18 research outputs found
Modelling Z → ττ processes in ATLAS with τ-embedded Z → μμ data
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
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- Altheimer A
- Alviggi G
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
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- Anders JK
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- Angelidakis S
- Angelozzi I
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- Angerami A
- Anghinolfi F
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- Antonelli M
- Antonov A
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- Aoki M
- Arabidze G
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- Argyropoulos S
- Arika M
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- Armbruster AJ
- Arnaez O
- Arnal V
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Aurousseau M
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
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- Bachacou H
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- Backes M
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- Bai Y
- Bain T
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- Budagov IA
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- Burckhart H
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- Burghgrave B
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- Burmeister I
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- Butterworth JM
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- Buttinger W
- Buzatu A
- Buzykaev AR
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- Caforio D
- Cairo VM
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- Caloba LP
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- Castanheira MTD
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- Chekulaev SV
- Chelkov GA
- Chelstowska MA
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- Chernyatin V
- Cheu E
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- Chiarella V
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- Childers JT
- Chiodini G
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Choi K
- Chouridou S
- Chow BKB
- Christodoulou V
- Chromek-Burckhart D
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Ciapetti G
- Ciftci AK
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Citron ZH
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- Deviveiros PO
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- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2015
- Field of study
This paper describes the concept, technical realisation and validation of a largely data-driven method to model events with Z→ττ decays. In Z→μμ events selected from proton-proton collision data recorded at √s=8 TeV with the ATLAS experiment at the LHC in 2012, the Z decay muons are replaced by τ leptons from simulated Z→ττ decays at the level of reconstructed tracks and calorimeter cells. The τ lepton kinematics are derived from the kinematics of the original muons. Thus, only the well-understood decays of the Z boson and τ leptons as well as the detector response to the τ decay products are obtained from simulation. All other aspects of the event, such as the Z boson and jet kinematics as well as effects from multiple interactions, are given by the actual data. This so-called τ-embedding method is particularly relevant for Higgs boson searches and analyses in ττ final states, where Zarrowττ decays constitute a large irreducible background that cannot be obtained directly from data control samples. In this paper, the relevant concepts are discussed based on the implementation used in the ATLAS Standard Model H→ττ analysis of the full datataset recorded during 2011 and 2012
Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector
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- Zieminska
- Zimine NI
- Zimmermann C
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
The rejection of forward jets originating from
additional proton–proton interactions (pile-up) is crucial for
a variety of physics analyses at the LHC, including Standard
Model measurements and searches for physics beyond
the Standard Model. The identification of such jets is challenging
due to the lack of track and vertex information in
the pseudorapidity range |η| > 2.5. This paper presents a
novel strategy for forward pile-up jet tagging that exploits
jet shapes and topological jet correlations in pile-up interactions.
Measurements of the per-jet tagging efficiency are
presented using a data set of 3.2 fb−1 of proton–proton collisions
at a centre-of-mass energy of 13 TeV collected with the
ATLAS detector. The fraction of pile-up jets rejected in the
range 2.5 < |η| < 4.5 is estimated in simulated events with
an average of 22 interactions per bunch-crossing. It increases
with jet transverse momentum and, for jets with transverse
momentum between 20 and 50 GeV, it ranges between 49%
and 67% with an efficiency of 85% for selecting hard-scatter
jets. A case study is performed in Higgs boson production
via the vector-boson fusion process, showing that these techniques
mitigate the background growth due to additional
proton–proton interactions, thus enhancing the reach for such
signatures
Measurement of differential cross sections of isolated-photon plus heavy-flavour jet production in pp collisions at √s=8 TeV using the ATLAS detector
- Author
- Aaboudd M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
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- Acharya BS
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- Wang Q
- Wang R
- Wang R-J
- Wang SM
- Wang T
- Wang W
- Wang W
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Washbrook A
- Watkins PM
- Watson AT
- Watson MF
- Watts G
- Watts S
- Waugh BM
- Webb AF
- Webb S
- Weber MS
- Weber SA
- Weber SM
- Weber SW
- Webster JS
- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Werner P
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong KHY
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wotschack J
