58 research outputs found
Phase structure of a two-fluid bosonic system
- Author
- Arias
- Arima
- Balanktekin
- Bijker
- Bijker
- Bohr
- Bès
- Caprio
- Casten
- Casten
- Davydov
- Dieperink
- Dieperink
- Dieperink
- Dieperink
- Dieperink
- Dobaczewski
- Duarte
- Ehrenfest
- Elliott
- F. Iachello
- Feng
- García-Ramos
- Gilmore
- Gilmore
- Gilmore
- Ginocchio
- Ginocchio
- Ginocchio
- Graham
- Harter
- Hartmann
- Heyde
- Heyde
- Iachello
- Iachello
- Iachello
- Iachello
- Iachello
- Jolie
- Ka-Hae Kim
- Leschber
- Leviatan
- Leviatan
- Leviatan
- Leviatan
- Leviatan
- Lipas
- López-Moreno
- M.A. Caprio
- Maragò
- Novoselsky
- Otsuka
- Otsuka
- Otsuka
- Rose
- Scholten
- Scholten
- Scholten
- Sevrin
- Sevrin
- Van Egmond
- Van Egmond
- Van Isacker
- Van Isacker
- Van Isacker
- Van Isacker
- Walet
- Warner
- Warner
- Zhang
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2005
- Field of study
The phase diagram of a two-fluid bosonic system is investigated. The
proton-neutron interacting boson model (IBM-2) possesses a rich phase structure
involving three control parameters and multiple order parameters. The surfaces
of quantum phase transition between spherical, axially-symmetric deformed, and
SU*(3) triaxial phases are determined, and the evolution of classical
equilibrium properties across these transitions is investigated. Spectroscopic
observables are considered in relation to the phase diagram.Comment: LaTeX (elsart), 46 pages, as published in Ann. Phys. (N.Y.
In Vitro Amplification of Misfolded Prion Protein Using Lysate of Cultured Cells
- Author
- A Balkema-Buschmann
- A Gorodinsky
- A Yanai
- AJ Beale
- C Kuwahara
- C Meyerett
- C Ryou
- C Soto
- CE Mays
- CE Mays
- CE Mays
- Charles E. Mays
- Chongsuk Ryou
- CR Birkett
- D Gonzalez-Romero
- F Wang
- Glenn C. Telling
- GP Saborio
- GP Saborio
- Hae-Eun Kang
- J Bian
- J Castilla
- J Castilla
- J Castilla
- J Castilla
- J-I Kim
- J-I Kim
- Jason C. Bartz
- JC Geoghegan
- JC Geoghegan
- JF Graham
- Jifeng Bian
- Jihyun Yeom
- Jiyan Ma
- JL Jainchill
- K Abid
- K Nishina
- KA Nishina
- KM Green
- L Thorne
- M Jones
- M Jones
- M Vey
- M-P Courageot
- MA Barria
- MH Tattum
- N Naslavsky
- N Stahl
- N-H Kim
- NJ Haley
- NR Deleault
- NR Deleault
- NR Deleault
- NR Deleault
- P Leblanc
- P Weber
- R Atarashi
- R Lucassen
- R Rubenstein
- RA Bessen
- RA Shikiya
- RJ Klebe
- S Shi
- SB Prusiner
- SB Prusiner
- TD Kurt
- TD Kurt
- Vadim Khaychuk
- Y Murayama
- Y Murayama
- Younghwan Kim
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Protein misfolding cyclic amplification (PMCA) recapitulates the prion protein (PrP) conversion process under cell-free conditions. PMCA was initially established with brain material and then with further simplified constituents such as partially purified and recombinant PrP. However, availability of brain material from some species or brain material from animals with certain mutations or polymorphisms within the PrP gene is often limited. Moreover, preparation of native PrP from mammalian cells and tissues, as well as recombinant PrP from bacterial cells, involves time-consuming purification steps. To establish a convenient and versatile PMCA procedure unrestricted to the availability of substrate sources, we attempted to conduct PMCA with the lysate of cells that express cellular PrP (PrPC). PrPSc was efficiently amplified with lysate of rabbit kidney epithelial RK13 cells stably transfected with the mouse or Syrian hamster PrP gene. Furthermore, PMCA was also successful with lysate of other established cell lines of neuronal or non-neuronal origins. Together with the data showing that the abundance of PrPC in cell lysate was a critical factor to drive efficient PrPSc amplification, our results demonstrate that cell lysate in which PrPC is present abundantly serves as an excellent substrate source for PMCA
Induction, characterization, and NMR-based metabolic profiling of adventitious root cultures from leaf explants of Gynura procumbens
- Author
- Anna Elisabeth Schulte
- C Simões-Gurgel
- CH Ho
- CH Wu
- CL Keng
- CS Jeong
- GA Akowuah
- HK Kim
- HK Kim
- JH Kim
- JP Hao
- KA Leiss
- KY Paek
- LG Korkina
- LM Perry
- M Khosh-Khui
- M Taya
- MA Baque
- MN Iskander
- Mohd Zuwairi Saiman
- N Dai
- N Praveen
- Natali Rianika Mustafa
- O Pérez-Tornero
- PS Sha Valli Khan
- Robert Verpoorte
- RV Reis
- SZ Hoe
- T Murashige
- U Mukundan
- W Jiratchariyakul
- X Qi
- XF Zhang
- XH Cui
- Y Toda
- YH Choi
- Young Hae Choi
- Z Hassan
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
25th annual computational neuroscience meeting: CNS-2016
- Author
- Abbott L.F.
