使用ATLAS探测器，在质心能量√s = 8 TeV的质子-质子碰撞中，测量产生[公式：见原文]且伴有一个或两个额外喷注的基准截面。
Measurements of fiducial cross-sections for [Formula: see text] production with one or two additional -jets in collisions at [Formula: see text]=8 TeV using the ATLAS detector.
作者信息
Aad G, Abbott B, Abdallah J, Abdinov O, Aben R, Abolins M, AbouZeid O S, Abramowicz H, Abreu H, Abreu R, Abulaiti Y, Acharya B S, Adamczyk L, Adams D L, Adelman J, Adomeit S, Adye T, Affolder A A, Agatonovic-Jovin T, Agricola J, Aguilar-Saavedra J A, Ahlen S P, Ahmadov F, Aielli G, Akerstedt H, Åkesson T P A, Akimov A V, Alberghi G L, Albert J, Albrand S, Alconada Verzini M J, Aleksa M, Aleksandrov I N, Alexa C, Alexander G, Alexopoulos T, Alhroob M, Alimonti G, Alio L, Alison J, Alkire S P, Allbrooke B M M, Allport P P, Aloisio A, Alonso A, Alonso F, Alpigiani C, Altheimer A, Alvarez Gonzalez B, Álvarez Piqueras D, Alviggi M G, Amadio B T, Amako K, Amaral Coutinho Y, Amelung C, Amidei D, Amor Dos Santos S P, Amorim A, Amoroso S, Amram N, Amundsen G, Anastopoulos C, Ancu L S, Andari N, Andeen T, Anders C F, Anders G, Anders J K, Anderson K J, Andreazza A, Andrei V, Angelidakis S, Angelozzi I, Anger P, Angerami A, Anghinolfi F, Anisenkov A V, Anjos N, Annovi A, Antonelli M, Antonov A, Antos J, Anulli F, Aoki M, Aperio Bella L, Arabidze G, Arai Y, Araque J P, Arce A T H, Arduh F A, Arguin J-F, Argyropoulos S, Arik M, Armbruster A J, Arnaez O, Arnold H, Arratia M, Arslan O, Artamonov A, Artoni G, Asai S, Asbah N, Ashkenazi A, Åsman B, Asquith L, Assamagan K, Astalos R, Atkinson M, Atlay N B, Augsten K, Aurousseau M, Avolio G, Axen B, Ayoub M K, Azuelos G, Baak M A, Baas A E, Baca M J, Bacci C, Bachacou H, Bachas K, Backes M, Backhaus M, Bagiacchi P, Bagnaia P, Bai Y, Bain T, Baines J T, Baker O K, Baldin E M, Balek P, Balestri T, Balli F, Balunas W K, Banas E, Banerjee Sw, Bannoura A A E, Barak L, Barberio E L, Barberis D, Barbero M, Barillari T, Barisonzi M, Barklow T, Barlow N, Barnes S L, Barnett B M, Barnett R M, Barnovska Z, Baroncelli A, Barone G, Barr A J, Barreiro F, Barreiro Guimarães da Costa J, Bartoldus R, Barton A E, Bartos P, Basalaev A, Bassalat A, Basye A, Bates R L, Batista S J, Batley J R, Battaglia M, Bauce M, Bauer F, Bawa H S, Beacham J B, Beattie M D, Beau T, Beauchemin P H, Beccherle R, Bechtle P, Beck H P, Becker K, Becker M, Beckingham M, Becot C, Beddall A J, Beddall A, Bednyakov V A, Bee C P, Beemster L J, Beermann T A, Begel M, Behr J K, Belanger-Champagne C, Bell W H, Bella G, Bellagamba L, Bellerive A, Bellomo M, Belotskiy K, Beltramello O, Benary O, Benchekroun D, Bender M, Bendtz K, Benekos N, Benhammou Y, Benhar Noccioli E, Benitez Garcia J A, Benjamin D P, Bensinger J R, Bentvelsen S, Beresford L, Beretta M, Berge D, Bergeaas Kuutmann E, Berger N, Berghaus F, Beringer J, Bernard C, Bernard N R, Bernius C, Bernlochner F U, Berry T, Berta P, Bertella C, Bertoli G, Bertolucci F, Bertsche C, Bertsche D, Besana M I, Besjes G J, Bessidskaia Bylund O, Bessner M, Besson N, Betancourt C, Bethke S, Bevan A J, Bhimji W, Bianchi R M, Bianchini L, Bianco M, Biebel O, Biedermann D, Bieniek S P, Biglietti M, Bilbao De Mendizabal J, Bilokon H, Bindi M, Binet S, Bingul A, Bini C, Biondi S, Bjergaard D M, Black