This is a sel -a chi ed e sion o an o iginal a icle. This e sion
may di e om he o iginal in pagina ion and ypog aphic de ails.
Au ho (s):
Ti le:
Yea :
Ve sion:
Copy igh :
Righ s:
Righ s u l:
Please ci e he o iginal e sion:
CC BY 4.0
h ps://c ea i ecommons.o g/licenses/by/4.0/
K(892)0 and φ(1020) p oduc ion in p-Pb collisions a √sNN = 8.16 TeV
©2023 CERN, o he ALICE Collabo a ion
Published e sion
ALICE Collabo a ion
ALICE Collabo a ion. (2023). K(892)0 and φ(1020) p oduc ion in p-Pb collisions a √sNN = 8.16
TeV. Physical Re iew C, 107(5), A icle 055201. h ps://doi.o g/10.1103/PhysRe C.107.055201
2023
PHYSICAL REVIEW C 107, 055201 (2023)
K∗(892)0and φ(1020) p oduc ion in p-Pb collisions a √sNN =8.16 TeV
S. Acha ya e al.∗
(ALICE Collabo a ion)
(Recei ed 28 Oc obe 2021; accep ed 16 Decembe 2022; published 9 May 2023)
The p oduc ion o K∗(892)0and φ(1020) esonances has been measu ed in p-Pb collisions a √sNN =
8.16 TeV using he ALICE de ec o . Resonances a e econs uc ed ia hei had onic decay channels in he
apidi y in e al −0.5 <y<0 and he ans e se momen um spec a a e measu ed o a ious mul iplici y
classes up o pT=20 GeV/c o K
∗(892)0and pT=16 GeV/c o φ(1020). The pT-in eg a ed yields and mean
ans e se momen a a e epo ed and compa ed wi h p e ious esul s in pp, p-Pb and Pb-Pb collisions. The xT
scaling o K∗(892)0and φ(1020) esonance p oduc ion is newly es ed in p-Pb collisions and ound o hold in
he high-pT egion a La ge Had on Collide ene gies. The nuclea modi ica ion ac o s (RpPb) as a unc ion o pT
o K∗0and φa √sNN =8.16 TeV a e p esen ed along wi h he new RpPb measu emen s o K∗0,φ,,anda
√sNN =5.02 TeV. A in e media e pT(2–8 GeV/c), RpPb o ,show a C onin-like enhancemen , while
K∗0and φshow no o li le nuclea modi ica ion. A high pT(>8 GeV/c), he RpPb alues o all had ons a e
consis en wi h uni y wi hin unce ain ies. The RpPb o K∗(892)0and φ(1020) a √sNN =8.16 and 5.02 TeV
show no signi ican ene gy dependence.
DOI: 10.1103/PhysRe C.107.055201
I. INTRODUCTION
High-ene gy hea y-ion (A-A) collisions p o ide a unique
oppo uni y o s udy he decon ined qua k-gluon plasma
(QGP) c ea ed in such collisions [1–3]. The ho and dense
medium c ea ed in hea y-ion collisions e ol es wi h ime
and cools down o o m a phase whe e had on esonance
gas is s udied. E idence a Rela i is ic Hea y Ion Collide
(RHIC) and he La ge Had on Collide (LHC) sugges ha
he QGP phase is ollowed by a had onic phase whe e he
had ons in e ac ia esca e ing and egene a ion p ocesses,
be o e he inal eeze-ou . Resonances a e sho -li ed had ons
ha decay ia he s ong in e ac ions. They play an impo -
an ole o unde s and he pa icle p oduc ion mechanisms
and o he cha ac e iza ion o he dynamic e olu ion o he
sys em o med in hea y-ion collisions. They a e used as
a sensi i e p obe o he had onic phase, whe e hei mass,
wid h and yield could be modi ied due o in e ac ion o hei
decay p oduc s h ough e-sca e ing and egene a ion p o-
cesses [4–15]. ALICE has p e iously measu ed K∗(892)0and
φ(1020) p oduc ion in pp collisions a √s=5.02, 7, 8, and
13 TeV [16–22], in p-Pb collisions a √sNN =5.02 TeV
[23] and Pb-Pb collisions a √sNN =2.76 and 5.02 TeV
[13,15,18,19].
P o on-lead collisions a e in e media e be ween pp and
Pb-Pb collisions in e ms o he size o he colliding sys em
∗Full au ho lis gi en a he end o he a icle.
