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29 research outputs found

The Generation of Flood Damage Time Sequences

Author: Breaden John P.
Publication venue: UKnowledge
Publication date: 01/01/1971
Field of study

There is a need in water resources planning to develop a procedure for determining the time pattern in which flood damages occur as a function of the rise and fall of the flood hydrograph. The widely-used approach for estimation of flood damages does not take into account the fact that the frequency of the annual flood peak may not be the same as the frequency of the total annual flood damages. As examples, several small storms during the year may do more damage than a single larger storm, or flood damages may be reduced by a reduction in flood duration rather than the flood peaks. This report presents a digital computer subroutine DAMAGE which can be used to estimate the direct and indirect damages to property in the four basic categories of crop, field, urban, and public facilities as functions of the depth and duration of flooding, seasons, and the time laps between flood events. DAMAGE may be called with recorded or simulated annual hydrographs and used to analyze the time pattern of damages in the flood plain for optimizing the policies for operating reservoir flood control storage or for estimating the average annual damages for use in formulation of alternative flood control schemes

University of Kentucky

A Perspective on Economic Impact

Author: Bates Clyde T.
Bianchi Dennis H.
Breaden John P.
Dowell Charles O.
Fulmer John L.
Hargrove Michael B.
Harman Kenneth R.
Higgins John M.
Holbrook Kenneth G.
James L. Douglas
Prebble Billy R.
Redman John C.
Rosenbaum David H.
Sirles John E.
Soule Donald M.
Thompson William O.
Tussey Robert C.
Vaughan Claude M.
Publication venue: UKnowledge
Publication date: 01/03/1972
Field of study

The institutions responsible for water resources management in the United States have originated as political responses to major social issues. Each agency institutionalized a procedure for structuring and comparing alternatives in the formulation of its total program. Each agency originally sought to promote effective resolution of its social issue (flood control, development of arid lands, soil erosion, etc.), but more recent efforts have sought better coordination among agency practices through a common procedure largely derived from economic theory. Any procedure, however, varies in application with the interpretation and judgment of individual planners. Today, public pressures have brought political directives requiring consideration of the local and nationwide impacts of projects that occur through direct, indirect, and secondary means in the spheres of economic, social and environmental effects. The body of the study reviews fourteen specific impact issues with the goals of providing planners a methodology for dealing with each one and of providing the theoretically inclined a basis for improving each methodology. The issues are reservoir effects on local property values, reservoir effects on the economy of the local county, changes in income and employment patterns around large reservoirs, patterns of land use change around reservoirs, reservoir effects on revenues and expenditures of local government, reservoir recreation benefits, application of marginal economic analysis to reservoir recreation planning, economic value of natural areas for recreational hunting, for stream fishing, the personal value of real property to its owner, reservoir project caused income redistribution, achievement of more flexible procedures for reservoir operation in order to match changes in demand for project output with time, estimation of flood damages by the time pattern in which they occur, and operation of reservoir systems for flood control. Each study ls presented in detail in a referenced report, and this report discusses the significance of the findings of the studies, individually and as a group

University of Kentucky

Combinations of single-top-quark production cross-section measurements and vertical bar f(LV)V(tb)vertical bar determinations at root s=7 and 8 TeV with the ATLAS and CMS experiments

