78 research outputs found
Impact of amendments on the physical properties of soil under tropical long-term no till conditions
- Author
- A Klute
- A Leys
- A Marsili
- AJ Franzluebbers
- Antonio C. A. Carmeis Filho
- AP Edwards
- B van Raij
- B van Raij
- C Briedis
- C Castro Filho
- CA Tormena
- CAC Crusciol
- Carlos A. C. Crusciol
- CH Roth
- D Baldock
- EF Caires
- EF Caires
- EF Caires
- EF Caires
- EJ Kiehl
- ET Elliott
- F Dube
- FJ Garbuio
- FP Valzano
- G Ogner
- GR Blake
- GSA Castro
- H Cantarella
- J Lehmann
- J RĂŒhlmann
- J Six
- JA Alcarde
- JC CorrĂȘa
- JM Reichert
- JM Tisdall
- Jorge Paz-Ferreiro
- JP Mitchell
- JSC Mbagwu
- Juliano C. Calonego
- K Denef
- KA Smith
- KM Hati
- M Manna
- M Muneer
- M Pagliai
- MCS Carvalho
- MD Bongiovanni
- MH McCallum
- MPW Farina
- MR Martins
- NK Fageria
- NK Fageria
- O Traoré
- R Lal
- RA Garcia
- RJ Haynes
- S Abiven
- Sacha J. Mooney
- T Chevallier
- Tiara M. GuimarĂŁes
- WD Kemper
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/12/2016
- Field of study
Tropical regions have been considered the world's primary agricultural frontier; however, some physico-chemical deficiencies, such as low soil organic matter content, poor soil structure, high erodibility, soil acidity, and aluminum toxicity, have affected their productive capacity. Lime and gypsum are commonly used to improve soil chemical fertility, but no information exists about the long-term effects of these products on the physical attributes and C protection mechanisms of highly weathered Oxisols. A field trial was conducted in a sandy clay loam (kaolinitic, thermic Typic Haplorthox) under a no-tillage system for 12 years. The trial consisted of four treatments: a control with no soil amendment application, the application of 2.1 Mg ha-1 phosphogypsum, the application of 2.0 Mg ha-1 lime, and the application of lime + phosphogypsum (2.0 + 2.1 Mg ha-1, respectively). Since the experiment was established in 2002, the rates have been applied three times (2002, 2004, and 2010). Surface liming effectively increased water-stable aggregates > 2.0 mm at a depth of up to 0.2 m; however, the association with phosphogypsum was considered a good strategy to improve the macroaggregate stability in subsoil layers (0.20 to 0.40 m). Consequently, both soil amendments applied together increased the mean weight diameter (MWD) and geometric mean diameter (GMD) in all soil layers, with increases of up to 118 and 89%, respectively, according to the soil layer. The formation and stabilization of larger aggregates contributed to a higher accumulation of total organic carbon (TOC) on these structures. In addition to TOC, the MWD and aggregate stability index were positively correlated with Ca2+ and Mg2+ levels and base saturation. Consequently, the increase observed in the aggregate size class resulted in a better organization of soil particles, increasing the macroporosity and reducing the soil bulk density and penetration resistance. Therefore, adequate soil chemical management plays a fundamental role in improving the soil's physical attributes in tropical areas under conservative management and highly affected by compaction caused by intensive farming
Observation of Two New Excited Îb0 States Decaying to Îb0 K-Ï+
- Author
- Aaij R
- Abdelmotteleb ASW
- Abrantes FG
- Ackernley T
- Adeva B
- Adinolfi M
- Afsharnia H
- Agapopoulou C
- Aidala CA
- Aiola S
- Ajaltouni Z
- Akar S
- Akiba KC
- Albero AA
- Albrecht J
- Alepuz CR
- Alessio F
- Alexander M
- Aliouche Z
- Alkhazov G
- Altarelli MP
- Amato S
- Amey JL
- Amhis Y
- An L
- Anderlini L
- Andreianov A
- Andreotti M
- Archilli F
- Artamonov A
- Artuso M
- Arzymatov K
- Aslanides E
- Atzeni M
- Audurier B
- Bachmann S
- Bachmayer M
- Back JJ
- Balagura V
- Baldini W
- Barajas CAC