Published by he Ame ican Physical Socie y unde he e ms o he
C ea i e Commons A ibu ion 4.0 In e na ional license. Fu he
dis ibu ion o his wo k mus main ain a ibu ion o he au ho (s)
and he published a icle’s i le, jou nal ci a ion, and DOI.
and he p oduced pa icle mul iplici ies. Recen measu emen s
in high-mul iplici y pp,p-Pb, and d-Au collisions a di e en
ene gies ha e unco e ed s ong lowlike e ec s e en in hese
small collision sys ems [14,22–25], whose o igin is no ully
unde s ood. To in es iga e he mechanism o pa icle p oduc-
ion and he o igin o hese e ec s, he ALICE Collabo a ion
has s udied he mul iplici y dependence o ligh - la o pa i-
cle p oduc ion o many species like π±,K
±,K
0
S,K
∗(892)0,
φ(1020), ,(1520), ∗±,±,∗0,±in p-Pb collisions
a √sNN =5.02 TeV [23,26–29] and in pp collisions a
√s=7 and 13 TeV [17,20,22,30]. This pape epo s on
he mul iplici y dependence o K∗(892)0and φ(1020) meson
p oduc ion a he highes cen e -o -mass ene gy, √sNN =
8.16 TeV, eached a he LHC in p-Pb collisions. This p o ides
an oppo uni y o ex end he p e ious s udies o p oduc ion
o hese pa icles in p-Pb collisions a √sNN =5.02 TeV
[23] o a highe mul iplici y each and a la ge pTco e age.
Had on p oduc ion is go e ned by he so and ha d sca e ing
p ocesses a LHC ene gies. The bulk o pa icles p oduced
in high-ene gy collisions is domina ed by low ans e se
momen um pa icles om so in e ac ions, which a e nonpe -
u ba i e in na u e. The yield o pa icles a low pTis no well
unde s ood om he i s p inciples o QCD and hei desc ip-
ion elies on phenomenological QCD-based models such as
EPOS-LHC, DPMJET, and HIJING. The measu emen s in he
low-momen um egion o he spec a p esen ed in his a icle
p o ide inpu o he uning o hese e en gene a o s. In his
pape , measu emen s o K∗(892)0and φ(1020) a e compa ed
wi h p edic ions om EPOS-LHC [31], DPMJET [32], and
HIJING [33].
The ans e se momen um spec a o ligh – la o had ons
ha e shown a clea e olu ion wi h mul iplici y in high-ene gy
pp and p-Pb collisions [17,22,23,26,34], simila o ha ob-
se ed in Pb-Pb collisions [13,18,19,35,36], whe e in he la e
2469-9985/2023/107(5)/055201(21) 055201-1 ©2023 CERN, o he ALICE Collabo a ion
S. ACHARYA e al. PHYSICAL REVIEW C 107, 055201 (2023)
case he e ec is usually a ibu ed o a collec i e expansion
o he sys em. The inc ease in slope o he pTspec a as a
unc ion o mul iplici y a ibu ed o he adial low is ela ed
o he low-pT egion o he spec um, whe e low is ele an .
This ea u e is also e lec ed in an inc ease o he a e age
ans e se momen um pTwi h mul iplici y. In con as o
he yields dN/dy, which e ol e smoo hly as a unc ion o
mul iplici y o di e en collision sys ems, he pTo ligh -
la o had ons as well as K∗(892)0and φ(1020), ises as e
as a unc ion o mul iplici y in pp and p-Pb collisions han
in Pb-Pb collisions, as discussed in Re s. [20,22,23]. The new
measu emen s, wi h he highes mul iplici y each in p-Pb col-
lisions, and compa ison wi h he di e en model p edic ions
can be used o u he ex end hese s udies.
The high-pTpa icle p oduc ion is analyzed wi hin
he amewo k o pe u ba i e Quan um Ch omodynamics
(pQCD) which ea u es a nea ly scale-in a ian beha io o
elemen a y pa on-pa on ha d-sca e ing p ocesses [37,38].
