1,632 research outputs found
Strongly interacting Ï-electrons and MgB2â superconductivity
- Author
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2001
- Field of study
MgB(pnÏâpnÏâ)2â is classified as a system with strongly
interacting Ï-electrons and non-correlated Ï-electrons of boron
ions. The kinematic and Coulomb interaction V between the orbitally degenerated
Ï-electrons provide the superconducting state with an anisotropic gap of
s*-wave symmetry. The critical temperature Tcâ has a non-monotonic dependence
on the distance r between the centers of gravity of Ï- and Ï-bands.
MgB2â corresponds to r=0.085 eV and V=0.45 eV in our model with flat bands.
The derived superconducting density of electronic states is in good agreement
with available experimental and theoretical data. The possibilities for
increasing Tcâ are discussed.Comment: 8 pages, 4 figure
Primordial magnetic fields at preheating
- Author
- A Duif
- A Plecenik
- AF Andreev
- AGM Jansen
- AGM Jansen
- AN Omelâyanchuk
- AV Khotkevich
- AV Khotkevich
- AV Zaitsev
- AV Zaitsev
- C Renner
- CJ Muller
- EL Wolf
- GE Blonder
- IK Yanson
- IK Yanson
- IK Yanson
- IK Yanson
- IK Yanson
- IK Yanson
- IK Yanson
- IK Yanson
- IK Yanson
- IO Kulik
- IO Kulik
- JM Rowell
- KS Ralls
- M Jourdan
- PN Chubov
- RC Dynes
- SN Artemenko
- T Ekino
- VA Khlus
- VA Khlus
- WL McMillan
- YV Sharvin
- Publication venue
- Publication date
- 01/01/2000
- Field of study
Using lattice techniques we investigate the generation of long range
cosmological magnetic fields during a cold electroweak transition. We will show
how magnetic fields arise, during bubble collisions, in the form of magnetic
strings. We conjecture that these magnetic strings originate from the alignment
of magnetic dipoles associated with EW sphaleron-like configurations. We also
discuss the early thermalisation of photons and the turbulent behaviour of the
scalar fields after tachyonic preheating.Comment: 7 pages. Talk presented at Lattice200
Sadiman Volcano, Crater Highlands, Tanzania; does it really contain melilitites and carbonatites or its is just a phonolite-nephelinite volcano?
- Publication venue
- Department of Mineralogy, Geochemistry and Petrology, University of Szeged, Szeged, Hungary
- Publication date
- 18/06/2018
- Field of study
Sadiman is 4.8-4.0 Ma old volcano located in the Crater Highlands area in northern Tanzania. Limited published data and field observations show that it consists of interlayered phonolitic tuffs and nephelinitic lavas. Rare xenoliths of phonolite and ijolite were observed in the nephelinites. It was suggested that Sadiman volcano contains melilititic and carbonatitic rocks. These also occur as tuffs in the Laetoli area where fossilised footprints from human ancestors are known which is why Sadiman is of special interest as a possible source of them.The attached document is the authorsâ final accepted/submitted version of the journal article. You are advised to consult the publisherâs version if you wish to cite from it
Fabrication of digital rainbow holograms and 3 D imaging using SEM based e beam lithography
- Publication venue
- 'The Optical Society'
- Publication date
- 01/01/2014
- Field of study
Recent progress in magnesium-based thermoelectric materials
- Author
- Aizawa
- An
- Balout
- Banik
- Bathula
- Bernard-Granger
- Bhandari
- Boulet
- Bourgeois
- Bux
- Cederkrantz
- Champier
- Chen
- Chen
- Chen
- de Boor
- de Boor
- Du
- Du
- Fan
- Farahi
- Farahi
- Gabbar
- Ganeshan
- Gao
- Gao
- Gao
- Gelbstein
- Goldsmid
- Guin
- He
- Heller
- Heremans
- Hu
- Hu
- Ihou-Mouko
- Ikeda
- Isoda
- Isoda
- Isoda
- Isoda
- Jung
- Jung
- Kanatzidis
- Kasap
- Kato
- Khan
- Kim
- Kim
- Kim
- Kolezynski
- Koumoto
- Kozlov
- Kraemer
- Kuroki
- Kutorasinski
- Kutorasinski
- KutorasiĆski
- LeBlanc
- LeBlanc
- Liu
- Liu
- Liu
- Liu
- Liu
- Luo
- Mao
- Mars
- Morris
- Muto
- Nakamura
- Nemoto
- Nikitin
- Ning
- Niu
- Nolas
- Orr
- Pei
- Perumal
- Polymeris
- Pshenai-Severin
- Ravich
- Riffel
- Rowe
- Sakamoto
- Sakamoto
- Santos
- Santos
- Satyala
- Satyala
- Shi
- Skomedal
- Snyder
- Song
- Tan
- Tang
- Tang
- Tani
- Tani
- Tani
- Tani
- Tani
- Tobola
- U.S. Department of Energy
- Viennois
- Vlachos
- Wang
- Wang
- Wiberg
- Wu
- Yamini
- Yang
- Yazawa
- Yin
- Yin
- You
- Yu
- Yu
- Zaitsev
- Zaitsev
- Zaitsev
- Zaitsev
- Zaitsev
- Zaitsev
- Zebarjadi
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zheng
- Publication venue
- 'Royal Society of Chemistry (RSC)'
- Publication date
- 01/01/2018
- Field of study
Magnesium-based thermoelectric materials (Mg2X, X = Si, Ge, Sn) are considered one of the most attractive groups for large-scale application, due to their materialsâ high availability, low cost, low mass density and reasonably high efficiency. In this work, we present an overview of the recent developments relating to magnesium-based thermoelectric materials and review the current approaches towards high thermoelectric efficiency
