206 research outputs found
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
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- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
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- Yeo BK
- Yexley MR
- Yin P
- Yorita K
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- Young CJS
- Yu C
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- Yuan R
- Yue L
- Zaazoua M
- Zabinski B
- Zaid E
- Zak ZK
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
- Zhai M
- Zhang DF
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- Zhang J
- Zhang K
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- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
The Effects of Arsenic Exposure on Neurological and Cognitive Dysfunction in Human and Rodent Studies: A Review
- Author
- A Rai
- A Roy
- AA Cronican
- AD Kligerman
- AG Milton
- AK Patlolla
- AK Whitbread
- B Sharma
- BI Giasson
- BK Ahir
- C Anacker
- C Anacker
- C Drews-Botsch
- C Klein
- CM Aelion
- CM George
- CR Tyler
- D Li
- D Rocha-Amador
- D Sen
- D Wilson
- DC Koestler
- DK Harkins
- DN Gandhi
- EH Syed
- EJ Martinez
- EJ Martinez-Finley
- EJ Martinez-Finley
- EJ Mufson
- F Franco-Marina
- F Tofail
- G Gong
- G Gong
- GA Wasserman
- GA Wasserman
- GA Wasserman
- GA Wasserman
- GM Hong
- H Garelick
- H Zeng
- I Kim
- J Beard
- J Calderon
- J Dong
- J Jing
- J Kang
- J Luo
- J Ventura-Lima
- JA Gosse
- JC Davey
- JD Hamadani
- JD Hamadani
- JE Bodwell
- JE Bodwell
- JE Heck
- JE Heck
- JF Reichard
- JF Reichard
- JG Ortiz
- JH Luo
- JH Luo
- JL Rosado
- JX Guo
- K Jomova
- K Kruger
- K Kruger
- KA Bailey
- KM Zierold
- L Martinez
- LA Baldissarelli
- LC Sanchez-Pena
- M Ahmad
- M Ram Kumar
- M Rodriguez-Barranco
- M Rosselli
- M Vahter
- MF Hughes
- MF Naujokas
- ML Kile
- MR Castro de
- N Govindarajan
- OS Ehrenstein von
- P Dominguez-Salas
- RM Gardner
- RO Wright
- RP Parajuli
- RS Yadav
- RS Yadav
- RS Yadav
- S Ahmed
- S Kaler
- S Liu
- S Llop
- S McDermott
- S Mondal
- S Piacentini
- S Roy
- S Zarazua
- S Zarazua
- SE O'Bryant
- SJ Flora
- SL Goggin
- SX Wang
- SY Tsai
- T Watanabe
- TN Nagaraja
- U Bardullas
- VM Rodriguez
- VM Rodriguez
- W He
- WJ Seow
- WM Dang
- X Liu
- X Wang
- X Zhou
- X Zhou
- X Zhou
- Y Chervona
- Y Fujino
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb−1 of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si157.svg"><mml:mrow><mml:msqrt><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msqrt><mml:mo linebreak="goodbreak" linebreakstyle="after">=</mml:mo><mml:mn>13</mml:mn></mml:mrow></mml:math> TeV pp collision data
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
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- Addepalli SV
- Addison MJ
- Adelman J
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- Ambler A
- Amelung C
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- Zenger DT
- Zenin O
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- Zerwas D
- Zhai M
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- Zhang J
- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
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- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
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- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Elsevier BV
- Publication date
- 01/07/2024
- Field of study
Results from a wide range of searches targeting different experimental signatures with and without missing transverse momentum (
) are used to constrain a Two–Higgs-Doublet Model (2HDM) with an additional pseudo-scalar mediating the interaction between ordinary and dark matter (2HDM + a). The analyses use up to 139 fb−1 of proton–proton collision data at a centre-of-mass energy
TeV recorded with the ATLAS detector at the Large Hadron Collider during 2015–2018. The results from three of the most sensitive searches are combined statistically. These searches target signatures with large
and a leptonically decaying Z boson; large