The con olu ion o ha d sca e ing c oss-sec ions wi h he
pa on dis ibu ion unc ions (PDFs) o inciden had ons and
agmen a ion unc ions (FFs) leads o he obse ed scaling
o he inclusi e in a ian c oss-sec ion Ed3σ/dp
3as p−n
Ta
ixed ans e se x,xT=2pT/√s[39,40]. The exponen n
can be ela ed o he sca e ing p ocesses in which high-pT
had ons a e p oduced. I had ons a e p oduced by leading
wis (LT) 2 →2 ha d subp ocesses, hen n ≈4, and o
highe wis (HT) p ocesses, n≈8. I has been obse ed ha
he exponen alue dec eases wi h inc easing collision ene gy,
which sugges s ha he con ibu ion o highe wis p ocesses
on high-pThad on p oduc ion is educed as a unc ion o
ene gy. The ans e se momen um dis ibu ions o di e en
pa icle species a high pTa e obse ed o sa is y a uni e sal
xTscaling o e a wide ene gy ange up o √s=13 TeV. This
scaling beha io was obse ed by he CDF [41–43] and UA1
[44] Collabo a ions in p(p) collisions, and by he STAR [45],
ALICE [46], and CMS [47] Collabo a ions in pp collisions.
In his pape , he xTscaling o K∗(892)0and φ(1020) mesons
a e es ed in p-Pb collisions a LHC ene gies. The ans e se
momen um dis ibu ions o he pa icles in p-Pb collisions
a e compa ed o hose in pp collisions using he nuclea
modi ica ion ac o (RpPb). The measu emen o RpPb ac s as
a con ol expe imen obse able in p-Pb collisions [48]in
he con ex o he obse ed high-pThad on supp ession in
Pb-Pb collisions [15]. In his pape , RpPb measu emen s o
K∗(892)0and φ(1020) in p-Pb collisions a √sNN =5.02 and
8.16 TeV, and ha o and in p-Pb collisions a 5.02
TeV a e epo ed. Simila measu emen s a e also epo ed o
s ange and mul is ange had ons by CMS [49], and o π±,
K±, and p(p) by ALICE [26]inp-Pb collisions a √sNN =
5.02 TeV. A high pT(>8GeV/c), he alues o RpPb o
all ligh had ons a e simila and ound o be consis en wi h
uni y wi hin he unce ain ies. A in e media e pT(2 <pT<
8GeV/c), he alues o RpPb o s ange ba yons (,)show
an enhancemen wi h a clea mass dependence [49]. In his
pT egion, he ha d sca e ing p ocesses s a o domina e o e
so p ocesses and he momen um ange whe e his ansi ion
may happen depend on he mass and qua k composi ion o
he pa icle species. The measu emen s o s ange pa icles
p oduced in high mul iplici y p-Pb collisions [27,50] sug-
ges ed he p esence o adial low [51]. Due o he adial low
e ec , had ons o g ea e mass a e pushed owa ds he highe
ans e se momen um and he e ec inc eases wi h had on
mass as well as mul iplici y [23,51]. Howe e , i should be
no ed ha some inal s a e e ec s such as colo econnec ion
in PYTHIA [52] which can mimic he adial lowlike e ec
and EPOS-LHC [31]which uses pa ame e ized low could
desc ibe he modi ica ion o ans e se momen um spec a.
The di e ence in he p oduc ion mechanism o ba yon and
meson has been obse ed in pa icle a ios [23,51] and he
nuclea modi ica ion ac o s [25,26,45,49,53]. The enhanced
p oduc ion o ba yon (RpPb >1) may happen as a esul o
had oniza ion by pa on ecombina ion [54]. In addi ion, he e
a e se e al ini ial-s a e e ec s such as isospin e ec , C onin
e ec , cold–nuclea ma e ene gy loss and nuclea shadowing
ha can esul in RpPb = 1[55]. The C onin enhancemen
[56] in he in e media e pTa e epo ed in he low-ene gy
expe imen s [57,58]. Simila enhancemen is obse ed o
(an i)p o on compa ed o pion and kaon in p-Pb collisions
a √sNN =5.02 TeV [26]. In his pape , he pa icle species
and collision ene gy dependence o RpPb is s udied o p-Pb
collisions a LHC ene gies.
Th oughou his pape , he esul s o K∗(892)0and
K∗(892)0a e a e aged and deno ed by he symbol K∗0, while
φ(1020) is deno ed by φ. The pape is o ganized as ollows.
In Sec. II, he da ase , e en , and ack selec ion c i e ia;
he analysis echniques; he p ocedu e o ex ac ion o he
yields; and he s udy o he sys ema ic unce ain ies a e b ie ly
discussed. In Sec. III, he esul s on he ans e se momen um
spec a, he dN/dy,pT,xTscaling, and RpPb in p-Pb colli-
sions a √sNN =8.16 TeV a e p esen ed. Finally, he esul s
a e summa ized in Sec. IV.