Deducing the source and composition of rare earth mineralising fluids in carbonatites: insights from isotopic (C, O, 87Sr/86Sr) data from Kangankunde, Malawi
- Author
- A Demény
- A Loges
- A Williams-Jones
- AG Doroshkevich
- AG Doroshkevich
- AG Doroshkevich
- AN Mariano
- AN Zaitsev
- AN Zaitsev
- AN Zaitsev
- AO Nier
- AP Jones
- AR Chakhmouradian
- AR Chakhmouradian
- AR Chakhmouradian
- AR Chakhmouradian
- AR Woolley
- AR Woolley
- AR Woolley
- B BĂŒhn
- B Ngwenya
- Baruch Spiro
- C Xu
- Clemens V. Ullmann
- D DolejĆĄ
- DA Neave
- DR Nelson
- E Ruberti
- EI Hamilton
- F Andrade
- F Poitrasson
- F Wall
- F Wall
- F Wall
- F Wall
- F Wall
- Frances Wall
- G Cressey
- H Craig
- HP Taylor
- J Borthwick
- J Gittins
- J Horita
- J Keller
- J Kynicky
- J Trofanenko
- JM McCrea
- JS Ray
- JS Ray
- L Chai
- L Zhang
- L Zhou
- M Bas Le
- M Bau
- M Bau
- M Louvel
- M Moore
- N Pearce
- N Pearce
- NJ Snelling
- P Deines
- P Deines
- P Deines
- P Richet
- PJ Downes
- PL Verplanck
- RA Duraswami
- RH Steiger
- RN Clayton
- RV Santos
- S Broom-Fendley
- S Broom-Fendley
- S Broom-Fendley
- S Broom-Fendley
- S Castor
- S Dallas
- S Spötl
- Sam Broom-Fendley
- T Andersen
- T Chacko
- T Chacko
- URF Ziegler
- W McDonough
- Y Matsuhisa
- Y Ni
- ZS Cetiner
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 09/11/2017
- Field of study
This is the final version of the article. Available from Springer Verlag via the DOI in this record.Carbonatites host some of the largest and highest grade rare earth element (REE) deposits but the composition and source of their REE-mineralising fluids remains enigmatic. Using C, O and 87Sr/86Sr isotope data together with major and trace element compositions for the REE-rich Kangankunde carbonatite (Malawi), we show that the commonly observed, dark brown, Fe-rich carbonatite that hosts REE minerals in many carbonatites is decoupled from the REE mineral assemblage. REE-rich ferroan dolomite carbonatites, containing 8â15 wt% REE2O3, comprise assemblages of monazite-(Ce), strontianite and baryte forming hexagonal pseudomorphs after probable burbankite. The 87Sr/86Sr values (0.70302â0.70307) affirm a carbonatitic origin for these pseudomorph-forming fluids. Carbon and oxygen isotope ratios of strontianite, representing the REE mineral assemblage, indicate equilibrium between these assemblages and a carbonatite-derived, deuteric fluid between 250 and 400 °C (ÎŽ18O + 3 to + 5â°VSMOW and ÎŽ13C â 3.5 to â 3.2â°VPDB). In contrast, dolomite in the same samples has similar ÎŽ13C values but much higher ÎŽ18O, corresponding to increasing degrees of exchange with low-temperature fluids (< 125 °C), causing exsolution of Fe oxides resulting in the dark colour of these rocks. REE-rich quartz rocks, which occur outside of the intrusion, have similar ÎŽ18O and 87Sr/86Sr to those of the main complex, indicating both are carbonatite-derived and, locally, REE mineralisation can extend up to 1.5 km away from the intrusion. Early, REE-poor apatite-bearing dolomite carbonatite (beforsite: ÎŽ18O + 7.7 to + 10.3â° and ÎŽ13C â5.2 to â6.0â°; 87Sr/86Sr 0.70296â0.70298) is not directly linked with the REE mineralisation.This project was funded by the UK Natural Environment Research Council (NERC) SoS RARE project (NE/M011429/1) and by NIGL (NERC Isotope Geoscience Laboratory) Project number 20135
Assessment of Arthrobacter viscosus as reactive medium for forming permeable reactive biobarrier applied to PAHs remediation
- Author
- A Tiehm
- AK Haritash
- AN Mabbett
- C Karigar
- C Quintelas
- C Quintelas
- C Raghukumar
- D Ăetin
- E LĂłpez
- E Manoli
- E Rosales
- F Costa
- F Moscoso
- F Moscoso
- G BlĂĄzquez
- G Rytwo
- GM Zaitsev
- H Peng
- J He
- K Furukawa
- L. Ferreira
- M Nadal
- M Pazos
- M. A. SanromĂĄn
- M. Cobas
- M. Pazos
- MIM Ferreira
- MT AlcĂĄntara
- OB Akpor
- R Thiruvenkatachari
- RH Peng
- S Kocaoba
- S Lameiras
- S Saponaro
- SK Samanta
- SM Bamforth
- T Srinath
- T. Tavares
- U Sack
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/10/2013
- Field of study