and a Higgs boson decaying to bottom quarks; and production of charged Higgs bosons in final states with top and bottom quarks, respectively. Constraints are derived for several common and new benchmark scenarios in the 2HDM + a
Search for dark photons in rare Z boson decays with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
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- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi A
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- Ali B
- Ali HMJ
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- Allaire C
- Allbrooke BMM
- Allen JF
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amor Dos Santos SP
- Amos KR
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
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- ATLAS Collaboration
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- Camerlingo MT
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- Dawson I
- Day-Hall HA
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- De Carvalho AL Moreira
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- Yamauchi H
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- Yao W-M
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- Yeo BK
- Yexley MR
- Yildiz H Duran
- Yin P
- Yorita K
- Younas S
- Young C
- Young CJS
- Yu Y
- Yuan M
- Yuan R
- Yue L
- Zaazoua M
- Zabinski B
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
- Zhang DF
- Zhang J
- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2023
- Field of study
A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the standard model
Z
boson is presented, using
139
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon’s coupling to the dark Higgs boson times the kinetic mixing between the standard model photon and the dark photon,
α
D
ϵ
2
, in the dark photon mass range of [5, 40] GeV except for the
Υ
mass window [8.8, 11.1] GeV. This search explores new parameter space not previously excluded by other experiments
Combined measurement of the Higgs boson mass from the H → γγ and H → ZZ∗ → 4ℓ decay channels with the ATLAS detector using √s = 7, 8, and 13 TeV pp collision data
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi F
- Algren M
- Alhroob M
- Ali B
- Ali HMJ
- Ali S
- Alibocus SW
- Aliev M
- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allen JF
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amor Dos Santos SP
- Amos KR
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
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- Tapia Araya S
- Tapprogge S
- Tarek Abouelfadl Mohamed A
- Tarem S
- Tariq K
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tassi E
- Tate AC
- Tateno G
- Tayalati Y
- Taylor GN
- Taylor W
- Tee AS
- Teixeira De Lima R
- Teixeira-Dias P
- Teoh JJ
- Terashi K
- Terron J
- Terzo S
- Testa M
- Teuscher RJ
- Thaler A
- Theiner O
- Themistokleous N
- Theveneaux-Pelzer T
- Thielmann O
- Thomas DW
- Thomas JP
- Thompson EA
- Thompson PD
- Thomson E
- Tian Y
- Tikhomirov V
- Tikhonov Yu A
- Timoshenko S
- Timoshyn D
- Ting EXL
- Tipton P
- Tlou SH
- Tnourji A
- Todome K
- Todorova-Nova S
- Todt S
- Togawa M
- Tojo J
- Tokushuku K
- Tokár S
- Toldaiev O
- Tombs R
- Tomoto M
- Tompkins L
- Topolnicki KW
- Torrence E
- Torres H
- Torró Pastor E
- Toscani M
- Tosciri C
- Tost M
- Tovey DR
- Traeet A
- Trandafir IS
- Trefzger T
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Trischuk DA
- Trocmé B
- Troncon C
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tsai M
- Tsiamis A
- Tsiareshka PV
- Tsigaridas S
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsujikawa Y
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsur O
- Tsuri K
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna AN
- Turchikhin S
- Turk Cakir I
- Turra R
- Turtuvshin T
- Tuts PM
- Tzamarias S
- Tzanis P
- Tzovara E
- Ukegawa F
- Ulloa Poblete PA
- Umaka EN
- Unal G
- Unal M
- Undrus A
- Unel G
- Urban J
- Urquijo P
- Urrejola P
- Usai G
- Ushioda R
- Usman M
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vafeiadis T