- Wozniak KW
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu L
- Xu T
- Xu W
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 10/01/2018
- Field of study
This Letter presents the measurement of differential cross sections of isolated prompt photons produced
in association with a b-jet or a c-jet. These final states provide sensitivity to the heavy-flavour content
of the proton and aspects related to the modelling of heavy-flavour quarks in perturbative QCD. The
measurement uses proton–proton collision data at a centre-of-mass energy of 8 TeV recorded by the
ATLAS detector at the LHC in 2012 corresponding to an integrated luminosity of up to 20.2 fb−1. The
differential cross sections are measured for each jet flavour with respect to the transverse energy of
the leading photon in two photon pseudorapidity regions: |ηγ | < 1.37 and 1.56 < |ηγ | < 2.37. The
measurement covers photon transverse energies 25 < Eγ
T < 400 GeV and 25 < Eγ
T < 350 GeV respectively
for the two |ηγ | regions. For each jet flavour, the ratio of the cross sections in the two |ηγ | regions is also
measured. The measurement is corrected for detector effects and compared to leading-order and nextto-leading-order
perturbative QCD calculations, based on various treatments and assumptions about the
heavy-flavour content of the proton. Overall, the predictions agree well with the measurement, but some
deviations are observed at high photon transverse energies. The total uncertainty in the measurement
ranges between 13% and 66%, while the central γ + b measurement exhibits the smallest uncertainty,
ranging from 13% to 27%, which is comparable to the precision of the theoretical predictions
Observation of Vertically Ejected Plumes Generated by the Impact of Hollow Projectiles at Various Velocities
- Author
- Publication venue
- IOP Publishing
- Publication date
- 01/01/2023
- Field of study
Recently, impact experiments in space have been conducted in planetary exploration using hollow or internally structured projectiles. In laboratory experiments using hollow projectiles to investigate the differences in crater and ejecta from the case of solid projectiles, a plume perpendicular to the target surface has been observed, which has not been seen in conventional cratering experiments using solid projectiles. In this study, we conducted crater-formation experiments using hollow resin projectiles to understand the mechanism through which vertical plumes form in the case of hollow projectiles. We examined the generation of a vertical plume as a function of the impact velocity, v _imp . We found that (i) no vertical plume occurs at v _imp < 200 m s ^−1 , (ii) the cases with or without a vertical plume are mixed at 200 < v _imp < 350 m s ^−1 , (iii) no vertical plume occurs at 350 < v _imp < 800 m s ^−1 , and (iv) a vertical plume occurs at 2 < v _imp < 3 km s ^−1 . We qualitatively discussed the generation mechanism of the vertical plume using the results of recovered projectiles. Depending on v _imp , an empty hole in which there is no projectile materials can be opened along the central axis, resulting in the generation of a vertical plume
Inhibitory Effects of Sizofiran on Anticancer Agent- or X-Ray-induced Sister Chromatid Exchanges and Mitotic Block in Murine Bone Marrow Cells
- Author
- Publication venue
- 'Wiley'
- Publication date
- Field of study
Successful twin pregnancy in a patient with parkin-associated autosomal recessive juvenile parkinsonism
- Author
- Publication venue
- BMC
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Pregnancy in patients with Parkinson disease is a rare occurrence. To the best of our knowledge, the effect of pregnancy as well as treatment in genetically confirmed autosomal recessive juvenile parkinsonism (ARJP) has never been reported. Here, we report the first case of pregnancy in a patient with ARJP associated with a <it>parkin </it>gene mutation, ARJP/PARK2.</p> <p>Case presentation</p> <p>A 27-year-old woman with ARJP/PARK2 was diagnosed as having a spontaneous dichorionic/diamniotic twin pregnancy. Exacerbation of motor disability was noted between ovulation and menstruation before pregnancy as well as during late pregnancy, suggesting that her parkinsonism might have been influenced by fluctuations in the levels of endogenous sex hormones. During the organogenesis period, she was only treated with levodopa/carbidopa, although she continued to receive inpatient hospital care for assistance in the activities of daily living. After the organogenesis period, she was administered sufficient amounts of antiparkinsonian drugs. She delivered healthy male twins, and psychomotor development of both the babies was normal at the age of 2 years.</p> <p>Conclusion</p> <p>Pregnancy may worsen the symptoms of ARJP/PARK2, although appropriate treatments with antiparkinsonian drugs and adequate assistance in the activities of daily living might enable successful pregnancy and birth of healthy children.</p
中空弾丸の衝突によって放出される粉体のパターン
- Author
- Publication venue
- Institute of Space and Astronautical Science, Japan Aerospace Exploration Agency(JAXA)(ISAS)
- Publication date
- 06/02/2023
- Field of study
Explicit-Solvent Molecular Dynamics Simulations of the Polysaccharide Schizophyllan in Water
- Author
- Anada
- Arika
- Barker
- Berendsen
- Buffle
- Chuah
- Coviello
- Coviello
- Coviello
- Damm
- David B. Kony
- Eggensperger
- Enomoto
- Ewald
- Fang
- Filella
- Hasegawa
- Hayashi
- Hirao
- Hockney
- Itou
- Itou
- Jorgensen
- Jorgensen
- Kashiwagi
- Kojima
- Kony
- Kony
- Lins
- Matricardi
- McIntire
- Miyoshi
- Nagai
- Norisuye
- Numata
- Palleschi
- Palleschi
- Philippe H. Hünenberger
- Poland
- Rizzo
- Rodgers
- Ryckaert
- Sakurai
- Sato
- Sato
- Sato
- Scott
- Serge Stoll
- Sletmoen
- Stokke
- Tabata
- Takahashi
- Teramoto
- Teramoto
- Teramoto
- Teramoto
- Van der Valk
- van Gunsteren
- Vickers
- Whistler
- Wilfred F. van Gunsteren
- Wolfgang Damm
- Yanaki
- Yanaki
- Yoshiba
- Zekovic
- Zimm
- Publication venue
- The Biophysical Society
- Publication date
- 15/07/2007
