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!1
Measurements with doubly-charmed
hadronsDaniel Vieira
University of Chinese Academy of Sciences On behalf of LHCb collaboration
9th International Workshop on Charm Physics 22/05/2018
!1
Outline
Introduction
LHCb
Experimental status
Ξcc++ observation
Lifetime measurement
Prospects and conclusion
!2
Doubly Heavy Baryons
Two SU(4) baryon 20-plets (JP = 1/2+ and JP = 3/2+)
Each has a doubly charmed SU(3) triplet (Ξcc++(ccu), Ξcc+(ccd) and Ωcc+(ccs))
!3
JP =1
2
+
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JP =3
2
+
<latexit sha1_base64="GDctsPmO4g0ue7iolgtkLoOYh68=">AAAB/HicdVDLSgMxFM3UV62vapdugkUQhJJUse1CKLoRVxXsA9ppyaSZNjTzIMkIw1B/xY0LRdz6Ie78GzNtBRU9cOFwzr3ce48TCq40Qh9WZml5ZXUtu57b2Nza3snv7rVUEEnKmjQQgew4RDHBfdbUXAvWCSUjniNY25lcpn77jknFA/9WxyGzPTLyucsp0UYa5AvX/QY8hz1XEpqcTJPytH88yBdRCSGEMYYpwZUzZEitVi3jKsSpZVAECzQG+ffeMKCRx3xNBVGqi1Go7YRIzalg01wvUiwkdEJGrGuoTzym7GR2/BQeGmUI3UCa8jWcqd8nEuIpFXuO6fSIHqvfXir+5XUj7VbthPthpJlP54vcSEAdwDQJOOSSUS1iQwiV3NwK6ZiYHLTJK2dC+PoU/k9a5RJGJXxzWqxfLOLIgn1wAI4ABhVQB1egAZqAghg8gCfwbN1bj9aL9TpvzViLmQL4AevtE07yk+o=</latexit><latexit sha1_base64="GDctsPmO4g0ue7iolgtkLoOYh68=">AAAB/HicdVDLSgMxFM3UV62vapdugkUQhJJUse1CKLoRVxXsA9ppyaSZNjTzIMkIw1B/xY0LRdz6Ie78GzNtBRU9cOFwzr3ce48TCq40Qh9WZml5ZXUtu57b2Nza3snv7rVUEEnKmjQQgew4RDHBfdbUXAvWCSUjniNY25lcpn77jknFA/9WxyGzPTLyucsp0UYa5AvX/QY8hz1XEpqcTJPytH88yBdRCSGEMYYpwZUzZEitVi3jKsSpZVAECzQG+ffeMKCRx3xNBVGqi1Go7YRIzalg01wvUiwkdEJGrGuoTzym7GR2/BQeGmUI3UCa8jWcqd8nEuIpFXuO6fSIHqvfXir+5XUj7VbthPthpJlP54vcSEAdwDQJOOSSUS1iQwiV3NwK6ZiYHLTJK2dC+PoU/k9a5RJGJXxzWqxfLOLIgn1wAI4ABhVQB1egAZqAghg8gCfwbN1bj9aL9TpvzViLmQL4AevtE07yk+o=</latexit><latexit sha1_base64="GDctsPmO4g0ue7iolgtkLoOYh68=">AAAB/HicdVDLSgMxFM3UV62vapdugkUQhJJUse1CKLoRVxXsA9ppyaSZNjTzIMkIw1B/xY0LRdz6Ie78GzNtBRU9cOFwzr3ce48TCq40Qh9WZml5ZXUtu57b2Nza3snv7rVUEEnKmjQQgew4RDHBfdbUXAvWCSUjniNY25lcpn77jknFA/9WxyGzPTLyucsp0UYa5AvX/QY8hz1XEpqcTJPytH88yBdRCSGEMYYpwZUzZEitVi3jKsSpZVAECzQG+ffeMKCRx3xNBVGqi1Go7YRIzalg01wvUiwkdEJGrGuoTzym7GR2/BQeGmUI3UCa8jWcqd8nEuIpFXuO6fSIHqvfXir+5XUj7VbthPthpJlP54vcSEAdwDQJOOSSUS1iQwiV3NwK6ZiYHLTJK2dC+PoU/k9a5RJGJXxzWqxfLOLIgn1wAI4ABhVQB1egAZqAghg8gCfwbN1bj9aL9TpvzViLmQL4AevtE07yk+o=</latexit><latexit sha1_base64="GDctsPmO4g0ue7iolgtkLoOYh68=">AAAB/HicdVDLSgMxFM3UV62vapdugkUQhJJUse1CKLoRVxXsA9ppyaSZNjTzIMkIw1B/xY0LRdz6Ie78GzNtBRU9cOFwzr3ce48TCq40Qh9WZml5ZXUtu57b2Nza3snv7rVUEEnKmjQQgew4RDHBfdbUXAvWCSUjniNY25lcpn77jknFA/9WxyGzPTLyucsp0UYa5AvX/QY8hz1XEpqcTJPytH88yBdRCSGEMYYpwZUzZEitVi3jKsSpZVAECzQG+ffeMKCRx3xNBVGqi1Go7YRIzalg01wvUiwkdEJGrGuoTzym7GR2/BQeGmUI3UCa8jWcqd8nEuIpFXuO6fSIHqvfXir+5XUj7VbthPthpJlP54vcSEAdwDQJOOSSUS1iQwiV3NwK6ZiYHLTJK2dC+PoU/k9a5RJGJXxzWqxfLOLIgn1wAI4ABhVQB1egAZqAghg8gCfwbN1bj9aL9TpvzViLmQL4AevtE07yk+o=</latexit>
JP = 3/2+ baryons decay via strong interactions to JP = 1/2+
JP = 1/2+ baryons decay weakly to other flavours
Ξcc++ - Mass
Theoretical predictions of Ξcc++ mass are 3.5-3.7 GeV/c2
and expected to be close to Ξcc+[1-6]!4