Polycyclic aromatic hydrocarbons (PAHs) are significant environmental contaminants as they are present naturally as well as anthropogenically in soil, air and water. In spite of their low solubility, PAHs are spread to the environment, and they are present in surface water, industrial effluent or groundwater. Amongst all remediation technologies for treating groundwater contaminated with PAHs, the use of a permeable reactive biobarrier (PRBB) appears to be the most cost-effective, energy efficient, and environmentally sound approach. In this technology, the microorganisms are used as reactive medium to degrade or stabilize the contaminants. The main limits of this approach are that the microorganisms or consortium used for forming the PRBB should show adequate characteristics. They must be retained in the barrier-forming biofilm, and they should also have degradative ability for the target pollutants. The aim of the present work is to evaluate the viability of Arthrobacter viscosus as bioreactive medium for forming PRBB. Initially, the ability of A. viscosus to remove PAHs, benzo[a]anthracene 100 ÎŒM and phenanthrene 100 ÎŒM was evaluated operating in a batch bench-scale bioreactor. In both cases, total benzo[a]anthracene and phenanthrene removals were obtained after 7 and 3 days, respectively. Furthermore, the viability of the microorganisms was evaluated in the presence of chromium in a continuous mode. As a final point, the adhesion of A. viscosus to sepiolite forming a bioreactive material to build PRBB was demonstrated. In view of the attained results, it can be concluded that A. viscosus could be a suitable microorganism to form a bioreactive medium for PAHs remediation.This work has been supported by the Spanish Ministry of Economy and Competitiveness and FEDER Funds (Project CTM 2011-25389). Marta Pazos received financial support under the Ramon y Cajal programme and Marta Cobas under the final project master grant "Campus do Mar Knowledge in depth"
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
- Bhattarai P
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boutle SK
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Camelia EA
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cantero J
- Cao T
- Cao Y
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carter JWS
- Casado MP
- Casha AF
- Casper DW
- Castelijn R
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Cerda Alberich L
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chau CC
- Che S
- Chekanov S
- Chekulaev S
- Chelkov GA
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov M
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Chytka L
- Cieri D
- Ciesla KM
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark MR
- Clark PJ
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Cohen H
- Coimbra AEC
- Cole B
- Colijn AP
- Collot J
- Conde Muino P
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Corga KDV
- Cormier F
- Cormier KJR
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Cowan G
- Cowley JW
- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cukierman AR
- Cunningham WR
- Czekierda S
- Czodrowski P
- D'amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- da Costa JBG
- Da Fonseca Pinto J
- Da Via C
- Dabrowski W
- Dachs F
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Dann NS
- Danninger M
- Dao V
- Darbo G
- Dartsi O
- Dattagupta A
- Daubney T
- David C
- Davidek T
- Davis DR
- Dawson I
- De Asmundis R
- De Beurs M
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DEF
- De Lima RT
- De Maria A
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Sousa MJDCS
- De K
- Debenedetti C
- Dedovich D
- Deiana AM
- Del Peso J
- Delgove D
- Deliot F
- Delitzsch CM
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Demontigny G
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Deutsch C
- Devesa MR
- Deviveiros PO
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Micco B
- Di Nardo R
- Di Petrillo KF
- Di Sipio R
- Diaconu C
- Dias FA
- Diaz LP
- Diaz MA
- Diaz YD
- Dickinson J
- Diehl EB
- Dietrich J
- Dimitrievska A
- Ding W
- Dingfelder J
- Dittus F
- Djama F
- Djobava T
- Djuvsland J
- Do Vale TD
- Dobre M
- Dodsworth D
- Doglioni C
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
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- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fbâ1 of â s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
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- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
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- Avramidou R
- Axen D
- Ay C
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- Azuma Y
- Baak MA
- Baccaglioni G
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- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
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- Baker MD
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
- Author
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- Yamazaki Y
- Yan Z
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- Yanush S
- Yao L
- Yao Y
- Yasu Y
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- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
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- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
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- Yu J
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- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal ZâČ Models
- âŠ