Author: Aaboud Morad
Aad G.
Abbott B.
Abbott D. C.
Abdinov O.
Abed Abud A.
Abhayasinghe D. K.
Abidi S. H.
AbouZeid O. S.
Abraham N. L.
Abramowicz H.
Abreu H.
Abulaiti Y.
Acharya B. S.
Adachi S.
Adam L.
Adamczyk L.
Adamek L.
Adelman J.
Adersberger M.
Adiguzel A.
Adorni S.
Adye T.
Affolder A. A.
Afik Y.
Agapopoulou C.
Agaras M. N.
Aggarwal A.
Agheorghiesei C.
Aguilar-Saavedra Juan Antonio
Ahmadov F.
Ai X.
Aielli G.
Akatsuka S.
Akilli E.
Akimov A. V.
Al Khoury K.
Alberghi G. L.
Albert J.
Alconada Verzini M. J.
Alderweireldt S.
Aleksa M.
Aleksandrov I. N.
Alexa C.
Alexandre D.
Alexopoulos T.
Alfonsi A.
Alhroob M.
Ali B.
Alimonti G.
Alison J.
Alkire S. P.
Allaire C.
Allbrooke B. M. M.
Allen B. W.
Allport P. P.
Aloisio A.
Alonso A.
Alonso F.
Alpigiani C.
Alshehri A. A.
Alstaty M. I.
Alvarez Estevez M.
Alvarez Gonzalez B.
Alviggi M. G.
Amaral Coutinho Y.
Ambler A.
Ambroz L.
Amelung C.
Amidei D.
Amor Dos Santos S. P.
Amoroso S.
Amrouche C. S.
An F.
Anastopoulos C.
Andari N.
Andeen T.
Anders C. F.
Anders J. K.
Andreazza A.
Andrei V.
Anelli C. R.
Angelidakis S.
Angelozzi I.
Angerami A.
Anisenkov A. V.
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Anthony M. T.
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Aparisi Pozo J. A.
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Arabidze G.
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Argyropoulos S.
Arling J. H.
Armbruster A. J.
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Armstrong A.
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Avolio G.
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Ayoub M. K.
Azoulay A. M.
Azuelos Georges
Baas A. E.
Baca Matthew John
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Publication venue
Publication date: 01/01/2019
Field of study

This paper presents the combinations of single-top-quark production cross-section measurements by the ATLAS and CMS Collaborations, using data from LHC proton-proton collisions at = 7 and 8 TeV corresponding to integrated luminosities of 1.17 to 5.1 fb(-1) at = 7 TeV and 12.2 to 20.3 fb(-1) at = 8 TeV. These combinations are performed per centre-of-mass energy and for each production mode: t-channel, tW, and s-channel. The combined t-channel cross-sections are 67.5 +/- 5.7 pb and 87.7 +/- 5.8 pb at = 7 and 8 TeV respectively. The combined tW cross-sections are 16.3 +/- 4.1 pb and 23.1 +/- 3.6 pb at = 7 and 8 TeV respectively. For the s-channel cross-section, the combination yields 4.9 +/- 1.4 pb at = 8 TeV. The square of the magnitude of the CKM matrix element V-tb multiplied by a form factor f(LV) is determined for each production mode and centre-of-mass energy, using the ratio of the measured cross-section to its theoretical prediction. It is assumed that the top-quark-related CKM matrix elements obey the relation |V-td|, |V-ts| << |V-tb|. All the |f(LV)V(tb)|(2) determinations, extracted from individual ratios at = 7 and 8 TeV, are combined, resulting in |f(LV)V(tb)| = 1.02 +/- 0.04 (meas.) +/- 0.02 (theo.). All combined measurements are consistent with their corresponding Standard Model predictions.Peer reviewe

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The ATLAS inner detector trigger performance in pp collisions at 13 TeV during LHC Run 2

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Abbott B
Abbott DC
Abeling K
Abhayasinghe DK
Abidi SH
AbouZeid OS
Abraham NL
Abramowicz H
Abreu H
Abud A Abed
Abulaiti Y
Acharya BS
Achkar B
Adam L
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Adamek L
Adelman J
Adiguzel A
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Agaras MN
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Allbrooke BMM
Allport PP
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Amelung C
Amidei D
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Gonzalez-Sevilla S
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Gorbounov PA
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Gottardo CA
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Hopkins WH
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Traeet A
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Yildiz H Duran
Yin P
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Young C
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Zaffaroni E
Zagazeta LF Gutierrez
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Zeissner SV
Zeitnitz C
Zemaityte G
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Zenin O
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Zerwas D
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Zhang B
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Zhang Y
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Zhao P
Zhao Y
Zhao Z
Zhemchugov A
Zheng Z
Zhong D
Zhou B
Zhou C
Zhou H
Zhou M
Zhou N
Zhou Y
Zhu C
Zhu CG
Zhu H
Zhu HL
Zhu J
Zhu Y
Zhuang X
Zhukov K
Zhulanov V
Zieminska D
Zimine NI
Zimmermann S
Zinonos Z
Ziolkowski M
Zivkovic L
Zoccoli A
Zoch K
Zorbas TG
Zou R
Zou W
Zwalinski L
Publication venue: EUROPEAN PHYSICAL JOURNAL C
Publication date: 08/03/2022
Field of study