https://indico.cern.ch/event/632400/
Ξcc++ - Lifetime
Large ambiguity in theoretical predictions [7-12]
!5
Reference Ξcc++ (ps) Ξcc+ (ps) Ωcc+ (ps)
Karliner, Rosner, 2014 0.185 0.053
Kiselev, Likhoded, Onishchenko, 1998
0.430 +/- 0.100 0.110 +/- 0.010
Kiselev, Likhoded, 2002 0.460 +/- 0.050 0.160 +/- 0.050 0.270 +/- 0.060
Guberina, Melic, Stefancic, 1998
1.050 0.200 0.300
Chang, Li, Li, Wang, 2007 0.670 0.250 0.210
W-exchange
SELEX experiment Ξcc+ measurement
Observed Ξcc+→ Λc+K-π+ and Ξcc+→pD+K- decays
Short lifetime: 𝞃Ξcc+ < 33 fs @90% CL
Large production: exceeding theoretical predictions by orders of magnitude
Mass (combined): 3518.7 ± 1.7 MeV !6
15.9 events
5.62 events
PRL 97, 162001 (2006)
Other Ξcc+ searches
Results not confirmed by other experiments (Focus, BaBar, Belle and LHCb)
JHEP 12 (2013) 090
!7
Belle
SELEXΞcc+
PRL 97, 162001 (2006)
LHCb
Good momentum resolution: p/δp ≈ 0.5% - 1% (5-200 GeV)
Good vertex resolution: IP resolution ≈ 20 µm
Particle identification: 𝜖(𝐾 → 𝐾) ~95%, Mis-ID 𝜖 (𝜋 → 𝐾) ~5% !8
LHCb
L0 hardware trigger: looks for transverse energy signatures
Software high level trigger: near real time alignment and calibration in trigger
!9
LHCb
Run I: 1.0 fb-1 at 7 TeV (2011) + 2.0 fb-1 at 8 TeV (2012)
Run II: 0.3 fb-1 (2015) + 1.7 fb-1 (2016) + 1.7 fb-1 (2017) at 13 TeV !10
Ξcc++→Λc+K-π+π+
Most promising channel for observation [13]
See talk in parallel session tomorrow by Prof. Yu https://indico.inp.nsk.su/event/10/session/7/contribution/29
Lifetime measurementimportant to confirm weakly decaying nature
!11
Dataset, reconstruction and selection
2016 data (1.7fb-1)
Signal kinematical distributions taken from MC
Background distributions taken from wrong-sign Ξcc++→ Λc+ K- π+π- samples
First reconstruct Λc+→pK-π+, then combine with K-π+π+
!12
Dataset, reconstruction and selection
Selection is performed in three steps:
Trigger (dedicated trigger line): Kinematical constraints, PID, track and vertex quality
Preselection: Ghost probability, kinematical constraints, vertex and PV refit quality
MVA: Kinematical constraints and Vertex refit quality!13
Mass fit
Signal yield: 313 ± 33
m⌅++cc
= 3621.40± 0.72(stat)± 0.27(syst)± 0.14(⇤c)MeV
PRL 119 (2017) 112001
!14
𝑚(Ξcc++) = 𝑚(Λc+𝐾-𝜋+) − 𝑚(Λc+) +
Local significance > 12𝜎
Mass value consistent with theoretical range of predictions! Not consistent with Ξcc+ SELEX measurement [MLHCb(Ξcc++) - MSELEX(Ξcc+) = 103 ± 2 MeV ]
Mass fit - Run I data
Also significant in 2012 and consistent with 2016 data
Signal yield: 113 ± 21
PRL 119 (2017) 112001
!15Local significance > 7𝜎
]2c) [MeV/++ccΞ(candm
3500 3600 3700
2 cC
andi
date
s per
5 M
eV/
10
20
30
40
50
60
70
DataTotalSignalBackground
LHCb 8 TeV