II. DATA ANALYSIS
The measu emen s o K∗0and φmeson p oduc ion in p-Pb
collisions a √sNN =8.16 TeV ha e been pe o med on da a
collec ed wi h he ALICE de ec o in he yea 2016. The
esonances a e econs uc ed ia hei had onic decay chan-
nels wi h b anching a ios (BR) o 66.6% o K∗0→π±K∓
and 49.2% o φ→K+K−in he apidi y in e al −0.5 <
y<0, whe e ys ands o he apidi y in he nucleon-nucleon
cen e -o -mass. Fo bo h K∗0and φ, he analysis is pe o med
in a ious mul iplici y classes and also using a mul iplici y-
in eg a ed sample.
A. E en selec ion
The de ailed desc ip ion o he ALICE de ec o se up and
i s pe o mance can be ound in Re s. [59,60]. In p-Pb con-
igu a ions, he 208Pb beam ci cula es owa ds he posi i e z
di ec ion in he ALICE labo a o y ame, while he p o on
beam ci cula es in he opposi e di ec ion. Due o he asymme -
ic sys em, he cen e -o -mass ame is shi ed in he apidi y
by y=−0.465 in he di ec ion o he p o on beam wi h
espec o he labo a o y ame. The minimum bias igge
was con igu ed o selec e en s by equi ing a leas a coinci-
dence signal in bo h he V0A and V0C de ec o s [61,62]. The
V0 de ec o sys em consis s o wo a ays o 32 scin illa o
055201-2
K∗(892)0AND φ(1020) PRODUCTION IN p-Pb COLLISIONS … PHYSICAL REVIEW C 107, 055201 (2023)
TABLE I. Mean cha ged pa icle mul iplici y densi ies
(dNch/dη) measu ed in pseudo apidi y ange |ηlab|<0.5,
co esponding o he a ious mul iplici y classes de ined using he
V0A de ec o in p-Pb collisions a √sNN =8.16 TeV [62].
V0A pe cen ile (%) dNch/dη|ηlab|<0.5
0–5 53.22 ±1.38
5–10 42.40 ±1.10
10–20 35.49 ±0.92
20–40 26.89 ±0.70
40–60 18.39 ±0.48
60–80 10.97 ±0.29
80–100 4.47 ±0.14
de ec o s, one on each side o he in e ac ion poin co e ing
he ull azimu hal angle in he pseudo apidi y egions 2.8 <
η<5.1 (V0A) and −3.7 <η<−1.7 (V0C). The backg ound
e en s due o beam-gas in e ac ion and o he machine-induced
backg ound collisions a e ejec ed using he iming in o ma-
ion om he V0 and he ze o deg ee calo ime e (ZDC) [60].
The p ima y e ex o a collision is de e mined using cha ged
acks econs uc ed in he inne acking sys em (ITS) [63]
and he ime p ojec ion chambe (TPC) [64]. The e en s a e
selec ed whose p ima y e ex posi ion along he beam axis
( z,zis he longi udinal di ec ion) is wi hin ±10 cm om
he nominal in e ac ion poin . Pileup e en s om he igge ed
bunch c ossing a e ejec ed i mul iple collision e ices a e
iden i ied in he silicon pixel de ec o (SPD), which is he
inne mos de ec o o he ITS [60,64]. The o al numbe o
e en s analyzed a e applying he e en selec ion c i e ia is
abou 30 million. The minimum bias e en s a e u he di ided
in o se en mul iplici y classes, acco ding o he o al cha ge
deposi ed in he o wa d V0A de ec o [61]. The yield o
K∗0and φa e measu ed in he apidi y in e al −0.5 <y<0
o he ollowing e en mul iplici y classes, 0–5%, 5–10%,
10–20%, 20–40%, 40–60%, 60–80%, and 80–100%. The pT
spec a no malized o he ac ion o non-single-di ac i e
(NSD) e en s a e also ob ained o bo h K∗0and φ. The mean
cha ged-pa icle mul iplici y (dNch/dη) co esponding o
each mul iplici y class, and measu ed in he pseudo apid-
i y in e al |ηlab|<0.5, is gi en in Table I aken om
Re . [62].
