236 research outputs found
The Silkworm as a Source of Natural Antimicrobial Preparations: Efficacy on Various Bacterial Strains
- Publication venue
- 'MDPI AG'
- Publication date
- 01/01/2021
- Field of study
The global spread of multi-resistant pathogens responsible for infections, which cannot be treated with existing drugs such as antibiotics, is of particular concern. Antibiotics are becoming increasingly ineffective and drug resistance is leading to more difficult-to-treat infections; therefore, new bioactive compounds with antimicrobial activity are needed and new alternative sources should be found. Antimicrobial peptides (AMPs) are synthesized by processes typical of the innate immune system and are present in almost all organisms. Insects are extremely resistant to bacterial infections as they can produce a wide range of AMPs, providing an effective first line of defense. The AMPs produced by insects therefore represent a possible source of natural antimicrobial molecules. In this paper, the possibility of using plasma preparations from silkworm (Bombyx mori) larvae as a source of antimicrobials was evaluated. After simple purification steps, insect plasma was analyzed and tested on different Gram-positive and Gram-negative bacterial strains. The results obtained are encouraging as the assays on Escherichia coli and Enterobacter cloacae showed significant decrease in the growth of these Gram-negative bacteria. Similar results were obtained on Gram-positive bacteria, such as Micrococcus luteus and Bacillus subtilis, which showed strong susceptibility to the silkworm AMPs pool. In contrast, Staphylococcus aureus displayed high resistance to Bombyx mori plasma. Finally, the tested plasma formulations were assessed for possible storage not only at 4 \ub0C, but also above room temperature. In conclusion, partially purified plasma from silkworm could be a promising source of AMPs which could be used in formulations for topical applications, without additional and expensive purification steps
Insights Into the Immune Response of the Black Soldier Fly Larvae to Bacteria
- Publication venue
- 'Frontiers Media SA'
- Publication date
- 01/01/2021
- Field of study
In insects, a complex and effective immune system that can be rapidly activated by a plethora of stimuli has evolved. Although the main cellular and humoral mechanisms and their activation pathways are highly conserved across insects, the timing and the ef\ufb01cacy of triggered immune responses can differ among different species. In this scenario, an insect deserving particular attention is the black soldier \ufb02 y (BSF), Hermetia illucens (Diptera: Stratiomyidae). Indeed, BSF larvae can be reared on a wide range of decaying organic substrates and, thanks to their high protein and lipid content, they represent a valuable source of macromolecules useful for different applications (e.g., production of feedstuff, bioplastics, and biodiesel), thus contributing to the development of circular economy supply chains for waste valorization. However, decaying substrates bring the larvae into contact with different potential pathogens that can challenge their health status and growth. Although these life strategies have presumably contributed to shape the evolution of a sophisticated and ef \ufb01 cient immune system in this dipteran, knowledge
about its functional features is still fragmentary. In the present study, we investigated the processes underpinning the immune response to bacteria in H. illucens larvae and characterized their reaction times. Our data demonstrate that the cellular and humoral responses in this insect show different kinetics: phagocytosis and encapsulation are rapidly triggered after the immune challenge, while the humoral components intervene later. Moreover, although both Gram-positive and Gram-negative bacteria are completely removed from the insect body within a few hours after injection, Gram-positive bacteria persist in the hemolymph longer than do Gram-negative bacteria. Finally, the activity of
two key actors of the humoral response, i.e., lysozyme and phenoloxidase, show unusual dynamics as compared to other insects. This study represents the \ufb01 rst detailed characterization of the immune response to bacteria of H. illucens larvae, expanding
knowledge on the defense mechanisms of this insect among Diptera. This information is a prerequisite to manipulating the larval immune response by nutritional and environmental factors to increase resistance to pathogens and optimize health status during mass rearing
Cryptococcus neoformans Capsular Enlargement and Cellular Gigantism during Galleria mellonella Infection