C W, Black J E, Black K M, Blackburn D, Blair R E, Blanchard J-B, Blanco J E, Blazek T, Bloch I, Blocker C, Blum W, Blumenschein U, Blunier S, Bobbink G J, Bobrovnikov V S, Bocchetta S S, Bocci A, Bock C, Boehler M, Bogaerts J A, Bogavac D, Bogdanchikov A G, Bohm C, Boisvert V, Bold T, Boldea V, Boldyrev A S, Bomben M, Bona M, Boonekamp M, Borisov A, Borissov G, Borroni S, Bortfeldt J, Bortolotto V, Bos K, Boscherini D, Bosman M, Boudreau J, Bouffard J, Bouhova-Thacker E V, Boumediene D, Bourdarios C, Bousson N, Boutle S K, Boveia A, Boyd J, Boyko I R, Bozic I, Bracinik J, Brandt A, Brandt G, Brandt O, Bratzler U, Brau B, Brau J E, Braun H M, Breaden Madden W D, Brendlinger K, Brennan A J, Brenner L, Brenner R, Bressler S, Bristow K, Bristow T M, Britton D, Britzger D, Brochu F M, Brock I, Brock R, Bronner J, Brooijmans G, Brooks T, Brooks W K, Brosamer J, Brost E, Bruckman de Renstrom P A, Bruncko D, Bruneliere R, Bruni A, Bruni G, Bruschi M, Bruscino N, Bryngemark L, Buanes T, Buat Q, Buchholz P, Buckley 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机构信息
CPPM, Aix-Marseille Université and CNRS/IN2P3, Marseille, France.
Homer L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman, OK USA.
出版信息
Eur Phys J C Part Fields. 2016;76:11. doi: 10.1140/epjc/s10052-015-3852-4. Epub 2016 Jan 7.
Fiducial cross-sections for [Formula: see text] production with one or two additional -jets are reported, using an integrated luminosity of 20.3 fb[Formula: see text] of proton-proton collisions at a centre-of-mass energy of 8 TeV at the Large Hadron Collider, collected with the ATLAS detector. The cross-section times branching ratio for [Formula: see text] events with at least one additional -jet is measured to be 950 [Formula: see text] 70 (stat.) [Formula: see text] (syst.) fb in the lepton-plus-jets channel and 50 [Formula: see text] 10 (stat.) [Formula: see text] (syst.) fb in the [Formula: see text] channel. The cross-section times branching ratio for events with at least two additional -jets is measured to be 19.3 [Formula: see text] 3.5 (stat.) [Formula: see text] 5.7 (syst.) fb in the dilepton channel ([Formula: see text], [Formula: see text], and ) using a method based on tight selection criteria, and 13.5 [Formula: see text] 3.3 (stat.) [Formula: see text] 3.6 (syst.) fb using a looser selection that allows the background normalisation to be extracted from data. The latter method also measures a value of 1.30 [Formula: see text] 0.33 (stat.) [Formula: see text] 0.28 (syst.)% for the ratio of [Formula: see text] production with two additional -jets to [Formula: see text] production with any two additional jets. All measurements are in good agreement with recent theory predictions.
报告了在大型强子对撞机质心能量为8 TeV的质子 - 质子碰撞中，利用ATLAS探测器收集的20.3 fb⁻¹的积分亮度，产生具有一个或两个额外喷注的[公式：见正文]的基准截面。在轻子加喷注通道中，至少有一个额外喷注的[公式：见正文]事件的截面乘以分支比被测量为950 ± 70（统计）±（系统）fb，在[公式：见正文]通道中为50 ± 10（统计）±（系统）fb。在双轻子通道（[公式：见正文]、[公式：见正文]和[公式：见正文]）中，使用基于严格选择标准的方法，至少有两个额外喷注的事件的截面乘以分支比被测量为19.3 ± 3.5（统计）± 5.7（系统）fb，而使用较宽松的选择（允许从数据中提取背景归一化）时为13.5 ± 3.3（统计）± 3.6（系统）fb。后一种方法还测量了具有两个额外喷注的[公式：见正文]产生与具有任意两个额外喷注的[公式：见正文]产生的比率为1.30 ± 0.33（统计）± 0.28（系统）%。所有测量结果与最近的理论预测都很好地吻合。
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