- Abeysuriya Romesh G.
- Aertsen Ad
- Agnes Everton J.
- Ahamed Tosif
- Ahmadabadi Majid Nili
- Ahn Sora
- Aihara Kazuyuki
- Aihara Kazuyuki
- Andreassen Ole A.
- Andreassen Ole A.
- Ardestani Mohammad Hovaidi
- Ardestani Mohammad Hovaidi
- Arroyo David
- Aton Sara J.
- Babichev Andrey
- Bachmann Claudia
- Badel Laurent
- Baek Hyeon-Man
- Baek JeongHun
- Baek Kwangyeol
- Bahuguna Jyotika
- Bak Ji Hyun
- Baker Chris I.
- Bakker Rembrandt
- Balaguer‑Ballester Emili
- Bard G.
- Barnett William H.
- Baroni Fabiano
- Basnayake Kanishka
- Baysal Velt
- Bennett Matthew R.
- Bernard Christophe
- Berry Hugues
- Beuth Frederick
- Bezgin` Gleb
- Bill Johannes
- Birgolias Justas
- Blackwell Justin
- Bohnenkamp Lisa
- Bojak Ingo
- Borisyuk Roman
- Bos Hannah
- Bradley Samual P.
- Breakspear Michael
- Breitwieser Oliver
- Briaire` Jeroen J.
- Briggman Kevin L
- Brinkman Braden A.
- Brown John
- Brown Ritchie E.
- Brunel Nicolas
- Buhry Laure
- Buice Michael
- Burkitt Anthony N.
- Burton Shawn D.
- Buttler Simone
- Bytschok Ilja
- Cantarelli Matteo
- Chakravarthy V.Srinivasa
- Chan Ho Ka
- Chapman Phillip D.
- Chatzikalymniou Alexandra Pierri
- Chavane Frédéric
- Chen Liang
- Chen Weiliang
- Cheung Chung Ching
- Chhabria Karishma
- Chintaluri Chaitanya
- Choe Yoonsuck
- Choi Hannah
- Choi Hansol
- Choi Ilhwan
- Choi Jee Hyun
- Choi Woochul
- Choi Yun Seo
- Choung Oh‑hyeon
- Chung SueYeon
- Clarke Eric F.
- Clements Katie
- Cloherty Shaun L.
- Clopath Claudia
- Cocchi Luca
- Cohen Yale E.
- Cook Mark
- Crook Sharon M.
- Cserpán Dorottya
- Culmone Viviana
- Dabaghian Yuri
- Dabaghian Yuri
- Dale Anders M.
- Daly Kevin C.
- Dasgupta Sakyasingha
- Davey Neil
- Davey Neil
- Davison Andrew
- de Weerd Peter
- Deco Gustavo
- Demkó László
- Demutz Harald
- Denk Cornelia
- Destexhe Alain
- Devor Anna
- DeVuti Justin
- Diamond Alan
- Diesmann Markus
- Dillen Kim
- Doya Kenji
- Dragoi Valentin
- Draguljić Daniel
- Drew Jordan
- Drysdale Peter M.