- Author
- A Casadevall
- A Casadevall
- A Vecchiarelli
- A Vecchiarelli
- Arturo Casadevall
- BB Fuchs
- BB Fuchs
- BI Park
- C Charlier
- C Monari
- C Monari
- C Retini
- C Xue
- CJ Chrisman
- D Bergin
- D Bergin
- DB Morton
- DL Goldman
- DL Goldman
- DL Toffaletti
- E Mylonakis
- E Mylonakis
- EE McClelland
- EP Reeves
- FL Fonseca
- G Jander
- IM Dubovskiy
- J Grijpstra
- J Heitman
- JN Steenbergen
- JN Steenbergen
- JN Steenbergen
- JN Steenbergen
- JR Perfect
- Juan Luís Rodríguez-Tudela
- K Hu
- KJ Kwon-Chung
- L Cerenius
- LH Okagaki
- LM Pierini
- M Brennan
- M Cytrynska
- M Feldmesser
- M Feldmesser
- MA Gates
- Manuel Cuenca-Estrella
- ME Maxson
- MF Brivio
- ML Rodrigues
- MR Botts
- O Zaragoza
- O Zaragoza
- O Zaragoza
- O Zaragoza
- O Zaragoza
- O Zaragoza
- Oscar Zaragoza
- R London
- R Velagapudi
- RJ St Leger
- Robert A. Cramer
- Rocío García-Rodas
- S Miyata
- S Tojo
- TR Kozel
- TR Kozel
- W Chaka
- Y Apidianakis
- YC Chang
- ZM Dong
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
We have studied infection of Cryptococcus neoformans in the non-vertebrate host Galleria mellonella with particular interest in the morphological response of the yeast. Inoculation of C. neoformans in caterpillars induced a capsule-independent increase in haemocyte density 2 h after infection. C. neoformans manifested a significant increase in capsule size after inoculation into the caterpillar. The magnitude of capsule increase depended on the temperature, being more pronounced at 37°C than at 30°C, which correlated with an increased virulence of the fungus and reduced phagocytosis at 37°C. Capsule enlargement impaired phagocytosis by haemocytes. Incubation of the yeast in G. mellonella extracts also resulted in capsule enlargement, with the polar lipidic fraction having a prominent role in this effect. During infection, the capsule decreased in permeability. A low proportion of the cells (<5%) recovered from caterpillars measured more than 30 µm and were considered giant cells. Giant cells recovered from mice were able to kill the caterpillars in a manner similar to regular cells obtained from in vivo or grown in vitro, establishing their capacity to cause disease. Our results indicate that the morphological transitions exhibited by C. neoformans in mammals also occur in a non-vertebrate host system. The similarities in morphological transitions observed in different animal hosts and in their triggers are consistent with the hypothesis that the cell body and capsular responses represent an adaptation of environmental survival strategies to pathogenesis
Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at root s=8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adair A
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adzic P
- Agapitos A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Al-bataineh A
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Alderweireldt S
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alimena J
- Almond J
- Alunni Solestizi L
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Amsler C
- Anagnostou G
- Anderson D
- Anderson I
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Anelli C
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asilar E
- Asin I
- Askew A
- Ata M
- Attikis A
- Aubin A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Awad A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Baber M
- Bacchetta N
- Bachmair F
- Bachtis M
- Baden A
- Baffioni S
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Ball AH
- Ball F
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
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- Bargassa P
- Baringer P
- Barker A
- Barnes VE
- Barney D
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- Bartek R
- Barth C
- Bartosik N
- Bartók M
- Baskakov A
- Battilana C
- Baty A
- Bauerdick LAT
- Baumgartel D
- Baus C
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Beck L
- Beernaert K
- Behera PK
- Behnamian H
- Behnke O
- Behrens U
- Bein S
- Beirão Da Cruz E Silva C
- Belchior Batista Das Chagas E
- Belforte S
- Beliy N
- Belknap DA
- Bell KW
- Bellan R
- Belloni A
- Beluffi C
- Belyaev A
- Belyaev A
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- Bendavid J
- Benedetti D
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- Bhardwaj A
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- Bhattacharya R
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- Bhawandeep U
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- Castiñeiras De Saa JR
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- Cepeda M
- Cerati GB