The design and performance of the inner detector trigger for the high level trigger of the ATLAS experiment at the Large Hadron Collider during the 2016-18 data taking period is discussed. In 2016, 2017, and 2018 the ATLAS detector recorded 35.6 fb

^{-1}

, 46.9 fb

^{-1}

, and 60.6 fb

^{-1}

respectively of proton-proton collision data at a centre-of-mass energy of 13 TeV. In order to deal with the very high interaction multiplicities per bunch crossing expected with the 13 TeV collisions the inner detector trigger was redesigned during the long shutdown of the Large Hadron Collider from 2013 until 2015. An overview of these developments is provided and the performance of the tracking in the trigger for the muon, electron, tau and

b

-jet signatures is discussed. The high performance of the inner detector trigger with these extreme interaction multiplicities demonstrates how the inner detector tracking continues to lie at the heart of the trigger performance and is essential in enabling the ATLAS physics programme

Apollo (Cambridge)

Recommended from our members

Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector

Author: Aad G
Abbott B
Abbott DC
Abeling K
Abhayasinghe DK
Abidi SH
Aboulhorma A
Abramowicz H
Abreu H
Abud A Abed
Abulaiti Y
Acharya BS
Achkar B
Adam L
Adamczyk L
Adamek L
Addepalli SV
Adelman J
Adiguzel A
Adorni S
Adye T
Affolder AA
Afik Y
Agapopoulou C
Agaras MN
Agarwala J
Aggarwal A
Agheorghiesei C
Aguilar-Saavedra JA
Agullo P Martinez
Ahmad A
Ahmadov F
Ahmed WS
Ai X
Aielli G
Aizenberg I
Akatsuka S
Akbiyik M
Akesson TPA
Akimov AV
Al Khoury K
Alberghi GL
Albert J
Albicocco P
Alderweireldt S
Aleksa M
Aleksandrov IN
Alexa C
Alexopoulos T
Alfonsi A
Alfonsi F
Alhroob M
Ali B
Ali S
Aliev M
Alimonti G
Allaire C
Allbrooke BMM
Allport PP
Aloisio A
Alonso F
Alpigiani C
Alves FL Lucio
Alviggi MG
Ambler A
Ambroz L
Amelung C
Amidei D
Amoroso S
Amrouche CS
Anastopoulos C
Andana RY Gonzalez
Andari N
Andeen T
Anders JK
Andrean SY
Andreazza A
Angelidakis S
Angerami A
Anisenkov AV
Annovi A
Antel C
Anthony MT
Antipov E
Antonelli M
Antrim DJA
Anulli F
Aoki M
Aparo MA
Aranda C Padilla
Aranzabal N
Araya S Tapia
Arcangeletti C
Arce ATH
Arena E
Arguin J-F
Argyropoulos S
Arling J-H
Armbruster AJ
Armstrong A
Arnaez O
Arnold H
Artoni G
Asada H
Asai K
Asai S
Asbah NA
Asimakopoulou EM
Asquith L
Assahsah J
Assamagan K
Astalos R
Astigarraga ME Pozo
Atkin RJ
Atkinson M
Atlay NB
Atmani H
Atmasiddha PA
Augsten K
Auricchio S
Austrup VA
Avner G
Avolio G
Ayoub MK
Azuelos G
Babal D
Bachacou H
Bachas K
Bachiu A
Backman F
Badea A
Bagnaia P
Bahilo JJ Lozano
Bahrasemani H
Bailey AJ
Bailey VR
Baines JT
Bakalis C
Baker OK
Bakker PJ
Bakos E
Balaji S
Balasubramanian R
Baldin EM
Balek P
Ballabene E
Balli F
Balunas WK
Balz J
Banas E
Bandieramonte M
Bandyopadhyay A
Bansal S
Barak L
Barberio EL
Barberis D
Barbero M
Barbour G
Barends KN
Barillari T
Barisits M-S
Barkeloo J
Barklow T
Barnett BM
Barnett RM
Baroncelli A
Barone G
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Barreiro F
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Bartoldus R
Bartolini G
Barton AE
Bartos P
Basalaev A
Basan A
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Bashta I
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Basso MJ
Basson CR
Bates RL
Batlamous S
Batley John
Batool B
Battaglia M
Bauce M
Bauer F
Bauer P
Bawa HS
Bayirli A
Beacham JB
Beau T
Beauchemin PH
Becherer F
Bechtle P
Beck HP
Becker K
Becot C
Beddall AJ
Bednyakov VA
Bee CP
Beermann TA
Begalli M
Begel M
Behera A
Behr JK
Beirer JF
Beisiegel F
Belfkir M
Bella G
Bella L Aperio
Bellagamba L
Bellerive A
Bellos P
Beloborodov K
Belotskiy K
Belyaev NL
Benchekroun D
Benhammou Y
Benjamin DP
Benoit M
Bensinger JR
Bentvelsen S
Beresford L
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Berge D
Berger N
Bergmann B
Bergsten LJ
Beringer J
Berlendis S
Berlingen J Montejo
Bernardi G
Bernius C