- Duarte Renato
- Dura‑Bernal Salvador
- Dura‑Bernal Salvador
- Dura‑Bernal Salvador
- Edwards Andy
- Einevoll Gaute T.
- Elices Irene
- Elnevoll Gaute T.
- Ernst Udo A.
- Esler Timothy B.
- Esposito Elric
- Faraji Mohammad Java
- Fedorov Leonid A.
- Fenk Lisa M.
- Ferguson Katie
- Ferrario Andrea
- Filipovi Marko
- Fink Christian G.
- Fink Gereon R.
- Fishman Yonatan I.
- Fornito Alex
- Forrow Csaba
- Fouquet Coralie
- Frangou Sophia
- Freestone Dean R.
- Frijns Johan H. M.
- Fulcher Ben D.
- Fung Felix
- Gajic N. Alex Cayco
- Gallimore Andrew R.
- Gallinaro Júlia
- Gerkin Richard C.
- Gerstner Wulfram
- Giaffar Hamza
- Giese Martin
- Giese Martin
- Giese Martin A.
- Gilson Matthieu
- Gips Bart
- Gleeson Padraig
- Gliske Stephen V.
- Glomb Katharina
- Goetze Felix
- Goldsworthy Mitchell R.
- Gollo Leonardo L.
- Goncharenko Julia
- Goodarzinic Abdorreza
- Graham Bruce P.
- Grayden David B.
- Grayden David B.
- Grewe Jan
- Hadrava Michal
- Hagen Espen
- Halnes Geir
- Halnes Geir
- Hamade Khaldoun
- Hamker Fred H.
- Han Hio-Been
- Han Seung Kee
- Hansen Mads
- Harper Zachary J.
- He Hu
- Helias Moritz
- Hermann Christoph S.
- Hilgetag` Claus‑Christian
- Hines Michael L.
- Hlinka Jaroslav
- Hof Patrick R.
- Holman Katherine A.
- Hong Sungho
- Hordacre Brenton
- Howard Jr. James H.
- Huang Guang-Bin
- Huang Haiping
- Huerta Ramon
- Huh Dongsung
- Hutt Axel
- Hwang Dong‑Uk
- Hwang Eunjin
- Hye Jr. Eoon
- Iannella Nicolangelo
- Iannella Nicolangelo
- Ibbotson Michael R.
- Ionta Silvlo
- Ishii Shin
- Issa Fadi A.
- Iyer Ramakrishnan
- Jacobs Heidi
- Jang Hyun Jae
- Jang Jaeson
- Jang Jaeson
- Jensen Ole
- Jeong Jaeseung
- Jeong Jaesung
- Jeong Yong
- Jirsa Viktor K.
- Jo Sumin
- Joo Pangyu
- Josić Kresimir
- Ju Huiwen
- Jun Eunji
- Jun Sang Beom
- Jung Nam
- Jung Woo-Sung
- Jung Younginha
- Kahng B.
- Kale Penelope J.
- Kalkman Randy K.
- Kameneva Tatiana
- Kameneva Tatiana
- Kang Jiyoung
- Karoly Philippa J.
- Kasumi Ohta
- Kavalali Enge T.
- Kawato Mitsuo
- Kazama Hokto
- Kedziora David J.
- Kekona Tyler
- Keller Daniel
- Kennedy Henry
- Kepple Daniel
- Kerr Cliff C.
- Kerr Robert R.
- Kilpatrick Zachary P.
- Kim Ammo J.
- Kim Bowon
- Kim Bowon
- Kim Chang Sub
- Kim DaeEun
- Kim Hojeong
- Kim Hoon-Hee
- Kim Hyoungkyu
- Kim Jae Kyoung
- Kim Jimin
- Kim Jinseop
- Kim Juhee
- Kim Minjung
- Kim Seongkyun
- Kim Su Hyun
- Kim Sung-Phil
- Kim Sung-Phil
- Kim Tae
- Kim Taegyo
- Kim Won Sup
- Kim Youngsoo
- Kiser Seth A.
- Klanner Felix
- Kleberg Florence I.
- Klingbeil Guido
- Knösche Thomas
- Koren Veronika
- Koren Veronika
- Kotaleski Jeanette Hellgren
- Koulakov Alex
- Kralik Jerald D.
- Kringelbach Morten L.