B. T ack selec ion and pa icle iden i ica ion
The cha ged acks coming om he p ima y e ex a e
selec ed in he pseudo apidi y in e al |η|<0.8 wi h pT>
0.15 GeV/c. This ensu es he uni o m accep ance o he
cen al ba el de ec o s. The high quali y acks a e chosen
based on selec ion c i e ia as done p e iously in Re . [23].
The K∗0and φmesons a e econs uc ed om he cha ged
acks which ha e c ossed a leas 70 o a maximum 159
ho izon al segmen s along he ans e se eadou plane o he
TPC. The con amina ion om seconda y pa icles o igina ing
om weak decays and beam backg ound e en s a e educed
by applying a selec ion on he dis ance o closes app oach
o he p ima y e ex in he ans e se plane (DCAxy) and
along he longi udinal di ec ion (DCAz). A pT-dependen
cu o DCAxy(pT)<(0.0105 +0.035p−1.1
T) cm, wi h pTin
GeV/c, is used, which is less han 7 imes i s esolu ion. The
ack DCAzis equi ed o be less han 2 cm [65]. The decay
daugh e s (pions and kaons) o esonances a e iden i ied by
measu ing he speci ic ioniza ion ene gy loss (dE/dx)in he
de ec o gas o he TPC and hei ime-o - ligh in o ma ion
using he TOF [66]. The dE/dx esolu ion o he TPC is
deno ed as σTPC and he cha ged acks a e iden i ied as pions
and kaons i he mean speci ic ene gy loss measu ed by he
TPC is wi hin 6σTPC,3σTPC, and 2σTPC om he expec ed
dE/dx alues in he momen um ange p<0.3 GeV/c,
0.3 <p<0.5 GeV/c, and p>0.5 GeV/c, espec i ely.
In addi ion o he TPC, i he TOF in o ma ion is a ailable,
hen he cha ged acks a e iden i ied by equi ing he ime-
o - ligh alues wi hin 3σTOF o he expec ed alues o he
ull momen um ange.
C. Yield ex ac ion
The K∗0and φ esonances a e econs uc ed om hei de-
cay p oduc s using he in a ian mass echnique. The in a ian
mass dis ibu ions a e ob ained om unlike cha ge πK( o
K∗0) and KK ( o φ) pai s in he same e en . The dis ibu ions
exhibi a signal peak and a la ge combina o ial backg ound
om he unco ela ed πK (KK) pai s. The combina o ial
backg ound is es ima ed using wo me hods, mixed-e en and
like-sign. In he mixed-e en me hod, he acks om one
e en a e pai ed wi h opposi ely cha ged acks om o he
e en s. Each e en is mixed wi h i e o he e en s o educe
he con ibu ion o s a is ical unce ain y om he backg ound
dis ibu ion. The e en s which a e mixed a e selec ed o ha e
simila cha ac e is ics like he longi udinal posi ion o p ima y
e ex ( z) mus di e by less han 1 cm and he mul iplici y
pe cen iles compu ed using he V0A ampli ude mus di e
by less han 5%. The mixed-e en dis ibu ions o K∗0(φ)
a e no malized in he mass egion 1.1 <min <1.15 GeV/c2
(1.04 <min <1.15 GeV/c2) ha is app oxima ely i e σ
away om he mass peak o each pa icle. In he like-sign
me hod, acks o iden ical cha ges om he same e en s a e
pai ed and he in a ian mass dis ibu ion o he unco ela ed
backg ound is ob ained as he geome ic mean 2√n++ ×n−−,
whe e n++ and n−− a e he numbe o posi i e-posi i e and
nega i e-nega i e pai s in each in a ian mass bin, espec-
i ely. The mixed-e en echnique is he de aul me hod used
o he ex ac ion o yield bo h o K∗0and φ, whe eas he
like-sign backg ound is used o he es ima ion o he sys em-
a ic unce ain y. Figu es 1(a) and 1(b) show he in a ian mass
dis ibu ions o π∓K±and K+K−pai s om he same e en s
and he mixed-e en s in he ans e se momen um in e al
1.4 ⩽pT<1.6 and 0.6 ⩽pT<0.8 GeV/c o 0–100% in
p-Pb collisions, espec i ely. The π∓K±and K+K−in a ian
mass dis ibu ions a e mixed-e en backg ound sub ac ion
a e shown in Figs. 1(c) and 1(d), espec i ely, whe e he
cha ac e is ic signal peak is obse ed on op o he esidual
backg ound. The esidual backg ound a ises due o co ela ed
pai s om je s, misiden i ica ion o he decay daugh e s o
esonances and decay o o he pa icles [23]. The aw yields
o esonances a e ex ac ed in each pTbin and mul iplici y
055201-3
S. ACHARYA e al. PHYSICAL REVIEW C 107, 055201 (2023)
FIG. 1. In a ian mass dis ibu ions o K∗0and φin he mul iplici y class 0–100% and ans e se momen um ange 1.4 ⩽pT<1.6 GeV/c
and 0.6 ⩽pT<0.8 GeV/c, espec i ely. In panels (a), (b), black ma ke s show he unlike-sign in a ian mass dis ibu ions and ed ma ke s
show he no malized mixed e en backg ound. A e he backg ound sub ac ion he signals a e shown in panels (c), (d). The K∗0peak is
desc ibed by a B ei -Wigne unc ion, whe eas he φpeak is i ed wi h a Voig ian unc ion. The esidual backg ound is desc ibed by he
second-o de polynomial unc ion.