- Barbetti M
- Barlow RJ
- Barsuk S
- Barter W
- Bartolini M
- Baryshnikov F
- Basels JM
- Bashir S
- Bassi G
- Batsukh B
- Battig A
- Bay A
- Beck A
- Becker M
- Bedeschi F
- Bediaga I
- Beiter A
- Belavin V
- Belin S
- Bellee V
- Belous K
- Belov I
- Belyaev I
- Ben-Haim E
- Bencivenni G
- Benito CM
- Berezhnoy A
- Bernet R
- Berninghoff D
- Bernstein HC
- Bertella C
- Bertolin A
- Betancourt C
- Beteta CA
- Betti F
- Bezshyiko I
- Bhasin S
- Bhom J
- Bian L
- Bieker MS
- Bifani S
- Billoir P
- Birch M
- Bishop FCR
- Bitadze A
- Bizzeti A
- Bjorn M
- Blago MP
- Blake T
- Blanc F
- Blusk S
- Bobulska D
- Boelhauve JA
- Boettcher T
- Boldyrev A
- Bondar A
- Bondar N
- Borghi S
- Borisyak M
- Borsato M
- Borsuk JT
- Bouchiba SA
- Bowcock TJV
- Boyer A
- Bozzi C
- Bradley MJ
- Braun S
- Brodski M
- Brodzicka J
- Brundu D
- Buonaura A
- Buonincontri L
- Burke AT
- Burr C
- Bursche A
- Butkevich A
- Butter JS
- Buytaert J
- Byczynski W
- Cadeddu S
- Cai H
- Calabrese R
- Calefice L
- Cali S
- Calladine R
- Calvi M
- Campana P
- Canudas NV
- Capelli S
- Capriotti L
- Carbone A
- Carboni G
- Cardinale R
- Cardini A
- Cardoso LAG
- Carli I
- Carniti P
- Cartelle PA
- Carus L
- Casasus MP
- Casse G
- Castro AP
- Castro JL
- Cattaneo M
- Cavallero G
- Cazon BRG
- Celani S
- Cerasoli J
- Cervenkov D
- Chadwick AJ
- Chapman MG
- Charles M
- Charpentier P
- Chatzikonstantinidis G
- Chefdeville M
- Chen C
- Chen S
- Chernov A
- Chobanova V
- Cholak S
- Chrzaszcz M
- Chubykin A
- Chulikov V
- Ciambrone P
- Cicala MF
- Ciezarek G
- Clarke PEL
- Clemencic M
- Cliff HV
- Closier J
- Cobbledick JL
- Coco V
- Coelho JAB
- Cogan J
- Cogneras E
- Cojocariu L
- Collins P
- Colombo T
- Congedo L
- Contu A
- Cooke N
- Coombs G
- Corredoira I
- Corti G
- Coutinho RS
- Couturier B
- Craik DC
- Crkovska J
- Currie R
- D'Ambrosio C
- D'Argent P
- Da Silva CL
- Dadabaev S
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- Dalseno J
- Danilina A
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- Davis A
- De Almeida FLS
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- De Miranda JM
- De Paula BS
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- De Serio M
- De Simone D
- De Simone P
- de Vries JA
- Dean CT
- Decamp D
- Dedu V
- Del Buono L
- Delaney B
- Dembinski HP
- Dendek A
- Denysenko V
- Derkach D
- Deschamps O
- Desse F
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- Di Cicco A
- Di Nezza P
- Diaz LC
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- Dijkstra H
- Dobishuk V
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- Donohoe AM
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- Downes AG
- Dudek MW
- Dufour L
- Duk V
- Durante P
- Durham JM
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- Egede U
- Egorychev V
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- Fazzini D
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- Fernandez RAR
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- Figueras EV
- Filippov S
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- Firlej M
- Fischer KM
- Fitzgerald DS
- Fitzpatrick C
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- Fleuret F
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- Gioventu A
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- Gkougkousis EL
- Gligorov VV
- Gobel C
- Goicochea JMO
- Golobardes E
- Golubkov D
- Golutvin A
- Gomes A
- Gomez MC
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- Gonzalo AB
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- Grabowski JP
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- Graverini E
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- Hulsbergen W
- Hunter RJ
- Hushchyn M
- Hutchcroft D
- Hynds D
- Ibis P
- Idzik M
- Ilin D
- Ilten P
- Inglessi A