- Kruscha Alexandra
- Kuhlmann Levin
- Kukolja Juraj
- Kumar Arvind
- Kumar Arvind
- Kundu Prantik
- Kunze Tim
- Kuravi Pradeep
- Kwag Jeehyun
- Kwon Jaehyung
- Lai Pik‑Yin
- Lakatos Peter
- Latorre Roberto
- Leahy Will
- Lee Changju
- Lee Chungho
- Lee Dan D.
- Lee Do-won
- Lee Heonsoo
- Lee Hyang Jung
- Lee Hyang Woon
- Lee Hyeonsu
- Lee Jae Woo
- Lee Jaejin
- Lee Jeungmin
- Lee Joonwon
- Lee Jung H.
- Lee Sang Wan
- Lee Sang-Hun
- Lee Seungjun
- Lee Soohyun
- Lee Sue-Hyun
- Lee Tae Ho
- Lee Won Hee
- Lee Yong‑il
- Lefebvre Baptiste
- Lefebvre Jérémie
- Leleu Timothée
- Leng Luziwei
- Levi Rafael
- Levina Anna
- Levy Brandon A.
- Li Luozheng
- Liang Guangsheng
- Lidner Benjamin
- Liedtke Joscha
- Lim Daeseob
- Lim Sewoong
- Lin Xiahoan
- Linder Benjamin
- Lines Glenn T.
- Lizler Joseph T.
- Lochmann Timm
- Lowet Eric
- Luebke Jennifer
- Lytton William W.
- Lytton William W.
- Lyu Cheng
- Ma Hailin
- Maeng Seung Eu
- Malmon Gabby
- Mandall Alekhya
- Maouene M.
- Marcelli Angelo
- Marin Boris
- Markin Sergey
- Markram Henry
- Marre Olivier
- Marsalek Petr
- Marsat Gary
- Martel Roman
- Marucci Lucia
- Maturana Matias I.
- McCarley Robert W.
- McDonnell Mark D.
- McDonnell Mark D.
- McKenna James T.
- McLauchlan Campbell
- Meffin Hamish
- Meffin Hamish
- Mehta Hima
- Meier Karlheinz
- Meijas Jorge F.
- Mellen Nick
- Memmeshei Raol-Martin
- Menzies Rosemary J.
- Merriosn-Hort Robert
- Metzner Christoph
- Mi Yuanyuan
- Mi Yuanyuan
- Mihalas Stefan
- Miller Thomas
- Moezzi Bahar
- Moezzi Bahar
- Molkov Yaroslav I.
- Moon Jangsup
- Moon Seok-hun
- Morris Laurel S.
- Morrison Abigail
- Mosqueiro Thiago S
- Mu Shang
- Muler Eilif
- Muralidharan Vignesh
- Murray John D.
- Murray Micha M.
- Mäki‑Marttunen Tuomo
- Neymotin Samuel
- Neymotin Samuel A.
- Niry Mohammad
- Nishikawa Isao
- Nolte Max
- Nowotny Thomas
- Oba Shigeyuki
- Obermayer Klaus
- Obermayer Klaus
- Ognjanovski Nicolette
- Ouyang Guang
- Ozer Mahmut
- Paik Se-Bum
- Paik Se‑Bum
- Palmer S.E.
- Palva Matias J.
- Paninski Liam
- Pariz Aref
- Park Chang-hyun
- Park Choongseok
- Park Hae‑Jeong
- Park Ji Sung
- Park Memming
- Park Sang-Min
- Park Sol
- Parsi Shervin S.
- Parziale Antonio
- Pasupathy Anitha
- Perotti Luca
- Peterson Andre
- Petkoski Spase
- Petrovici Mihai A.
- Petterson Klas H.
- Philips Ryan T.
- Phillips Ryan S.
- Pillow Jonathan
- Pittà Maurizio De
- Plogmacher Lukas
- Podlaski William
- Pollonini Luca
- Ponce‑Alvarez Adrián
- Popp Pamela Osborn
- Preuschoff Kerstin
- Priesemann Viola
- Priesemann Viola
- Priyadharsini B. Praga
- Psarrou Maria
- Quang Le Anh
- Quintana Adrian
- Ramsey Julia
- Ranjan Rajnish
- Rankin James
- Rankin James
- Rasch Malte J.