Bernlochner FU
Berry T
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Berthold A
Bertram IA
Bethke S
Betti A
Bevan AJ
Bhatta S
Bhattacharya DS
Bhattarai P
Bhopatkar VS
Bi R
Bianchi RM
Biebel O
Bielski R
Biesuz NV
Biglietti M
Billoud TRV
Bindi M
Bingul A
Bini C
Biondi S
Biondini A
Birch-sykes CJ
Bird GA
Birman M
Bisanz T
Biswal JP
Biswas D
Bitadze A
Bittrich C
Bjorke K
Bloch I
Blocker C
Blue A
Blumenschein U
Blumenthal J
Bobbink GJ
Bobrovnikov VS
Boehler M
Boeriu OE Vickey
Bogavac D
Bogdanchikov AG
Bohm C
Boisvert V
Bokan P
Bolanos G Rabanal
Bold T
Bomben M
Bona M
Boonekamp M
Booth CD
Borbely AG
Borecka-Bielska HM
Borgna LS
Borissov G
Bortoletto D
Bosca S Rodriguez
Boscherini D
Bosman M
Bostanabad M Ghasemi
Bouaouda K
Boudreau J
Bouhova-Thacker EV
Boumediene D
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Bourdarios C Adam
Boveia A
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Boyko IR
Bozson AJ
Bracinik J
Brahimi N
Brandt G
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Braren F
Brau B
Brau JE
Brendlinger K
Brener R
Brenner L
Brenner R
Bressler S
Bret M Cano
Brickwedde B
Briglin DL
Britton D
Britzger D
Brock I
Brock R
Brooijmans G
Brooks WK
Brost E
Bruers B
Bruncko D
Bruni A
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Bruschi M
Bruscino N
Bryngemark L
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Buchholz P
Buckley AG
Budagov IA
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Bullard BA
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Burgard CD
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Burr Jon
Burton CD
Burzynski JC
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Bussey PJ
Butler JM
Buttar CM
Butterworth JM
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Bylund O Bessidskaia
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Caforio D
Cai H
Cairo VMM
Cakir I Turk
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Calafiura P
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Caloba LP
Calvet D
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Calvet TP
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Collaboration ATLAS
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De Vivie De Regie JB
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Publication venue: EUROPEAN PHYSICAL JOURNAL C
Publication date: 03/02/2022
Field of study

This paper presents the measurement of the electroweak production of two jets in association with a

Z\gamma

pair with the

Z

boson decaying into two neutrinos. It also presents the search for invisible or partially invisible decays of a Higgs boson with a mass of 125 GeV produced through vector-boson fusion with a photon in the final state. These results use data from LHC proton-proton collisions at

\sqrt{s}

= 13 TeV collected with the ATLAS detector corresponding to an integrated luminosity of 139 fb

^{-1}

. The event signature, shared by all benchmark processes considered for measurements and searches, is characterized by a significant amount of unbalanced transverse momentum and a photon in the final state, in addition to a pair of forward jets. For electroweak production of

Z\gamma

in association with two jets, the background-only hypothesis is rejected with an observed (expected) significance of 5.2 (5.1) standard deviations. The measured fiducial cross-section for this process is 1.31

\pm

0.29 fb. Observed (expected) upper limit of 0.37 (0.34) at 95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to invisible particles, assuming the Standard Model production cross-section. The signature is also interpreted in the context of decays of a Higgs boson to a photon and a dark photon. An observed (expected) 95% CL upper limit on the branching ratio for this decay is set at 0.018 (0.017), assuming the 125 GeV Standard Model Higgs boson production cross-section

Apollo (Cambridge)