- Ishteev A
- Ivshin K
- Jacobsson R
- Jage H
- Jakobsen S
- Jans E
- Jashal BK
- Jawahery A
- Jevtic V
- Jiang F
- John M
- Johnson D
- Jones CR
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- Jost B
- Jurik N
- Kadavath SHK
- Kandybei S
- Kang Y
- Karacson M
- Karpov M
- Keizer F
- Keller DM
- Kenzie M
- Ketel T
- Khanji B
- Kharisova A
- Kholodenko S
- Kirn T
- Kirsebom VS
- Kitouni O
- Klaver S
- Kleijne N
- Klimaszewski K
- Kmiec MR
- Koliiev S
- Kondybayeva A
- Konoplyannikov A
- Kopciewicz P
- Kopecna R
- Koppenburg P
- Korolev M
- Kostiuk I
- Kot O
- Kotriakhova S
- Kravchenko P
- Kravchuk L
- Krawczyk RD
- Kreps M
- Kress F
- Kretzschmar S
- Krokovny P
- Krupa W
- Krzemien W
- Kucewicz W
- Kucharczyk M
- Kudryavtsev V
- Kuindersma HS
- Kunde GJ
- Kvaratskheliya T
- Lacarrere D
- Lafferty G
- Lai A
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- Langenbruch C
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- Leite JB
- Lener MP
- Leroy O
- Lesiak T
- Leverington B
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- Li P
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- Liang X
- Lima VF
- Lin T
- Lindner R
- Lisovskyi V
- Litvinov R
- Liu G
- Liu H
- Liu Q
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- Loi A
- Longstaff I
- Lopes JH
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- Lopez JAR
- Lovell GH
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- Lucarelli C
- Lucchesi D
- Luchuk S
- Lukashenko V
- Luo Y
- Lupato A
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- Lusiani A
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- Machado DT
- Machefert F
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- Mackowiak P
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- Madejczyk O
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- Magalhaes PC
- Maisuzenko D
- Majewski MW
- Malczewski JJ
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- Malecki B
- Malinin A
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- Marchand JF
- Marconi U
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- Massafferri A
- Materok M
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- Matiunin V
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- Mattioli KR
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- Mcconnell L
- Mcgrath TH
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- Morello G
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- Muzzetto P
- Naik P
- Nakada T
- Nandakumar R
- Nanut T
- Nasteva I
- Needham M
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- Neubert S
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- Nguyen TD
- Nguyen-Mau C
- Niel EM
- Nieswand S
- Nikitin N
- Nolte NS
- Norella ES
- Normand C
- Nunez C
- O'Hanlon DP
- O'Neil RH
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- Obraztsov V
- Oeser T
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- Oliva F
- Olivares ME
- Onderwater CJG
- Ossowska A
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- Oyanguren A
- Padeken KO
- Pagare B
- Pais PR
- Pajero T
- Palano A
- Palutan M
- Pan Y
- Panshin G
- Papanestis A
- Pappagallo M
- Pappalardo LL
- Pappenheimer C
- Pardinas JG
- Parker W
- Parkes C
- Passalacqua B
- Passaleva G
- Pastore A
- Patel M
- Patrignani C
- Pawley CJ
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- Pellegrino A
- Perazzini S
- Pereima D
- Pernas MR
- Perret P
- Petric M
- Petridis K
- Petrolini A
- Petrov A
- Petrucci S
- Petruzzo M
- Pham TTH
- Philippov A
- Pica L
- Piccini M
- Pietrzyk B
- Pietrzyk G
- Pili M
- Pinci D
- Pisani F
- Pizzichemi M
- Placinta V
- Plana BG
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- Polci F
- Poliakova M
- Poluektov A
- Polukhina N
- Polyakov I
- Polycarpo E