�M(2012, 2016) = 0.8± 1.4MeV<latexit sha1_base64="UEJJnJPSGQhCvhrWzuw+HABkLLg=">AAACGXicdVDBahsxENW6TZu6Sbtpj70MMQUHwiKZkCaHgGkuuRhSqO2AdzFaeRyLSLuLpC2Yxb/RS3+llx4aSo7tKX8TreNA2yQPJB7vzTAzLy2UtI7S66Dx5Onas+frL5ovNzZfvQ633gxsXhqBfZGr3Jyl3KKSGfaddArPCoNcpwqH6cVx7Q+/oLEyzz67eYGJ5ueZnErBnZfGIY0nqByHHrRjzd3M6KpDWWcX/L+/2IEjoNEBxIUGFu1BDwfjsEWjQ8oO9xncJyyiS7TICqfj8Hc8yUWpMXNCcWtHjBYuqbhxUihcNOPSYsHFBT/HkacZ12iTannZAt57ZQLT3PiXOViqf3dUXFs716mvrLe3/3u1+JA3Kt30IKlkVpQOM3E7aFoqcDnUMcFEGhROzT3hwki/K4gZN1w4H2bTh3B3KTxOBp2I0Yh92mt1P67iWCfvyDZpE0Y+kC45IaekTwT5Sr6Tn+Qy+Bb8CH4FV7eljWDV85b8g+DPDVZznBs=</latexit><latexit sha1_base64="UEJJnJPSGQhCvhrWzuw+HABkLLg=">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</latexit><latexit sha1_base64="UEJJnJPSGQhCvhrWzuw+HABkLLg=">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</latexit><latexit sha1_base64="UEJJnJPSGQhCvhrWzuw+HABkLLg=">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</latexit>
Signal properties
Measuring its lifetime is crucial to establish the weak nature of its decay and for comparison with theoretical predictions
!16
PRL 119 (2017) 112001
Lifetime measurementWe perform a lifetime measurement, using the Ξcc++→ Λc+K-π+π+ decay, relative to the control channel of same topology, Λb0→Λc+π−π+π−
Unbinned maximum likelihood fit of the background subtracted Ξcc++ decay time distribution (sFit)
!17
f⌅++cc
(t) = h⇤0b(t)⇥
✏⌅++cc
(t)
✏⇤0b(t)
⇥ e�
1⌧⌅++cc
� 1⌧⇤0b
!t
<latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit><latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit><latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit><latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit>
Lifetime measurementWe perform a lifetime measurement, using the Ξcc++→ Λc+K-π+π+ decay, relative to the control channel of same topology, Λb0→Λc+π−π+π−
Unbinned maximum likelihood fit of the background subtracted Ξcc++ decay time distribution (sFit)
Λb0 data and acceptances incorporated to PDF as histograms
!17
f⌅++cc
(t) = h⇤0b(t)⇥
✏⌅++cc
(t)
✏⇤0b(t)
⇥ e�
1⌧⌅++cc
� 1⌧⇤0b
!t
<latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit><latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit><latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit><latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit>
Lifetime measurementWe perform a lifetime measurement, using the Ξcc++→ Λc+K-π+π+ decay, relative to the control channel of same topology, Λb0→Λc+π−π+π−
Unbinned maximum likelihood fit of the background subtracted Ξcc++ decay time distribution (sFit)
Λb0 data and acceptances incorporated to PDF as histograms
PDG Λb0 lifetime (1.470 +/- 0.010 ps) used as input
!17
f⌅++cc
(t) = h⇤0b(t)⇥
✏⌅++cc
(t)
✏⇤0b(t)
⇥ e�
1⌧⌅++cc
� 1⌧⇤0b
!t
<latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit><latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit><latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit><latexit sha1_base64="AEEptZaEYMmBgZ9WhIB8h8JBcxU=">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</latexit>
Lifetime measurementWe perform a lifetime measurement, using the Ξcc++→ Λc+K-π+π+ decay, relative to the control channel of same topology, Λb0→Λc+π−π+π−
Unbinned maximum likelihood fit of the background subtracted Ξcc++ decay time distribution (sFit)
Λb0 data and acceptances incorporated to PDF as histograms