class. The signal peak is i ed wi h a B ei -Wigne and a
Voig ian unc ion (con olu ion o B ei -Wigne and Gaussian
unc ions) o K∗0and φ, espec i ely. A second-o de poly-
nomial unc ion is used o desc ibe he shape o he esidual
backg ound o bo h esonances. The signal peak i is pe -
o med in he ange 0.75 <MKπ<1.15 GeV/c2(0.99 <
MKK <1.07 GeV/c2) o K
∗0(φ). The wid hs o he K∗0and
φa e ixed o hei PDG alues (K∗0)=47.4 ±0.6 MeV/c2,
(φ)=4.26 ±0.04 MeV/c2[67], whe eas he esolu ion
pa ame e o he Voig ian unc ion o φis kep as a ee pa-
ame e . The measu ed esolu ion o he φmass as a unc ion
o pT(σo Gaussian) a ies be ween 1 and 3 MeV/c2.The
sensi i i y o he choice o he i ing ange, he no maliza ion
in e al, he shape o he backg ound unc ion, he wid h and
esolu ion pa ame e s ha e been s udied by a ying he de aul
se ings, as desc ibed in Sec. II D. In minimum bias collisions,
K∗0(φ) p oduc ion is measu ed in he pT ange om 0 o 20
GeV/c(0.4 o16GeV/c). Wi h he a ailable da a samples,
K∗0p oduc ion is measu ed up o pT=15 GeV/c in 0–5%
and 5–10%, up o pT=20 GeV/c in 10–20%, 20–40%, and
40–60%, up o 10 GeV/c in 60–80% and up o 6 GeV/c
in 80–100% mul iplici y classes, while he φp oduc ion is
measu ed up o pT=16 GeV/c in 0–5%, 5–10%, 10–20%,
20–40%, pT=12 GeV/c in 40–60%, pT=10 GeV/cin
60–80%, and pT=6GeV/c in 80–100% mul iplici y class.
The aw ans e se momen um dis ibu ions a e no mal-
ized by he numbe o accep ed e en s and co ec ed o he
b anching a io, de ec o accep ance and econs uc ion e i-
ciency (A× ec) and, signal loss. The co ec ion ac o due o
he e ex econs uc ion e iciency is negligible in all mul i-
plici y classes. The A× ec is ob ained om he Mon e Ca lo
simula ion (MC) based on he DPMJET [32] e en gene a o
and he in e ac ion o he gene a ed pa icles passing h ough
he ALICE de ec o geome y is modeled using GEANT3
[68]. I is de ined as he a io o he econs uc ed K∗0(φ) o
he gene a ed K∗0(φ), bo h in he apidi y in e al −0.5 <y<
0, and de e mined as a unc ion o pT. The same ack and pa -
icle iden i ica ion (PID) selec ion c i e ia a e applied o he
decay daugh e o esonances in MC as a e used in he anal-
ysis. The shape o he gene a ed pTdis ibu ions a e di e en
om he measu ed pTdis ibu ions, he e o e a e-weigh ing
p ocedu e is used, in which he gene a ed dis ibu ions a e
weigh ed o ma ch he measu ed dis ibu ions. The e ec o
he eweigh ing p ocedu e on A× ec is ≈2–5% a low pT
(<1GeV/c) and negligible o pT>1GeV/c. The eweigh ed
A× ec is used o co ec he awpTdis ibu ion. No signi i-
can mul iplici y dependence o A× ec is obse ed, he e o e
he aw pTspec a in he a ious mul iplici y classes a e co -
ec ed wi h he minimum bias A× ec alues. The signal loss
co ec ions ha accoun o he loss in K∗0and φyields caused
055201-4

K∗(892)0AND φ(1020) PRODUCTION IN p-Pb COLLISIONS … PHYSICAL REVIEW C 107, 055201 (2023)
TABLE II. The sou ces o sys ema ic unce ain ies o K∗0and φ
yields in p-Pb collisions a √sNN =8.16 TeV. Fo each sou ce, he
a e age unce ain ies a e lis ed o he low and high-pTin e als.