- Rasuli Nader
- Ratnadurai‑Giridharan Shivakeshavan
- Reig Ramon
- Reimann Michael W.
- Rennle Chris J.
- Reyes Amy
- Richter René
- Ridding Michael C.
- Rieke Fred
- Rinberg Dima
- Rinzel John
- Ritter Petra
- Roach James P.
- Robb Daniel T.
- Roberts Mark J.
- Robinson Peter A.
- Robinson Peter A.
- Rodriguez Francisco B.
- Rotter Stefan
- Rubchinsky Leonid L.
- Rubinov Mikail
- Rumbell Timothy
- Rupp André
- Rybak Ilya A.
- Ryu Juhyoung
- Sadeh Sadra
- Saggio Maria L.
- Sander Leonard M.
- Sanger Terence D.
- Sanz-Leon Paula
- Sanz‑Leon Paula
- Saska Daniel
- Schaworonkow Natalie
- Schemmel Johannes
- Scheutz Matthias
- Schiff Steven J.
- Schilstra Maria
- Schilstra Marla
- Schmidt Maximilian
- Schmidt Robert
- Schottdorf Manual
- Schutter Erik De
- Schwikard Achim
- Seeholzer Alexander
- Seidenstein Alexandra
- Sejnowski Terrence J.
- Sekulić Vladisla
- Senatore Rosa
- Senk Johanna
- Seo Sat Byul
- Seung H. Sebastian
- Sharpee Tatyana O.
- Shea Steven
- Shea-Brown Eric
- Shea‑Brown Eric
- Shen Kelly
- Shiau LieJune
- Shimazaki Hideaki
- Shin Hee‑sup
- Shin In-Seob
- Shivkumar Sabyasach
- Shlizerman Eli
- Shomali Safura Rashid
- Siep Silvan F.
- Silberberg Gilad
- Silver Angus
- Silver R. Angus
- Skiker K.
- Skilling Quinton M.
- Skinner Frances K.
- Skinner Frances K.
- Smit Daniel
- Smith Brian
- Smith Jeffrey
- Soh Jaehyun
- Soman Karthik
- Somogyvári Zoltán
- Sompolinsky Haim
- Song Min
- Song Min-Ho
- Song Youngjo
- Soundry Daniel
- Sourina Olga
- Spampinato Giulia Lia Beatrice
- Spiegler Andreas
- Spinney Richard E.
- Sprecher Simon
- Stacey William C.
- Stacey William C.
- Stephens Greg
- Stern Merav
- Steuber Volker
- Steyn-Ross D. Alistair
- Steyn-Ross Moira L.
- Stimberg Marcel
- Strube‑Bloss Martin F.
- Stöckel David
- Su Jianzhong
- Sun Haoqi
- Sweeney Yann
- Tabas Alejandro
- Tahayori Bahman
- Takashima Akira
- Tam Nicoladie D.
- Tamagnini Francesco
- Tang Rongxiang
- Tang Yi-Yuan
- Tang Yi-Yuan
- Teka Wondimu
- Tetzlaff Tom
- Tezuka Taro
- Toporikova Natalia
- Torres Joaquin J.
- Toyoizumi Taro
- Tran Patricia H. P.
- Trembleau Alain
- Triesch Jochen
- Trisch Jochen
- Tsaneva‑Atanasova Krasimira
- Tsuchimoto Yoshiko
- Tuomo Maki-Martun
- Tveito Aslak
- Valizadeh Alireza
- Valizadeh Alireza
- van Albada Sacha J
- van Albada Sacha J.
- van der Eerden Jan
- Varona Pablo
- Varona Pablo
- Veale Richard
- Viriyopase Atthaphon
- Vitay Julien
- Vogels Rufin
- Vogels Tim
- Vogels Tim P.
- Vogt Simon M.
- Voon Valerie
- Voronenko Sergej O.
- Vuust Peter
- Vörös János
- Wallentin Mikkel
- Wang Dahui
- Wang Jisung
- Wang Sheng-Ju
- Wang Yuzhe
- Warburton Julia M.
- Weaver Christina M.
- Wegener Detlef
- Weidel Philipp
- Welzig Charles M.
- Werdt Stephen Van
- Wibral Michael
- Wickens Jeffery R.
- Widmer Yves
- Witek Maria A. G.