PDG Λb0 lifetime (1.470 +/- 0.010 ps) used as input
Measurement performed with Λb0 and result consistent with PDG value !17
f⌅++cc
(t) = h⇤0b(t)⇥
✏⌅++cc
(t)
✏⇤0b(t)
⇥ e�
1⌧⌅++cc
� 1⌧⇤0b
!t
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Data samples and selectionLHCb 2016 (~1.7 fb-1 - 13TeV)
Mostly same selection criteria of observation
Specific hardware trigger:
Large hadronic ET deposit from decay products;
Or large ET deposit in calorimeters or muon stations from tracks other than the decay products
Decay time range: 0.10-2.00 ps
Mass fits used to obtain sWeights!18
N⌅++cc
= 304± 35<latexit sha1_base64="yKKda7lkm6YQDff1sKlgKWO56RA=">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</latexit><latexit sha1_base64="yKKda7lkm6YQDff1sKlgKWO56RA=">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</latexit><latexit sha1_base64="yKKda7lkm6YQDff1sKlgKWO56RA=">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</latexit><latexit sha1_base64="yKKda7lkm6YQDff1sKlgKWO56RA=">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</latexit>
N⇤0b= 3397± 119
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]2c) [MeV/+π+π−π+cΛ(m5500 5600 5700
)2 cC
andi
date
s / (5
MeV
/
0
100
200
300
400
500
600
700
800
DataTotal fitSignalBackground
LHCbPreliminary
(b)
]2c) [MeV/+π+π−K+cΛ(m3500 3600 3700
)2 cC
andi
date
s / (5
MeV
/
020406080
100120140160
DataTotal fitSignalBackground
LHCbPreliminary
(a)
LHCB-PAPER-2018-19
LHCB-PAPER-2018-19
Decay time
Normalized, background subtracted decay time distributions!19
0.5 1 1.5 2Decay time [ps]
0.00
0.05
0.10
0.15
0.20N
orm
aliz
ed y
ield
/ (0
.095
ps)
++ccΞ0bΛ
LHCbPreliminary
LHCB-PAPER-2018-19
Decay time and acceptance
MC samples reweighted to match PT distributions in data
!20
0.5 1 1.5 2Decay time [ps]
0
0.5
1
1.5
2
2.5
3
Acc
epta
nce
(arb
itrar
y sc
ale)
++ccΞ0bΛ
LHCb simulation
✏(t) =Nrec(t)
Ngen(t)<latexit sha1_base64="2ej3clzrm9qbk1fEwEtN+p+IPiw=">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</latexit><latexit sha1_base64="2ej3clzrm9qbk1fEwEtN+p+IPiw=">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</latexit><latexit sha1_base64="2ej3clzrm9qbk1fEwEtN+p+IPiw=">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</latexit><latexit sha1_base64="2ej3clzrm9qbk1fEwEtN+p+IPiw=">AAACFXicdZDNSgMxFIUz/lv/qi7dBIugICVTKjoLoejGlVSwWmhLyaR32tBMZkgyQhn6Em58FTcuFHEruPNtzIwVVPRA4OPce7m5x48F14aQd2dqemZ2bn5hsbC0vLK6VlzfuNJRohg0WCQi1fSpBsElNAw3ApqxAhr6Aq794WlWv74BpXkkL80ohk5I+5IHnFFjrW5xvw2x5iKSeNfs4WPcDhRl6Xk3VcDG1hpn3AeZc7dYImXPI5UqwRkcVI68HAjxPOyWSa4SmqjeLb61exFLQpCGCap1yyWx6aRUGc4EjAvtRENM2ZD2oWVR0hB0J82vGuMd6/RwECn7pMG5+30ipaHWo9C3nSE1A/27lpl/1VqJCY46KZdxYkCyz0VBIrCJcBYR7nF7vBEjC5Qpbv+K2YDaXIwNsmBD+LoU/w9XlbJLyu5FtVQ7mcSxgLbQNtpFLjpENXSG6qiBGLpF9+gRPTl3zoPz7Lx8tk45k5lN9EPO6wfk2Z6x</latexit>
LHCB-PAPER-2018-19
Decay time [ps]0.5 1 1.5 2
Yie
ld /
(0.0
95 p
s)
0
10
20
30
40
50
60 LHCbPreliminary
DataFit
Results
!21
⌧⌅++cc
= 0.256+0.024�0.022 ps (stat. only)