K∗0φ
pT(GeV/c)
Sys ema ic a ia ion 0.0–4.0 4.0–20.0 0.4–4.0 4.0–16.0
Yield ex ac ion (%) 7.5 8.0 2.8 4.5
T ack selec ion (%) 3.0 2.0 4.4 5.5
Pa icle iden i ica ion (%) 4.3 5.0 1.9 3.5
Global acking e iciency (%) 2.0 3.2 2.0 2.3
Ma e ial budge (%) 1.2 <0.5 2.2 <0.5
Had onic In e ac ion (%) 1.9 <0.5 2.4 <1
To al (%) 9.6 10.2 6.7 8.3
by he e en selec ion wi h minimum bias igge , a he han
all NSD e en s, a e ound o be negligible in he measu ed
pT ange. The minimum bias pTspec a a e no malized o he
ac ion o NSD e en s, which is 0.992.
D. Sys ema ic unce ain ies
The sou ces o sys ema ic unce ain ies o he measu e-
men o K∗0and φp oduc ion a e signal ex ac ion, ack
selec ion c i e ia, pa icle iden i ica ion, global acking e -
iciency, unce ain y in he ma e ial budge o he ALICE
de ec o and he had onic in e ac ion c oss-sec ion in he de-
ec o ma e ial. A simila app oach is adop ed as used o he
sys ema ic unce ain y s udy o K∗0and φin p-Pb collisions
a √sNN =5.02 TeV [23]. No mul iplici y dependence o
he sys ema ic e ec s is obse ed, he e o e he sys ema ic
unce ain ies o minimum bias pTspec a a e p opaga ed o
all mul iplici y e en classes s udied. A summa y o sys em-
a ic unce ain ies o K∗0(φ) in wo ans e se momen um
in e als, 0 <pT<4GeV/c(0.4<pT<4GeV/c) and
4<pT<20 GeV/c(4<pT<16 GeV/c) a e gi en in
Table II. The unce ain ies due o signal ex ac ion include
a ia ions o he signal peak i ing ange, a ia ions o wid h
and mass esolu ion, mixed-e en backg ound no maliza ion
egion, choice o esidual backg ound unc ion, and combina-
o ial backg ound. The i ing ange o he πK (KK) in a ian
mass dis ibu ion is a ied by ≈50 (5) MeV/c2on each side
o he signal peak. The no maliza ion ange o he πK (KK)
in a ian mass dis ibu ions di e ed by app oxima ely 150
(50) MeV/c2wi h espec o he de aul alue. The wid h o
he esonances is ixed o he de aul i whe eas i is kep
ee o sys ema ic s udies. The esidual backg ound is i ed
wi h a i s -o de and hi d-o de polynomial unc ion o he
sys ema ic s udies o he signal ex ac ion. Fo φ esonance,
he e ec o he a ia ion o he esolu ion pa ame e (σo
he Gaussian) on he yield is also included in he sys ema ic
unce ain ies. The combina o ial backg ound om he like-
sign me hod is used o sys ema ic s udies. The con ibu ion o
sys ema ic unce ain ies due o he signal ex ac ion is 7.5–8%
o K∗0and 2.8–4.5% o φ. The sys ema ic e ec s due o
he cha ged ack selec ion a e s udied by a ying he c i e ia
based on he numbe o c ossed eadou ows in he TPC and
he dis ance o closes app oach o he p ima y e ex o he
collision [65]. The ela i e con ibu ion o unce ain ies due o
he ack selec ion a e 2–3% o K∗0and abou 4.4–5.5% o
he φ. Fo he PID sys ema ic unce ain y, he selec ions based
on he TPC dE/dx and TOF ime-o - ligh a e a ied. Th ee
a ia ions a e aken whe e one is a momen um dependen
PID selec ion o 5σTPC (0 <p<0.3), 2.5σTPC (0.3 <p
<0.5), 1.5σTPC (p>0.5) wi h 3σTOF, and wo momen um-
independen selec ion; 2σTPC wi h 3σTOF and 2σTPC only, o
bo h K∗0and φ. This esul s in sys ema ic unce ain ies o