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- Chabert EC
- Chamizo Llatas M
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- Ciocci MA
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- Ciulli V
- Civinini C
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- Cutts D
- Czellar S
- Da Costa EM
- Da Silveira GG
- Dabrowski A
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- Dahmes B
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- Di Mattia A
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- Dierlamm A
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- Dishaw A
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- Dittmann J
- Dittmar M
- Dittmer S
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- Dominguez A
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- Draeger AR
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- Erbacher R
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- Erdmann W
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- Erdweg S
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- Eskandari Tadavani E
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- Evangelou I
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- Evdokimov O
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- Haller J
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- Hatakeyama K
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- Heindl SM
- Heintz U
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- Hempel M
- Henderson C
- Hensel C
- Heracleous N
- Heredia-De La Cruz I
- Hernandez JM
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- Herndon M
- Hervé A
- Hidas D
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- Hindrichs O
- Hinzmann A
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- Hoehle F
- Hoepfner K
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- Hortiangtham A
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- Höing RS
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- Ibrahim ZA
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- Zorbilmez C
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- Zsigmond AJ
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Peer reviewe
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
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- Wulz C-E
- Wurthwein F
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- Yang UK
- Yang YC
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- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- Yu I
- Yu SS
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- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Elsevier BV'
- Publication date
- 10/09/2019
- Field of study
The production cross sections of B_{s}^{0} mesons and charge conjugates are measured in proton-proton (pp) and PbPb collisions via the exclusive decay channel B_{s}^{0}→J/ψϕ→μ^{+}μ^{−}K^{+}K^{−} at a center-of-mass energy of 5.02 TeV per nucleon pair and within the rapidity range |y|<2.4 using the CMS detector at the LHC. The pp measurement is performed as a function of transverse momentum (p_{T}) of the B_{s}^{0} mesons in the range of 7 to 50 GeV/c and is compared to the predictions of perturbative QCD calculations. The B_{s}^{0} production yield in PbPb collisions is measured in two p_{T} intervals, 7 to 15 and 15 to 50 GeV/c, and compared to the yield in pp collisions in the same kinematic region. The nuclear modification factor (R_{AA}) is found to be 1.5±0.6(stat)±0.5(syst) for 7–15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15–50 GeV/c, respectively. Within current uncertainties, the B_{s}^{0} results are consistent with models of strangeness enhancement, and suppression by parton energy loss, as observed for the B+ mesons
Measurement of the tt¯ production cross section, the top quark mass, and the strong coupling constant using dilepton events in pp collisions at √s = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Acharya H
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
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- Wurthwein F
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- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
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- Yang UK
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- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- Yu I
- Yu SS
- Yuan L
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 29/04/2019
- Field of study