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- Poslavskii S
- Prasanth K
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- Qi H
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- Quagliani R
- Quezada AFC
- Quintana B
- Raab NV
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- Rademacker JH
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- Rangel MS
- Ratnikov F
- Raven G
- Reboud M
- Redi F
- Regueiro PV
- Reiss F
- Ren Z
- Renaudin V
- Resmi PK
- Ribatti R
- Ricciardi S
- Rinnert K
- Rios CS
- Robbe P
- Robertson G
- Rodrigues AB
- Rodrigues E
- Rodrigues FF
- Rodriguez AB
- Rodriguez ERRR
- Rodriguez PB
- Rollings A
- Roloff P
- Romanovskiy V
- Rosales FAG
- Roth JD
- Rotondo M
- Rudolph MS
- Ruf T
- Ryzhikov A
- Ryzka J
- Sagidova N
- Sahoo N
- Saitta B
- Salomoni M
- Salvia AL
- Santacesaria R
- Santimaria M
- Santos DM
- Santovetti E
- Saranin D
- Sarpis G
- Sarpis M
- Sarti A
- Satriano C
- Satta A
- Saur M
- Savrina D
- Sazak H
- Scarabotto A
- Schael S
- Scherl S
- Schiller M
- Schindler H
- Schmelling M
- Schmidt B
- Schmitt S
- Schneider O
- Schopper A
- Schubiger M
- Schulte S
- Schune MH
- Schwemmer R
- Sciascia B
- Sellam S
- Semennikov A
- Sergi A
- Serra N
- Sestini L
- Seuthe A
- Sevilla MF
- Shang Y
- Shangase DM
- Shapkin M
- Shchemerov I
- Shchutska L
- Shears T
- Shekhtman L
- Shen Z
- Shevchenko V
- Shields EB
- Shimizu Y
- Shmanin E
- Shupperd JD
- Siddi BG
- Sierra CV
- Silva JJS
- Simi G
- Simone S
- Skidmore N
- Skwarnicki T
- Slater MW
- Slazyk I
- Smallwood JC
- Smead LGS
- Smeaton JG
- Smetkina A
- Smith E
- Smith M
- Snoch A
- Soares M
- Soares MS
- Sobral CMC
- Sokoloff MD
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- Soler FJP
- Solino SL
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- Solovyev I
- Spaan B
- Spradlin P
- Stagni F
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- Stahl S
- Stanislaus S
- Steinkamp O
- Stenyakin O
- Stevens H
- Stone S
- Straticiuc M
- Strekalina D
- Suljik F
- Sun J
- Sun L
- Sun Y
- Svihra P
- Swallow PN
- Swientek K
- Szabelski A
- Szumlak T
- Szymanski M
- T'Jampens S
- Taneja S
- Tanner AR
- Tat MD
- Terentev A
- Teubert F
- Thomas E
- Thompson DJD
- Thomson KA
- Tisserand V
- Tobin M
- Tomassetti L
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- Torreira AG
- Torres MC
- Tou DY
- Tran MT
- Trejo RIR
- Trifonova E
- Trippl C
- Tuci G
- Tully A
- Tuning N
- Ukleja A
- Unverzagt DJ
- Ursov E
- Usachov A
- Ustyuzhanin A
- Uwer U
- Vagner A
- Vagnoni V
- Valassi A
- Valenti G
- van Beuzekom M
- Van Dijk M
- van Herwijnen E
- Van Hulse CB
- van Veghel M
- Vecchi S
- Velthuis JJ
- Veltri M
- Venkateswaran A
- Veronesi M
- Vesterinen M
- Vidal AC
- Vidal AR
- Vidal FM
- Vidal JR
- Vidal XC
- Vieira D
- Viemann H
- Vilasis-Cardona X
- Villa A
- Vincent P
- Volle FC
- Vom Bruch D
- Vorobyev A
- Vorobyev V
- Voropaev N
- Vos K
- Waldi R
- Walsh J
- Wang C
- Wang J
- Wang J
- Wang J
- Wang J
- Wang M
- Wang R
- Wang Y
- Wang Z
- Wang Z
- Wang Z
- Ward JA
- Watson NK
- Weber SG
- Websdale D
- Weisser C
- Westhenry BDC
- White DJ
- Whitehead M
- Wiederhold AR
- Wiedner D
- Wilkinson G
- Wilkinson M
- Williams I
- Williams M
- Williams MRJ
- Wilson FF
- Wislicki W
- Witek M
- Witola L
- Wormser G
- Wotton SA
- Wu H
- Wyllie K
- Xiang Z
- Xiao D
- Xie Y
- Xu A
- Xu J
- Xu L
- Xu M
- Xu Q
- Xu Z
- Xu Z
- Yang D
- Yang S
- Yang Y
- Yang Z
- Yang Z
- Yao Y
- Yeomans LE
- Yin H
- Yu J
- Yuan X
- Yushchenko O
- Zaffaroni E
- Zavertyaev M
- Zdybal M
- Zenaiev O
- Zeng M
- Zhang D
- Zhang L
- Zhang S
- Zhang S
- Zhang Y
- Zhang Y
- Zharkova A
- Zhelezov A
- Zheng Y
- Zhou T
- Zhou X
- Zhou Y
- Zhovkovska V
- Zhu X
- Zhu X
- Zhu Z
- Zhukov V
- Zonneveld JB
- Zou Q
- Zucchelli S
- Zuliani D
- Zunica G
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