- Vaitkus A
- Valderanis C
- Valdes Santurio E
- Vale T Dias Do
- Valente M
- Valentinetti S
- Valero A
- Valiente Moreno E
- Vallier A
- Valls Ferrer JA
- Van Arneman DR
- Van Daalen TR
- Van Der Graaf A
- Van Gemmeren P
- Van Rijnbach M
- Van Stroud S
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vannicola D
- Vannoli L
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varriale L
- Varvell KE
- Vasile ME
- Vaslin L
- Vasquez GA
- Vasyukov A
- Vazeille F
- Vazquez Schroeder T
- Veatch J
- Vecchio V
- Veen MJ
- Veliscek I
- Veloce LM
- Veloso F
- Veneziano S
- Ventura Gonzalez S
- Ventura A
- Verbytskyi A
- Verducci M
- Vergis C
- Verissimo De Araujo M
- Verkerke W
- Vermeulen JC
- Vernieri C
- Vessella M
- Vetterli MC
- Vgenopoulos A
- Viaux Maira N
- Vickey Boeriu OE
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Villaplana Perez M
- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Visibile A
- Vittori C
- Vivarelli I
- Voevodina E
- Vogel F
- Voigt JC
- Vokac P
- Volkotrub Yu
- Von Ahnen J
- Von Toerne E
- Vormwald B
- Vorobel V
- Vorobev K
- Vos M
- Voss K
- Vossebeld JH
- Vozak M
- Vozdecky L
- Vranjes Milosavljevic M
- Vranjes N
- Vreeswijk M
- Vu NK
- Vuillermet R
- Vujinovic O
- Vukotic I
- Wada S
- Wagner C
- Wagner JM
- Wagner W
- Wahdan S
- Wahlberg H
- Wakida M
- Walder J
- Walker R
- Walkowiak W
- Wall A
- Wamorkar T
- Wang AZ
- Wang C
- Wang C
- Wang H
- Wang J
- Wang R
- Wang R
- Wang R-J
- Wang S
- Wang SM
- Wang T
- Wang W
- Wang WT
- Wang X
- Wang X
- Wang X
- Wang Y
- Wang Y
- Wang Z
- Wang Z
- Wang Z
- Warburton A
- Ward RJ
- Warrack N
- Watson AT
- Watson H
- Watson MF
- Watton E
- Watts G
- Waugh BM
- Weber C
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- Weber MS
- Weber SM
- Wei C
- Wei Y
- Weidberg AR
- Weik EJ
- Weingarten J
- Weirich M
- Weiser C
- Wells CJ
- Wenaus T
- Wendland B
- Wengler T
- Wenke NS
- Wermes N
- Wessels M
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Wickremasinghe L
- Wiedenmann W
- Wiel C
- Wielers M
- Wiglesworth C
- Wilbern DJ
- Wilkens HG
- Williams DM
- Williams HH
- Williams S
- Willocq S
- Wilson BJ
- Windischhofer PJ
- Winkel FI
- Winklmeier F
- Winter BT
- Winter JK
- Wittgen M
- Wobisch M
- Wolffs Z
- Wollrath J
- Wolter MW
- Wolters H
- Wongel AF
- Woodward EL
- Worm SD
- Wosiek BK
- Wozniewski S
- Woźniak KW
- Wraight K
- Wu C
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- Wu M
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wu Z
- Wuerzinger J
- Wyatt TR
- Wynne BM
- Xella S
- Xia L
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- Xiang J
- Xie M
- Xie X
- Xin S
- Xiong A
- Xiong J
- Xu D
- Xu H
- Xu L
- Xu R
- Xu T
- Xu Y
- Xu Z
- Yabsley B
- Yacoob S
- Yamaguchi Y
- Yamashita E
- Yamauchi H
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- Yan J
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- Yang Z
- Yao W-M
- Yap YC
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- Ye S
- Ye X
- Yeh Y
- Yeletskikh I
- Yeo BK
- Yexley MR
- Yin P
- Yorita K
- Younas S
- Young C
- Young CJS
- Yu C
- Yu Y
- Yuan M
- Yuan R
- Yue L
- Zaazoua M
- Zabinski B
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
- Zhang DF
- Zhang J
- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2023
- Field of study
A measurement of the mass of the Higgs boson combining the
H
→
Z
Z
∗
→
4
ℓ
and
H
→
γ
γ
decay channels is presented. The result is based on
140
fb
−
1
of proton-proton collision data collected by the ATLAS detector during LHC run 2 at a center-of-mass energy of 13 TeV combined with the run 1 ATLAS mass measurement, performed at center-of-mass energies of 7 and 8 TeV, yielding a Higgs boson mass of
125.11
±
0.09
(
stat
)
±
0.06
(
syst
)
=
125.11
±
0.11
GeV
. This corresponds to a 0.09% precision achieved on this fundamental parameter of the Standard Model of particle physics
Effects of Functional Fitness Enhancement through Taekwondo Training on Physical Characteristics and Risk Factors of Dementia in Elderly Women with Depression