- Witting Jens
- Wolf Fred
- Wong Michael
- Wu Si
- Wu Sl
- Wójcik Daniel K.
- Xu Zhiheng
- Yamada Yasnori
- Yamamura Yorkio
- Yang Huei-Fang
- Yang Xu
- Yeon Ji Won
- Yger Pierre
- Yilmaz Ergin
- Yoo Minsu
- Yoon Sangsup
- Yoshimoto Junichiro
- Young-Ah Rho
- Yu Suin
- Zaho Yuan
- Zamora Criseida
- Zaptocky Martin
- Zhang Mingsha
- Zhang Wenhao
- Zhao Chang
- Zhao Xiaochen
- Zhao Xuelong
- Zhou Changsong
- Zochowski Michal
- Zochowski Michal R.
- Zouridakis George
- Zurowski Bartosz
- Publication venue
- BMC
- Publication date
- 01/01/2016
- Field of study
The same neuron may play different functional roles in the neural circuits to which it belongs. For example, neurons in the Tritonia pedal ganglia may participate in variable phases of the swim motor rhythms [1]. While such neuronal functional variability is likely to play a major role the delivery of the functionality of neural systems, it is difficult to study it in most nervous systems. We work on the pyloric rhythm network of the crustacean stomatogastric ganglion (STG) [2]. Typically network models of the STG treat neurons of the same functional type as a single model neuron (e.g. PD neurons), assuming the same conductance parameters for these neurons and implying their synchronous firing [3, 4]. However, simultaneous recording of PD neurons shows differences between the timings of spikes of these neurons. This may indicate functional variability of these neurons. Here we modelled separately the two PD neurons of the STG in a multi-neuron model of the pyloric network. Our neuron models comply with known correlations between conductance parameters of ionic currents. Our results reproduce the experimental finding of increasing spike time distance between spikes originating from the two model PD neurons during their synchronised burst phase. The PD neuron with the larger calcium conductance generates its spikes before the other PD neuron. Larger potassium conductance values in the follower neuron imply longer delays between spikes, see Fig. 17.Neuromodulators change the conductance parameters of neurons and maintain the ratios of these parameters [5]. Our results show that such changes may shift the individual contribution of two PD neurons to the PD-phase of the pyloric rhythm altering their functionality within this rhythm. Our work paves the way towards an accessible experimental and computational framework for the analysis of the mechanisms and impact of functional variability of neurons within the neural circuits to which they belong
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Measurement of the differential tt¯ 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
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Acosta HAE
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Agram J-L
- Aguilar-Benitez M
- Agyel D
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Aimè C
- Akchurin N
- Akgun B
- Akpinar A
- Albert A
- Albrecht A
- Albrecht S
- Albrow M
- Alcerro LFA
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allmond B
- Almond J
- Alonso AG
- Alpana A
- Alvarez JDR
- Alverson G
- Alves BAFS
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amaral SMSD
- Amarilo KM
- Ambrozas M
- Amendola C
- Amin N
- Amram O
- Amsler C
- An S
- An Y
- Anagnostou G
- Anampa KH
- Andrea J
- Andreev V
- Andreev Y
- Andrejkovic JW
- Andrews MB
- Androsov K
- Anguiano J
- Antchev G
- Anthony D
- Antonello M
- Antunovic Z
- Anuar AAB
- Apollinari G
- Apparu D
- Appelt E
- Apresyan A
- Araujo M
- Arbol PMRD
- Arcaro D
- Arcidiacono R
- Argiro S
- Arneodo M
- Aruta C
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Asmuss P
- Assiouras P
- Assran Y
- Atakisi IO
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awais A
- Awan MIM
- Ayala E
- Ayala G
- Aydilek O
- Azarkin M
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babbar J
- Bacchetta N
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Bakshi AS
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Banos LIE
- Bansal S
- Baradia S
- Barbagli G
- Barberis E
- Bardelli G
- Bargassa P
- Baringer P
- Barman S
- Barnes VE
- Barney D
- Baron O
- Barrera CB
- Barrera CO
- Barria P
- Barroso AV
- Bartek R
- Bartosik N
- Bartók M
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baxter S
- Bayatmakou M
- Bean A
- Beauceron S
- Beaudette F
- Becerra DAS
- Bedoya CF
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Belforte S
- Bell KW
- Bellan R
- Bellato M
- Belloni A
- Bellora A
- Belyaev A
- Belyaev A
- Bemden MV
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- Yuldashev BS
- Yumiceva F
- Yusuff I
- Yzquierdo AP-C
- Zabi A
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
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- Zecchinelli AG
- Zeid SA
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- Zghiche A
- Zhang F
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- Zhizhin I
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- Zoi I
- Zolkapli Z
- Zorbakir IS