A measurement of the top quark–antiquark pair production cross section σtt¯ in proton–proton collisions at a centre-of-mass energy of 13TeV is presented. The data correspond to an integrated luminosity of 35.9fb−1, recorded by the CMS experiment at the CERN LHC in 2016. Dilepton events (e ± μ ∓, μ+μ−, e+e−) are selected and the cross section is measured from a likelihood fit. For a top quark mass parameter in the simulation of mMCt=172.5GeV the fit yields a measured cross section σtt¯=803±2(stat)±25(syst)±20(lumi)pb, in agreement with the expectation from the standard model calculation at next-to-next-to-leading order. A simultaneous fit of the cross section and the top quark mass parameter in the POWHEG simulation is performed. The measured value of mMCt=172.33±0.14(stat)+0.66−0.72(syst)GeV is in good agreement with previous measurements. The resulting cross section is used, together with the theoretical prediction, to determine the top quark mass and to extract a value of the strong coupling constant with different sets of parton distribution functions
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexander J
- Alhusseini M
- Ali MAB Md
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JD Ruiz
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa K Hurtado
- Anderson D
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Angioni L Pinna
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
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- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arndt T
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asghar MI
- Asilar E
- Askew A
- Assran Y
- Atakisi IO
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avila C
- Ayala E
- Azarkin M
- Azhgirey I
- Aziz T
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- Azzolini V
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
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- Bachiller I
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- Backhaus M
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- Bahinipati S
- Baidali S
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- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
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- Bani L
- Bansal S
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- Barnyakov A
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- Barria P
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- Bartek R
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- Bartosik N
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- Baty A
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- Bauerdick LAT
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- Becerra DA Sanz
- Beernaert K
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at \sqrt{s} = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexander J
- Alhusseini M
- Ali MABM
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JDR
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Angioni GLP
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- Antunovic Z
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- Yazgan E
- Yetkin EA
- Yohay R
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- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
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- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
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- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuolo D
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2019
- Field of study
A search for nonresonant excesses in the invariant mass spectra of electron and muon pairs is presented. The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment in 2016, corresponding to a total integrated luminosity of 36 fb^{-1}. No significant deviation from the standard model is observed. Limits are set at 95% confidence level on energy scales for two general classes of nonresonant models. For a class of fermion contact interaction models, lower limits ranging from 20 to 32 TeV are set on the characteristic compositeness scale Λ. For the Arkani-Hamed, Dimopoulos, and Dvali model of large extra dimensions, the first results in the dilepton final state at 13 TeV are reported, and values of the ultraviolet cutoff parameter Λ_{T} below 6.9 TeV are excluded. A combination with recent CMS diphoton results improves this exclusion to Λ_{T} below 7.7 TeV, providing the most sensitive limits to date in nonhadronic final states
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta G
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexakhin V
- Alexander J
- Alhusseini M
- Ali MAB Md
- Alimena J
- Allen B
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- Alvarez Fernandez A
- Alvarez JD Ruiz
- Alverson G
- Alves FL
- Alves GA