<latexit sha1_base64="L/bO6/9ndZPZyo20q36qnBAJFU8=">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</latexit><latexit sha1_base64="L/bO6/9ndZPZyo20q36qnBAJFU8=">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</latexit><latexit sha1_base64="L/bO6/9ndZPZyo20q36qnBAJFU8=">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</latexit><latexit sha1_base64="L/bO6/9ndZPZyo20q36qnBAJFU8=">AAACXnicdVFRa9swEJa9re3Sdc22l0JfxMKgo8zIJl7ah0HpXvrYQdMG4szIitKISrKRzoMg/Cf3VvrSn1I5zaAN64Hgu++74+4+FZUUFgi5DcJXr99sbG697Wy/23m/2/3w8dKWtWF8yEpZmlFBLZdC8yEIkHxUGU5VIflVcfOz1a/+cGNFqS9gUfGJotdazASj4Km8W2dA69xlI5E7xprf7vCwafAPTKIk/e4zEpGk3+TuWwuSBmdzW1HGHYlipnyqKMyNcriy69KBBQrROltqufja5N0eiY6PSZIS3IK0nw5acJTGgz6OI7KMHlrFed79m01LViuugUlq7TgmFUwcNSCY5E0nqy33Y27oNR97qKniduKW9jT4i2emeFYa/zTgJfu0w1Fl7UIVvrI9x65rLfk/bVzD7GjihK5q4Jo9DprVEkOJW6/xVBjOQC48oMwIvytmc2ooA/8jHW/Cv0vxy+AyiWLv3a9+7+R0ZccW2kef0QGK0QCdoDN0joaIobsgCDrBdnAfboQ74e5jaRisej6hZxHuPQCvgrH+</latexit>
Statistical errors from MC and Λb0 samples obtained from pseudoexperiments
LHCB-PAPER-2018-19
�MC = 0.007 ps<latexit sha1_base64="Zm42EmIIq47weJzpo9K/jDuX5Ao=">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</latexit><latexit sha1_base64="Zm42EmIIq47weJzpo9K/jDuX5Ao=">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</latexit><latexit sha1_base64="Zm42EmIIq47weJzpo9K/jDuX5Ao=">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</latexit><latexit sha1_base64="Zm42EmIIq47weJzpo9K/jDuX5Ao=">AAACGXicdVDLSgMxFM34rPU16tJNsAiuSqa0tF0IxW7cCBXsAzpDyaRpG5rMDElGKMP8hht/xY0LRVzqyr8x01ZQ0QMXDufcy733+BFnSiP0Ya2srq1vbOa28ts7u3v79sFhR4WxJLRNQh7Kno8V5Sygbc00p71IUix8Trv+tJn53VsqFQuDGz2LqCfwOGAjRrA20sBGrmJjgQfJVTOF5xAVEapCd6IiTGiCig4kIoWuwHoiRRKpFA7sAirW66hUQTAjlXKlmpFaxamWoWPmMxTAEq2B/eYOQxILGmjCsVJ9B0XaS7DUjHCa5t1YUbNtise0b2iABVVeMv8shadGGcJRKE0FGs7V7xMJFkrNhG86sxvVby8T//L6sR7VvIQFUaxpQBaLRjGHOoRZTHDIJCWazwzBRDJzKyQTLDHRJsy8CeHrU/g/6ZSKjonwulxoXCzjyIFjcALOgAOqoAEuQQu0AQF34AE8gWfr3nq0XqzXReuKtZw5Aj9gvX8C/tGfGg==</latexit>
�⇤0b= 0.006 ps
<latexit sha1_base64="sI4xMgGZENeaRl88/y7N54ANm6M=">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</latexit><latexit sha1_base64="sI4xMgGZENeaRl88/y7N54ANm6M=">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</latexit><latexit sha1_base64="sI4xMgGZENeaRl88/y7N54ANm6M=">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</latexit><latexit sha1_base64="sI4xMgGZENeaRl88/y7N54ANm6M=">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</latexit>
Systematic uncertainties
!22
Source Uncertainty (ps) Signal and background mass models 0.005Correlation of mass and decay-time 0.004Binning 0.001Data-simulation differences 0.004Resonant structure of decays 0.011Hardware trigger threshold 0.002Simulated Ξcc++ lifetime 0.002Λ0b lifetime uncertainty 0.001Sum in quadrature 0.014
Total systematic uncertainties significantly lower than statistical uncertainties
Additional Checks
Sample splitting
Charge
Polarity
Number of primary vertices
L0 requirements
Binned approach
!23
Future prospectsΞcc++:
Other decay modes:
Ξcc++→Ξc+π+
Ξcc++→Λc+π+
Ξcc++→pD+K-π+
Production cross-section
Other states:
Ξcc+
Ωcc+ !24
Conclusions
A significant structure consistent with Ξcc++ was observed in LHCb 2016 data PRL 119, 112001 (2017)
Measured mass is consistent with theoretical range of predictions*
Lifetime is measured to be:LHCB-PAPER-2018-19
Many studies more to come:
Other Ξcc++ decay modes and properties
Other doubly-charmed baryon states!25
⌅++cc = 0.256+0.024
�0.022 (stat.) ± 0.014 (syst.) ps<latexit sha1_base64="1J/R1ZwhNAe1486R/wZx0zI4hC8=">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</latexit><latexit sha1_base64="1J/R1ZwhNAe1486R/wZx0zI4hC8=">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</latexit><latexit sha1_base64="1J/R1ZwhNAe1486R/wZx0zI4hC8=">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</latexit><latexit sha1_base64="1J/R1ZwhNAe1486R/wZx0zI4hC8=">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</latexit>
m⌅++cc
= 3621.40± 0.72(stat)± 0.27(syst)± 0.14(⇤c)MeV
*not compatible with SELEX Ξcc+ mass measurement
!26
Backup
LHCb
JINST 3 (2008) S08005 IJMPA 30 (2015) 1530022 !27
LHCb
Interaction Region
JINST 3 (2008) S08005 IJMPA 30 (2015) 1530022 !27
LHCb
- Vertex Locator (vertex reconstruction)• Impact parameter resolution: 20μm• Decay time resolution: 45 fs (𝜏}~1.5 p
JINST 3 (2008) S08005 IJMPA 30 (2015) 1530022 !27
LHCb- Tracking system (particle reconstruction)
• 𝜖 Tracking ~ 96% • 𝛿𝑝⁄𝑝 ~ 0.5%-1% (5-200 GeV) • 𝜎(mB→cc) ≈ 22MeV
JINST 3 (2008) S08005 IJMPA 30 (2015) 1530022 !27
LHCb- Magnet
• Bending power: 4 Tm • Reversable polarity
JINST 3 (2008) S08005 IJMPA 30 (2015) 1530022 !27
LHCb- RICH detectors (𝐾⁄𝜋/𝑝 separation)
• 𝜖 (𝐾 → 𝐾) ~95% • Mis-ID 𝜖 (𝜋 → 𝐾) ~5%
JINST 3 (2008) S08005 IJMPA 30 (2015) 1530022 !27
LHCb- Calorimeters
• L0 • Scintilating detectors • ID and energy
JINST 3 (2008) S08005 IJMPA 30 (2015) 1530022 !27
LHCb- Muon chambers
• Multi-Wire Proportional Chamber (MWPC) • MisID rates between 6.2% and 0.33 %
JINST 3 (2008) S08005 IJMPA 30 (2015) 1530022 !27
Additional testsMultiple candidates: not creating fake narrow structure
Checking combinations of tracks from Λc+ and Ξcc++ : not peaking
MVA efficiency as a function of mass: very smooth
Varying threshold value of MVA selector and using cut based selection: structure stays significant
Varying particle ID selections: no peaking structure emerging in WS combinations, structure stays in RS sample
Run I sample used as crosscheck: same structure seen!28
Additional tests
Structure still significant with 𝛕Ξcc > 5σ
Consistent with weak decay
!29
Systematic uncertainties
!30
References[1]D.-H. He et al., Evaluation of spectra of baryons containing two heavy quarks in bag model, Phys. Rev. D70 (2004) 094004, arXiv:hep-ph/0403301.
[2]C.-H. Chang, C.-F. Qiao, J.-X. Wang, and X.-G. Wu, Estimate of the hadronic production of the doubly charmed baryon Ξcc under GM-VFN scheme, Phys. Rev. D73 (2006) 094022, arXiv:hep-ph/0601032.
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