- Publication venue
- 'MDPI AG'
- Publication date
- 01/07/2021
- Field of study
The purpose of this research is to identify the correlations between functional fitness enhancement through a long-term Taekwondo training program and the physical characteristics and risk factors of dementia among elderly women with depression. The study has found that conducting three 60-min Taekwondo training sessions a week for the duration of 12 weeks has enhanced a number of functional fitness indexes, including hand grip strength/weight (p < 0.01), 4-m gait speed (p < 0.001), 3-m timed up and go (p < 0.05), and figure-of-eight track (p < 0.05), and significantly improved general health condition indexes as well, including percent fat (p < 0.05), appendicular skeletal muscle mass index (p < 0.01), systolic blood pressure (p < 0.01), and diastolic blood pressure (p < 0.001). Furthermore, the arteriosclerosis index and cognitive function have been found to be improved with an increase of brain-derived neurotrophic factor (BDNF; which prevents dementia) and a significant decrease of β-amyloid—a risk factor of dementia—as a result of enhancements in serum lipids and adiponectin, confirming the positive effects of functional fitness enhancement on fighting depression, promoting physical characteristics, and reducing the risk factors of dementia
Ameliorating Effect of Dietary Xylitol on Human Respiratory Syncytial Virus (hRSV) Infection
- Publication venue
- 'Pharmaceutical Society of Japan'
- Publication date
- 01/01/2016
- Field of study
Seasonal and altitudinal variation in roe deer (Capreolus pygargus tianschanicus) diet on Jeju Island, South Korea
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/12/2016
- Field of study
In order to understand the feeding ecology and dietary differences of roe deer (Capreolus pygargus tianschanicus) in different seasons and altitudes, this study was carried out at three altitudinal sites (Songdang 250–270 m above sea level (ASL), Aradong 330–370 m ASL, Mt. Hallasan 1100 m ASL) on Jeju Island, South Korea. Altogether, 205 plants taxa of six categories of foods (forbs-climbers, graminoids, trees, shrubs, conifers, and ferns) were identified using morphological and molecular analyses. The highest number of dietary plants was found in summer (93 taxa) and at Aradong (124 taxa) and lowest at Songdang (71 taxa) and in winter (51 taxa). Food categories were significantly different among the seasons (F = 15.646, p < 0.05) and altitudinal sites (F = 3.941, p < 0.05). This study revealed that dietary selectivity of roe deer shifted with seasonal and altitudinal variations and preferred to the nutritive and low fibers food
The Effect of Precursor Concentration on the Crystallite Size of CeO<sub>2</sub> to Enhance the Sulfur Resistance of Pt/CeO<sub>2</sub> for Water Gas Shift
- Author
- Publication venue
- MDPI AG
- Publication date
- 01/01/2024
- Field of study
To develop customized sulfur–resistant catalysts for the water gas shift (WGS) reaction in the waste–to–hydrogen process, the effects of changing the nucleation conditions of the CeO2 support on catalytic performance were investigated. Supersaturation is a critical kinetic parameter for nuclei formation. The degree of supersaturation of the CeO2 precipitation solution was controlled by varying the cerium precursor concentration from 0.02 to 0.20 M. Next, 2 wt.% of Pt was impregnated on those various CeO2 supports by the incipient wetness impregnation method. The prepared samples were then evaluated in a WGS reaction using waste–derived synthesis gas containing 500 ppm H2S. The Pt catalyst supported by CeO2 prepared at the highest precursor concentration of 0.20 M exhibited the best sulfur resistance and catalytic activity regeneration. The sulfur tolerance of the catalyst demonstrated a close correlation with its oxygen storage capacity and easier reducibility. The formation of oxygen vacancies in CeO2 supports is promoted by the formation of small crystals due to a high degree of supersaturation
- …