- Alyari M
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- Amendola C
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- Amsler C
- Anagnostou G
- Anampa K Hurtado
- Anderson D
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Angioni GL Pinna
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
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- Arcaro D
- Arcidiacono R
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- Asawatangtrakuldee C
- Asghar MI
- Asilar E
- Askew A
- Assran Y
- Atakisi IO
- Atay S
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
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- Avery P
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- Ayala E
- Azarkin M
- Azhgirey I
- Aziz T
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- Azzurri P
- Baarmand MM
- Babaev A
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- Bachiller I
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Relative Modification of Prompt psi(2S) and J/psi Yields from pp to PbPb Collisions at root(S)(NN)=5.02 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
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- Rad N
- Radburn-Smith BC
- Radi A
- Radogna R
- Radziej M
- Ragazzi S
- Rahatlou S
- Rahbaran B
- Raics P
- Raidal M
- Rakness G
- Rander J
- Randle-conde A
- Rane A
- Ranieri A
- Ranjan K
- Rank D
- Rankin D
- Rappoccio S
- Raspereza A
- Rathjens D
- Ratti SP
- Rauco G
- Ravera F
- Raymond DM
- Razis PA
- Re V
- Rebassoo F
- Rebello Teles P
- Redjimi R
- Redondo I
- Regnard S
- Reid ID
- Reinsvold A
- Reis T
- Reithler H
- Rekovic V
- Riccardi C
- Ricci-Tam F
- Richards A
- Richardson C
- Richman J
- Rieger M
- Riley G
- Rinkevicius A
- Ristori L
- Rizzi A
- Roberts J
- Robmann P
- Robutti E
- Rodozov M
- Rodrigo T
- Rodrigues Antunes J
- Rodrigues AM
- Rodriguez JL
- Roecker S
- Roh Y
- Rohe T
- Rohlf J
- Rohringer H
- Roland B
- Roland C
- Roland G
- Rolandi G
- Romanowska-Rybinska K
- Romeo F
- Romero Abad D
- Romero A
- Romero L
- Ronchese P
- Roozbahani B
- Rorie J
- Roscher F
- Rose A
- Rose A
- Rose K
- Roskes J
- Rosowsky A
- Rossi AM
- Rossini M
- Rovelli C
- Rovelli T
- Rovere M
- Roy A
- Roy D
- Roy T
- Ruan M
- Ruchti R
- Ruckstuhl N
- Ruggles T
- Ruiz Alvarez JD
- Ruiz Vargas JC
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Ruspa M
- Russ J
- Ryd A
- Rykaczewski H
- Ryu G
- Ryu MS
- Ryutin R
- Sabes D
- Sacchi R
- Saddique A
- Safarzadeh B
- Safonov A
- Safronov G
- Sagir S
- Saha A
- Sahin MO
- Sahoo DK
- Sahoo N
- Saini LK
- Saka H
- Sakulin H
- Sakuma T
- Salazar Ibarguen HA
- Salerno D
- Salerno R
- Salfeld-Nebgen J
- Saltzberg D
- Salur S
- Salva S
- Salvini P
- Sanabria JC
- Sanchez Cruz S
- Sanchez MCDLB
- Sanchez-Hernandez A
- Sander C
- Sanders S
- Sani M
- Santanastasio F
- Santocchia A
- Santoro A
- Santra A
- Saoulidou N
- Sarica U
- Sarkar S
- Sarkar T
- Sauvan JB
- Savin A
- Savoy-Navarro A
- Savrin V
- Saxena P
- Schael S
- Schafer C
- Scharf C
- Scheuch F
- Schieck J
- Schleper P
- Schmidt A
- Schmitt MH
- Schnaible C
- Schnetzer S
- Schoerner-Sadenius T
- Schofbeck R
- Schomakers C
- Schonenberger M
- Schroeder M
- Schulte JF
- Schulz J
- Schumann S
- Schwandt J
- Schwick C
- Sciacca C
- Scodellaro L
- Sculac T
- Seez C
- Seidel M
- Seitz C
- Seixas J
- Sekmen S
- Selvaggi G
- Selvaggi M
- Sen S
- Seo SH
- Seva T
- Sevilla MF
- Sexton-Kennedy E
- Sguazzoni G
- Shah MA
- Shaheen SM
- Shalhout S
- Sharan M
- Sharma A
- Sharma A
- Sharma R
- Sharma S
- Sharma V
- Sharma V
- Shchelina K
- Shchutska L
- Sheffield D
- Sheldon P
- Shepherd-Themistocleous CH
- Shi X
- Shin YH
- Shirazi SMAG
- Shmatov S
- Shoaib M
- Shrinivas A
- Shtol D
- Shukla P
- Shulha S
- Shumeiko N
- Shvetsov I
- Si W
- Siado JE
- Sieber G
- Sikler F
- Silva CBDCE
- Silva P
- Silvestris L
- Simon S
- Simonetto F
- Simonis HJ
- Singh G
- Singh JB
- Sinthuprasith T
- Sirois Y
- Siroli GP
- Sirunyan AM
- Skatchkov N
- Skhirtladze N
- Skinnari L
- Skovpen K
- Skovpen Y
- Skuja A
- Smirnov V
- Smith D
- Smith G
- Smith J
- Smith N
- Smith VJ
- Smith WH
- Snigirev A
- Snow GR
- Snyder C
- Soares MS
- Sobol A
- Soffi L
- Soha A
- Sola V
- Solano A
- Solestizi LA
- Somalwar S
- Son DC
- Sonnenschein L
- Sordini V
- Sorokin P
- Spagnolo P
- Spalding WJ
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- Spannagel S
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- Spiegel L
- Spiezia A
- Spiridonov A
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- Squires M
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- Stadie H
- Stahl A
- Staiano A
- Starodumov A
- Stefaniuk N
- Stefanovitch R