- Field of study
Schizophyllan is a β(1→3)-D-glucan polysaccharide with β(1→6)-branched lateral glucose residues that presents a very stiff triple-helical structure under most experimental conditions. Despite the remarkable stability of this structure (which persists up to 120°C in aqueous solution), schizophyllan undergoes a major change of state around 7°C in water that has been hypothesized to result from an order-disorder transition in the lateral residues. This hypothesis is only supported by indirect experimental evidence and detailed knowledge (at the atomic level) concerning hydrogen-bonding networks, interactions with the solvent molecules, orientational freedom of the lateral residues, and orientational correlations among them is still lacking. In this study explicit-solvent molecular dynamics simulations of a schizophyllan fragment (complemented by simulations of its tetrasaccharide monomer) are performed at three different temperatures (273 K, 350 K, and 450 K) and with two different types of boundary conditions (finite nonperiodic or infinite periodic fragment) as an attempt to provide detailed structural and dynamical information about the triple-helical conformation in solution and the mechanism of the low-temperature transition. These simulations suggest that three important driving forces for the high stability of the triple helix are i), the limited conformational work involved in its formation; ii), the formation of a dense hydrogen-bonding network at its center; and iii), the formation of interchain hydrogen bonds between main-chain and lateral glucose residues. However, these simulations evidence a moderate and continuous variation of the simulated observables upon increasing the temperature, rather than a sharp transition between the two lowest temperatures (that could be associated with the state transition). Although water-mediated hydrogen-bonded association of neighboring lateral residues is observed, this interaction is not strong enough to promote the formation of an ordered state (correlated motions of the lateral residues), even at the lowest temperature considered
Performance of the ATLAS track reconstruction algorithms in dense environments in LHC Run 2
- Author
- Aaboudd M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaitia Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TP
- Akimov AV
- Alberghia GL
- Alberich LC
- Albert J
- Albicocco P
- Aleksa M
- Aleksandrov IN
- Alexab C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimontia G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisioa A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty M
- Alviggia MG
- Amadio BT
- Amelung C
- Amidei D
- Amorima A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
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- Anders JK
- Andersb CF
- Anderson KJ
- Andreazza A
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- Angelidakis S
- Angelozzi I
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- Annovia A
- Antela C
- Antonelli M
- Antonov A
- Antrim DJ
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- Arai Y
- Aranda CP
- Araquea JP
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin JF
- Argyropoulos S
- Arika M
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
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- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
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- Ayoub MK
- Azuelosd G
- Baasa AE
- Baca MJ
- Bachacou H
- Bachasa K
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- Backhaus M
- Bagnaiaa P
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Baldinc EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Banerjeee S
- Bannoura AAE
- Barajas CAC
- Barak L
- Barberio EL
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- Barisits MS
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- Baroncellia A
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- Barreiro F
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- Boumediene D
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- Burgard CD
- Burger AM
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- Chernyatin V
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- Dhrssen M
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- Di Clemente WK
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- Di Girolamo A
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- Di Petrillo KF
- Di Simone A
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- Dietrich J
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- Djuvslanda JI
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- Toro RC
- Urban SC
- Urek TJ
- Vale MAB
- Vazquez JGP
- Verzini MJA
- Villara DIN
- Walls FMG
- Yildiz HD
- Publication venue
- Publication date
- 01/01/2017
- Field of study
With the increase in energy of the Large Hadron Collider to a centre-of-mass energy of 13 TeV for Run 2, events with dense environments, such as in the cores of highenergy jets, became a focus for new physics searches as well as measurements of the Standard Model. These environments are characterized by charged-particle separations of the order of the tracking detectors sensor granularity. Basic track quantities are compared between 3.2 fb(-1) of data collected by the ATLAS experiment and simulation of protonproton collisions producing high-transverse-momentum jets at a centre-of-mass energy of 13 TeV. The impact of chargedparticle separations and multiplicities on the track reconstruction performance is discussed. The track reconstruction efficiency in the cores of jets with transverse momenta between 200 and 1600 GeV is quantified using a novel, datadriven, method. The method uses the energy loss, dE/ dx, to identify pixel clusters originating from two charged particles. Of the charged particles creating these clusters, themeasured fraction that fail to be reconstructed is 0.061 +/- 0.006 (stat.) +/- 0.014 (syst.) and 0.093 +/- 0.017 (stat.) +/- 0.021 (syst.) for jet transverse momenta of 200-400GeV and 1400-1600GeV, respectively