Two narrow resonant states are observed in the Îb0K-Ï+ mass spectrum using a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV, collected by the LHCb experiment and corresponding to an integrated luminosity of 6 fb-1. The minimal quark content of the Îb0K-Ï+ system indicates that these are excited Îb0 baryons. The masses of the Îb(6327)0 and Îb(6333)0 states are m[Îb(6327)0]=6327.28-0.21+0.23±0.12±0.24 and m[Îb(6333)0]=6332.69-0.18+0.17±0.03±0.22 MeV, respectively, with a mass splitting of Îm=5.41-0.27+0.26±0.12 MeV, where the uncertainties are statistical, systematic, and due to the Îb0 mass measurement. The measured natural widths of these states are consistent with zero, with upper limits of Î[Îb(6327)0]<2.20(2.56) and Î[Îb(6333)0]<1.60(1.92) MeV at a 90% (95%) credibility level. The significance of the two-peak hypothesis is larger than nine (five) Gaussian standard deviations compared to the no-peak (one-peak) hypothesis. The masses, widths, and resonant structure of the new states are in good agreement with the expectations for a doublet of 1D Îb0 resonances
Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- AdĂĄn DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aime' C
- Akchurin N
- Akgun B
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- Ăzçelik Ă
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams MR
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- Adzic P
- AdĂĄn DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmad WH
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Allen B
- Almond J
- Alonso AG
- Alvarez JDR
- Alverson G
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- Alves GA
- Aly R
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- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
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- Andreev Y
- Andrews MB
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- Angioni GLP
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- Anuar AAB
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- Ăzçelik Ă
- Publication venue
- Publication date
- 01/01/2020
- Field of study
We describe a method to obtain point and dispersion estimates for the energies of jets arising from b quarks produced in proton-proton collisions at an energy of s = 13 TeV at the CERN LHC. The algorithm is trained on a large sample of simulated b jets and validated on data recorded by the CMS detector in 2017 corresponding to an integrated luminosity of 41 fb - 1 . A multivariate regression algorithm based on a deep feed-forward neural network employs jet composition and shape information, and the properties of reconstructed secondary vertices associated with the jet. The results of the algorithm are used to improve the sensitivity of analyses that make use of b jets in the final state, such as the observation of Higgs boson decay to b b ÂŻ
Recommended from our members
Measurement of the differential ttÂŻ production cross section as a function of the jet mass and extraction of the top quark mass in hadronic decays of boosted top quarks
- Author
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- Abbaneo D
- Abbiendi G
- Abbrescia M
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- Yumiceva F
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- Yzquierdo AP-C
- Zabi A
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- Zorbakir IS
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- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Ălvarez CR
- Publication venue
- Springer Nature
- Publication date
- 03/07/2023
- Field of study
Data Availability:
This manuscript has no associated data or the data will not be deposited. [Authorsâ comment: Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in https://cms-docdb.cern.ch/cgibin/PublicDocDB/RetrieveFile?docid=6032 &filename=CMSDataPolicyV1.2.pdf &version=2.]A measurement of the jet mass distribution in hadronic decays of Lorentz-boosted top quarks is presented. The measurement is performed in the lepton + jets channel of top quark pair production (ttÂŻ
) events, where the lepton is an electron or muon. The products of the hadronic top quark decay are reconstructed using a single large-radius jet with transverse momentum greater than 400GeV
. The data were collected with the CMS detector at the LHC in proton-proton collisions and correspond to an integrated luminosity of 138fbâ1
. The differential ttÂŻ
production cross section as a function of the jet mass is unfolded to the particle level and is used to extract the top quark mass. The jet mass scale is calibrated using the hadronic W boson decay within the large-radius jet. The uncertainties in the modelling of the final state radiation are reduced by studying angular correlations in the jet substructure. These developments lead to a significant increase in precision, and a top quark mass of 173.06±0.84GeV.SCOAP
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- Author
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- Ăzçelik Ă
- Publication venue
- Springer Science and Business Media LLC
- Publication date
- 07/07/2022
- Field of study
A Correction to this paper has been published (18 October 2023) : https://doi.org/10.1038/s41586-023-06164-8.Data availability:
Tabulated results are provided in the HEPData record for this analysis. Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS data preservation, re-use and open acess policy.Code availability:
The CMS core software is publicly available on GitHub (https://github.com/cms-sw/cmssw).In July 2012, the ATLAS and CMS collaborations at the CERN Large Hadron Collider announced the observation of a Higgs boson at a mass of around 125âgigaelectronvolts. Ten years later, and with the data corresponding to the production of a 30-times larger number of Higgs bosons, we have learnt much more about the properties of the Higgs boson. The CMS experiment has observed the Higgs boson in numerous fermionic and bosonic decay channels, established its spinâparity quantum numbers, determined its mass and measured its production cross-sections in various modes. Here the CMS Collaboration reports the most up-to-date combination of results on the properties of the Higgs boson, including the most stringent limit on the cross-section for the production of a pair of Higgs bosons, on the basis of data from protonâproton collisions at a centre-of-mass energy of 13âteraelectronvolts. Within the uncertainties, all these observations are compatible with the predictions of the standard model of elementary particle physics. Much evidence points to the fact that the standard model is a low-energy approximation of a more comprehensive theory. Several of the standard model issues originate in the sector of Higgs boson physics. An order of magnitude larger number of Higgs bosons, expected to be examined over the next 15 years, will help deepen our understanding of this crucial sector.BMBWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, FAPERGS, and FAPESP (Brazil); MES and BNSF (Bulgaria); CERN; CAS, MoST, and NSFC (China); MINCIENCIAS (Colombia); MSES and CSF (Croatia); RIF (Cyprus); SENESCYT (Ecuador); MoER, ERC PUT and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRI (Greece); NKFIH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); MSIP and NRF (Republic of Korea); MES (Latvia); LAS (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MOS (Montenegro); MBIE (New Zealand); PAEC (Pakistan); MES and NSC (Poland); FCT (Portugal); MESTD (Serbia); MCIN/AEI and PCTI (Spain); MOSTR (Sri Lanka); Swiss Funding Agencies (Switzerland); MST (Taipei); MHESI and NSTDA (Thailand); TUBITAK and TENMAK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie programme and the European Research Council and Horizon 2020 Grant, contract Nos. 675440, 724704, 752730, 758316, 765710, 824093, 884104, and COST Action CA16108 (European Union); the Leventis Foundation; the Alfred P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation Ă la Recherche dans lâIndustrie et dans lâAgriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the F.R.S.