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- Steinbrueck G
- Stenson K
- Stephans GSF
- Stickland D
- Stieger B
- Stober FM
- Stoever M
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- Stone R
- Stoye M
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- Strait J
- Strauss J
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- Stringer R
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- Stuart D
- Stupak J
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- Suarez Andres I
- Suarez I
- Suarez RG
- Sudic L
- Sulak L
- Sulimov V
- Sultanov G
- Summers S
- Sun J
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- Sun X
- Sung K
- Sur N
- Susa T
- Sutar B
- Suwonjandee N
- Svyatkovskiy A
- Swain SK
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- Syarif R
- Symonds P
- Szillasi Z
- Szleper M
- Sznajder A
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- Takahashi Y
- Takaki JDT
- Takasugi E
- Tali B
- Talvitie J
- Tambe N
- Tan P
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- Tapper A
- Taroni S
- Tatar K
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- Tavernier S
- Tavolaro VR
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- Teodorescu L
- Terkulov A
- Teyssier D
- Thakur S
- Thapa K
- Thea A
- Theofilatos K
- Tholen H
- Thom J
- Thomas L
- Thomas S
- Thomassen P
- Thueer S
- Thyssen F
- Tiko A
- Tiras E
- Titov M
- Tkaczyk S
- Tlisov D
- Toda S
- Toldaiev O
- Tomalin IR
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- Tonelli Manganote EJ
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- Tonjes MB
- Tonwar SC
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- Topsis-Giotis I
- Torassa E
- Toriashvili T
- Toropin A
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- Trocino D
- Trocsanyi ZL
- Troendle D
- Troshin S
- Trovato M
- Tsai JF
- Tsamalaidze Z
- Tsiakkouri D
- Tsirou A
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- Tucker J
- Tully C
- Tumasyan A
- Tuo S
- Tuominiemi J
- Tuovinen E
- Turkcapar S
- Turkewitz J
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- Tuuva T
- Tuve C
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- Tyurin N
- Tzeng YM
- Tziaferi E
- Uchida K
- Ujvari B
- Ulmer KA
- Ulrich R
- Undleeb S
- Uplegger L
- Uribe Estrada C
- Usai E
- Uzunian A
- Vaandering EW
- Vadruccio D
- Vai I
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- Valuev V
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- Van Doninck W
- Van Driessche W
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- Van Hove P
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- Van Mulders P
- Van Onsem GP
- Van Parijs I
- Van Remortel N
- Van Spilbeeck A
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- Vanlaer P
- Vannerom D
- Vardanyan I
- Varela J
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- Veelken C
- Velasco M
- Velde CV
- Velicanu D
- Velkovska J
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- Venturi A
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- Verdini PG
- Veres GI
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- Vernieri C
- Verweij M
- Verwilligen P
- Verzetti M
- Verzocchi M
- Veszpremi V
- Vesztergombi G
- Veverka J
- Vidal R
- Vignali MC
- Vila I
- Vilar Cortabitarte R
- Vilela Pereira A
- Viliani L
- Virdee T
- Viret S
- Vischia P
- Vitulo P
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- Volkov A
- Volobouev I
- Vormwald B
- Vorobiev I
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- Wolf R
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- Woodard A
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- Wu Z
- Wulsin HW
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- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xie S
- Xie W
- Xin Y
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- Yagil A
- Yalvac M
- Yang M
- Yang UK
- Yang Y
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- Yazgan E
- Yelton J
- Yetkin EA
- Yetkin T
- Yi K
- Yilmaz Y
- Yohay R
- Yonamine R
- Yoo HD
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- Yu I
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- Yumiceva F
- Yusli MN
- Zabel J
- Zabi A
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- Zagozdzinska A
- Zakaria M
- Zalewski P
- Zanetti A
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- Zarubin A
- Zeinali M
- Zenoni F
- Zenz SC
- Zeuner WD
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- Zhokin A
- Zhu RY
- Zhukova V
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- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- Zykunov V
- Publication venue
- Publication date
- 04/11/2016
- Field of study
Peer reviewe
- …