; BARNBY L; BARRET V; BARTKE J; BARILE F; BASILE M; BASMANOV V; BASTID N; BATHEN B; BATIGNE G; BATYUNYA B; BAUMANN C; BEARDEN I; 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 A; BIANCHI L; BIANCHI N; BIANCHIN C; BIELIK J; BIELIKOVA J; BILANDZIC A; BIMBOT L; BIOLCATI E; BLANC A; BLANCO F; BLANCO F; BLAU D; BLUME C; BOCCIOLI M; BOCK N; BOGDANOV A; BOGGILD H; BOGOLYUBSKY M; BOHM J; BOLDIZSAR L; BOMBARA M; BOMBONATI C; BONDILA M; BOREL H; BORISOV A; BORTOLIN C; BOSE S; BOSISIO L; BOSSU F; BOTJE M; BOTTGER S; BOURDAUD G; BOYER B; BRAUN M; BRAUN MUNZINGER P; BRAVINA L; BREGANT M; BREITNER T; BRUCKNER G; BRUN R; BRUNA E; BRUNO G; BUDNIKOV D; BUESCHING H; BUNCIC P; BUSCH O; BUTHELEZI Z; CAFFARRI D; CAI X; CAINES H; CAMACHO E; CAMERINI P; CAMPBELL M; CANOA ROMAN V; CAPITANI G; CARA ROMEO G; CARENA F; CARENA W; CARMINATI F; DIAZ AC; CASELLE M; CASTELLANOS JC; CASTILLO HERNANDEZ J; CATANESCU V; CATTARUZZA E; CAVICCHIOLI C; CERELLO P; CHAMBERT V; CHANG B; CHAPELAND S; CHARPY A; CHARVET J; CHATTOPADHYAY S; CHATTOPADHYAY S; CHERNEY M; CHESHKOV C; CHEYNIS B; CHIAVASSA E; BARROSO VC; CHINELLATO D; CHOCHULA P; CHOI K; CHOJNACKI M; CHRISTAKOGLOU P; CHRISTENSEN C; CHRISTIANSEN P; CHUJO T; CHUMAN F; CICALO C; CIFARELLI L; CINDOLO F; CLEYMANS J; COBANOGLU O; COFFIN JP; COLI S; COLLA A; CONESA BALBASTRE G; DEL VALLE ZC; CONNER E; CONSTANTIN P; CONTIN G; CONTRERAS J; MORALES YC; CORMIER T; CORTESE P; MALDONADO IC; COSENTINO M; COSTA F; COTALLO M; CRESCIO E; CROCHET P; CUAUTLE E; CUNQUEIRO L ;CUSSONNEAU J; DAINESE A; DALSGAARD H; DANU A; DAS I; DASH A; DASH S; BARROS G; CARO A; DE CATALDO G; DE CUVELAND J; FALCO A; GASPARI M; DE GROOT J; GRUTTOLA D; MARCO N; PASQUALE S; REMIGIS R; DE ROOIJ R; DE VAUX G; DELAGRANGE H; DELLACASA G; DELOFF A; DEMANOV V; DENES E; DEPPMAN A; D'ERASMO G; DERKACH D; DEVAUX A; DI BARI D; DI GIGLIO C; DI LIBERTO S; DI MAURO A; DI NEZZA P; DIALINAS M; DIAZ L; DIAZ R; DIETEL T; DIVI R; DJUVSLAND O; DOBRETSOV V; DOBRIN A; DOBROWOLSKI T; DONIGUS B; DOMINGUEZ I; DON D; DORDIC O; DUBEY A; DUBUISSON J; DUCROUX L; DUPIEUX P; DUTTA MAJUMDAR A; DUTTA MAJUMDAR M; ELIA D; EMSCHERMANN D; ENOKIZONO A; ESPAGNON B; ESTIENNE M; ESUMI S; EVANS D; 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2010
Abstract
The pseudorapidity density and multiplicity distribution of charged particles produced in proton-proton collisions at the LHC, at a centre-of-mass energy root s = 7 TeV, were measured in the central pseudorapidity region vertical bar eta vertical bar < 1. Comparisons are made with previous measurements at root s = 0.9 TeV and 2.36 TeV. At root s = 7 TeV, for events with at least one charged particle in |eta vertical bar| < 1, we obtain dN(ch)/d eta = 6.01 +/- 0.01(stat.)(-0.12)(+0.20) (syst.). This corresponds to an increase of 57.6%+/-0.4%(stat.)(-1.8%)(+3.6) (syst.) relative to collisions at 0.9 TeV, significantly higher than calculations from commonly used models. The multiplicity distribution at 7 TeV is described fairly well by the negative binomial distribution.
Citazione
Charged-particle multiplicity measurement in proton-proton collisions at root s=7 TeV with ALICE at LHC / Aamodt, K; Abel, N; Abeysekara, U; ABRAHANTES QUINTANA, A; Abramyan, A; Adamova, D; Aggarwal, M; AGLIERI RINELLA, G; Agocs, A; AGUILAR SALAZAR, S; Ahammed, Z; Ahmad, A; Ahmad, N; Ahn, S; Akimoto, R; Akindinov, A; Aleksandrov, D; Alessandro, B; ALFARO MOLINA, R; Alici, A; ALMARAZ AVIA, E; Alme, J; 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, H; Arcelli, S; Arceo, R; Arend, A; Armesto, N; Arnaldi, R; Aronsson, T; Arsene, I; Asryan, A; Augustinus, A; Averbeck, R; Awes, T; Aysto, J; Azmi, M; Bablok, S; Bach, M; Badalia, A; Baek, Y; Bagnasco, S; Bailhache, R; Bala, R; Baldisseri, A; Baldit, A; Ban, J; Barbera, R; Barnafoldi, G; Barnby, L; Barret, V; Bartke, J; Barile, F; Basile, M; Basmanov, V; Bastid, N; Bathen, B; Batigne, G; 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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione.