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- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez 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. [Authors’ 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 (tt¯
) 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 138fb−1
. The differential tt¯
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
Recommended from our members
Search for light Higgs bosons from supersymmetric cascade decays in pp collisions at √s=13TeV
- Author
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- Álvarez CR
- Özçelik Ö
- 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 √s = 13TeV and corresponding to an integrated lumi
nosity of 138fb−1 is used. The search targets events where
both H1 bosons decay into b¯b 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 “singlino” 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 b¯b branching
fraction of the H1 in a benchmark model containing almost
mass-degenerategluinosandlight-flavoursquarks.Underthe
assumption of an SM-like H1 → b¯b branching fraction, H1
bosonswithmassesintherange40–120GeVarisingfromthe
decays of squarks or gluinos with a mass of 1200–2500GeV
are excluded at 95% confidence level.SCOA
Recommended from our members
Measurements of Higgs boson production in the decay channel with a pair of τ leptons in proton-proton collisions at s = 13 TeV
- Author
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- Abbaneo D
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- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 19/10/2022
- Field of study
A preprint version of the article is available at arXiv:2204.12957v2 [hep-ex], https://arxiv.org/abs/2204.12957v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables, including additional supplementary figures and tables, can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-19-010 (CMS Public Pages). Report number: CMS-HIG-19-010, CERN-EP-2022-027.Measurements of Higgs boson production, where the Higgs boson decays into a pair of τ leptons, are presented, using a sample of proton-proton collisions collected with the CMS experiment at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb^{−1}. Three analyses are presented. Two are targeting Higgs boson production via gluon fusion and vector boson fusion: a neural network based analysis and an analysis based on an event categorization optimized on the ratio of signal over background events. These are complemented by an analysis targeting vector boson associated Higgs boson production. Results are presented in the form of signal strengths relative to the standard model predictions and products of cross sections and branching fraction to τ leptons, in up to 16 different kinematic regions. For the simultaneous measurements of the neural network based analysis and the analysis targeting vector boson associated Higgs boson production signal strengths are found to be 0.82 ± 0.11 for inclusive Higgs boson production, 0.67 ± 0.19 (0.81 ± 0.17) for the production mainly via gluon fusion (vector boson fusion), and 1.79 ± 0.45 for vector boson associated Higgs boson production.SCOAP3
X-ray CT and histological imaging of xylem vessels organization in Mimosa pudica
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2019
- Field of study
Mimosa pudica has three distinct specialized organs, namely, pulvinus, secondary pulvinus, and pulvinule, which are respectively controlling the movements of petioles, leaflets, and pinna in response to external stimuli. Water flow is a key factor for such movements, but detailed studies on the organization of the vascular system for water transport in these organs have not been published yet. In this study, organizations of the xylem vessels and morphological features of the pulvinus, the secondary pulvinus, and the pulvinule were experimentally investigated by X-ray computed tomography and histological technique. Results showed that the xylem vessels were circularly distributed in the specialized motile organs and reorganized into distinct vascular bundles at the extremities. The number and the total cross-sectional area of the xylem vessels were increased inside the specialized motile organs. Morphological characteristics obtained in this study provided new insight to understand the functions of the vascular networks in the dynamic movements of M. pudica. Microsc. Res. Tech. 76:1204-1212, 2013. (c) 2013 Wiley Periodicals, Inc.X113Nsciescopu
Supersymmetric Multiphonon Structure
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/1996
- Field of study
A multiphonon structure, which is known to exist in boson systems [e.g., the U(5) and O(6) limits of the interacting boson model], is shown to arise also in a mixed system of bosons and fermions. This is illustrated with the example of the Spin(6) limit of U( 6|4) in which a j = 3 / 2 fermion is coupled to an O(6) boson core. All states in the supersymmetric multiplet of U( 6|4) are shown to be multiphonon states obtained by multiple action of a quadrupole operator
- …