-FNRS and FWO (Belgium) under the âExcellence of Science â EOSâ â be.h project n. 30820817; the Beijing Municipal Science & Technology Commission, No. Z191100007219010; the Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Stavros Niarchos Foundation (Greece); the Deutsche Forschungsgemeinschaft (DFG), under Germanyâs Excellence Strategy â EXC 2121 âQuantum Universeâ â 390833306, and under project number 400140256 - GRK2497; the Hungarian Academy of Sciences, the New National Excellence Program - ĂNKP, the NKFIH research grants K 124845, K 124850, K 128713, K 128786, K 129058, K 131991, K 133046, K 138136, K 143460, K 143477, 2020-2.2.1-ED-2021-00181, and TKP2021-NKTA-64 (Hungary); the Council of Science and Industrial Research, India; the Latvian Council of Science; the Ministry of Education and Science, project no. 2022/WK/14, and the National Science Center, contracts Opus 2021/41/B/ST2/01369 and 2021/43/B/ST2/01552 (Poland); the Fundação para a CiĂȘncia e a Tecnologia, grant CEECIND/01334/2018 (Portugal); the National Priorities Research Program by Qatar National Research Fund; MCIN/AEI/10.13039/501100011033, ERDF âa way of making Europeâ, and the Programa Estatal de Fomento de la InvestigaciĂłn CientĂfica y TĂ©cnica de Excelencia MarĂa de Maeztu, grant MDM-2017-0765 and Programa Severo Ochoa del Principado de Asturias (Spain); the Chulalongkorn Academic into Its 2nd Century Project Advancement Project, and the National Science, Research and Innovation Fund via the Program Management Unit for Human Resources & Institutional Development, Research and Innovation, grant B05F650021 (Thailand); the Kavli Foundation; the Nvidia Corporation; the SuperMicro Corporation; the Welch Foundation, contract C-1845; and the Weston Havens Foundation (USA)
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Search for light Higgs bosons from supersymmetric cascade decays in pp collisions at âs=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
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- Afanasiev S
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- Ahmad WH
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- Zorbilmez C
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- Zuo X
- Zuolo D
- Zygala L
- Ălvarez CR
- Ăzçelik Ă
- Publication venue
- Springer Science and Business Media LLC
- Publication date
- 06/07/2023
- Field of study
A search is reported for pairs of light Higgs
bosons (H1) produced in supersymmetric cascade decays in
f
inal states with small missing transverse momentum. A data
set of LHC pp collisions collected with the CMS detector
at âs = 13TeV and corresponding to an integrated lumi
nosity of 138fbâ1 is used. The search targets events where
both H1 bosons decay into bÂŻb pairs that are reconstructed
as large-radius jets using substructure techniques. No evi
dence is found for an excess of events beyond the back
ground expectations of the standard model (SM). Results
from the search are interpreted in the next-to-minimal super
symmetric extension of the SM, where a âsinglinoâ of small
mass leads to squark and gluino cascade decays that can pre
dominantly end in a highly Lorentz-boosted singlet-like H1
andasinglino-likeneutralinoofsmalltransversemomentum.
Upperlimitsaresetontheproductofthesquarkorgluinopair
production cross section and the square of the bÂŻb branching
fraction of the H1 in a benchmark model containing almost
mass-degenerategluinosandlight-flavoursquarks.Underthe
assumption of an SM-like H1 â bÂŻb branching fraction, H1
bosonswithmassesintherange40â120GeVarisingfromthe
decays of squarks or gluinos with a mass of 1200â2500GeV
are excluded at 95% confidence level.SCOA
Search for long-lived particles decaying to leptons with large impact parameter in proton-proton collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- AdĂĄn DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aimeâ C
- Akchurin N
- Akgun B
- Akpinar A
- Albergo S
- Albert A
- Albrecht S
- Albrow M
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Almond J
- Alonso AG
- Alpana K
- Alvarez JDR
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amarilo KM
- Ambrozas M
- Amendola C
- Amin N
- Amram O
- Amsler C
- An S
- An Y
- Anagnostou G
- Anampa KH
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- Andreassi G
- Andreev V
- Andreev Y
- Andrejkovic JW
- Andrews MB
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- Appelt E
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- Arbol PMRD
- Arcaro D
- Arcidiacono R
- Arenton MW
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- Arneodo M
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- Ălvarez CR
- Ăzçelik Ă
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/11/2021
- Field of study
Copyright © CERN for the benefit of the CMS collaboration 2022. A search for new long-lived particles decaying to leptons using protonâproton collision data produced by the CERN LHC at sâ=13TeV is presented. Events are selected with two leptons (an electron and a muon, two electrons, or two muons) that both have transverse impact parameter values between 0.01 and 10cm and are not required to form a common vertex. Data used for the analysis were collected with the CMS detector in 2016, 2017, and 2018, and correspond to an integrated luminosity of 118 (113)fbâ1 in the ee channel (eÎŒ and ΌΌ channels). The search is designed to be sensitive to a wide range of models with displaced eÎŒ, ee, and ΌΌ final states. The results constrain several well-motivated models involving new long-lived particles that decay to displaced leptons. For some areas of the available phase space, these are the most stringent constraints to date.SCOAP3
Recommended from our members
Search for low-mass dilepton resonances in Higgs boson decays to four-lepton final states in protonâproton collisions at âs=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
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- Aggleton R
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- Ahmed A
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- Ăzçelik Ă
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/04/2022
- Field of study
Data Availability: This manuscript has no associated data or the data will not be deposited. [Authorsâ comment: For CMS Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in âCMS data preservation, re-use and open access policyâ (https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032&filename=CMSDataPolicyV1.2.pdf&version=2).]Copyright © CERN for the benefit of the CMS collaboration 2022. A search for low-mass dilepton resonances in Higgs boson decays is conducted in the four-lepton final state. The decay is assumed to proceed via a pair of beyond the standard model particles, or one such particle and a Z boson. The search uses protonâproton collision data collected with the CMS detector at the CERN LHC, corresponding to an integrated luminosity of 137fbâ1, at a center-of-mass energy sâ=13TeV. No significant deviation from the standard model expectation is observed. Upper limits at 95% confidence level are set on model-independent Higgs boson decay branching fractions. Additionally, limits on dark photon and axion-like particle production, based on two specific models, are reported.SCOAP3
Search for dark matter produced in association with a leptonically decaying Z boson in protonâproton collisions at sâ=13TeV
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- Zeuner WD
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- Zygala L
- Ălvarez CR
- Ăzçelik Ă
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 07/12/2020
- Field of study
A search for dark matter particles is performed using events with a Z boson candidate and large missing transverse momentum. The analysis is based on protonâproton collision data at a center-of-mass energy of 13TeV, collected by the CMS experiment at the LHC in 2016â2018, corresponding to an integrated luminosity of 137fbâ1. The search uses the decay channels Zâee and ZâΌΌ. No significant excess of events is observed over the background expected from the standard model. Limits are set on dark matter particle production in the context of simplified models with vector, axial-vector, scalar, and pseudoscalar mediators, as well as on a two-Higgs-doublet model with an additional pseudoscalar mediator. In addition, limits are provided for spin-dependent and spin-independent scattering cross sections and are compared to those from direct-detection experiments. The results are also interpreted in the context of models of invisible Higgs boson decays, unparticles, and large extra dimensions.SCOAP
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