4.3–5% o K∗0and 1.9–3.5% o he φ. The unce ain y
ela ed o global acking a ises om he di e ence in he
ITS-TPC ack ma ching e iciency in da a and MC. I is
es ima ed om he single cha ged ack unce ain y by aking
he linea sum o he unce ain ies o he wo cha ged acks
which a e used o econs uc he esonances. I con ibu es
o he sys ema ic unce ain ies wi h 2–3.2% and 2–2.3% o
K∗0and φ, espec i ely. The ma e ial budge sys ema ic e -
ec s accoun o he unce ain ies in he es ima ion o he
ALICE de ec o ma e ial budge and is es ima ed o be 1.2%
o K∗0and 2.2% o φa low pT. I is negligible a pT
>4GeV/c o bo h K∗0and φ. The sys ema ic unce ain y
due o he had onic in e ac ion c oss-sec ion in he de ec o
ma e ial is es ima ed o be 1.9% o K∗0and 2.4% o φ
a low pT, and negligible o pT>4GeV/c. The e ec s
o ma e ial budge and had onic in e ac ion a e e alua ed by
combining he unce ain ies o he wo cha ged acks (π,K
o K∗0and wo K o φ) acco ding o he kinema ics o he
decay. The sys ema ic unce ain ies o he ma e ial budge
and he had onic in e ac ion c oss-sec ion we e aken om
Re . [23]. The o al sys ema ic unce ain y is aken as he
quad a ic sum o all con ibu ions and a ies as 9.6–10.2%
o K∗0and 6.7–8.3% o φ. The sou ces o sys ema ic un-
ce ain ies ha a e mul iplici y-dependen and unco ela ed
ac oss di e en mul iplici y classes a e also es ima ed. The
sys ema ic unce ain ies due o signal ex ac ion and PID a e
ully unco ela ed, whe eas global acking, ack selec ion
c i e ia, ma e ial budge and had onic c oss-sec ion a e co -
ela ed among e en mul iplici y classes.
III. RESULTS AND DISCUSSION
A. T ans e se momen um spec a
The measu emen o K∗0(φ) p oduc ion pe o med in he
apidi y in e al −0.5 <y<0up opT=20 (16) GeV/c
in p-Pb collisions a √sNN =8.16 TeV is epo ed. Figu e 2
shows pTspec a o K∗0(le panel) and φ( igh panel)
o NSD e en s. These a e compa ed wi h he p edic ions
om EPOS-LHC [31,69], DPMJET [32], and HIJING [33]
models. The bo om panels o Fig. 2show he a ios o pT
spec a om hese models o he da a. The EPOS Mon e Ca lo
e en gene a o is a had onic in e ac ion pa on model based
on G ibo ’s Reggeon ield heo y o malism which includes
he ea u e o collec i e had oniza ion and he co e-co ona
mechanism om pp o A-A collisions [70–72]. I he s ing
segmen s o he inal s a e pa on ha e high-ene gy densi y,
hen ha egion is known as he “co e,” whe eas he e-
gion wi h s ings o low-ene gy densi y su ounding he co e
055201-5
S. ACHARYA e al. PHYSICAL REVIEW C 107, 055201 (2023)
FIG. 2. Top panels: T ans e se momen um spec um o K∗0(le ) and φ( igh ) as a unc ion o pT o he NSD e en s, measu ed in he
apidi y in e al −0.5 <y<0 o p-Pb collisions a √sNN =8.16 TeV. The s a is ical and sys ema ic unce ain ies a e shown as ba s and
boxes, espec i ely. The NSD spec um is compa ed wi h he p edic ions om EPOS-LHC [31,69], DPMJET [32], and HIJING [33]. Bo om
panels: The a ios o pTspec a om model o da a. The shaded bands a ound uni y desc ibe he s a is ical and sys ema ic unce ain ies o he
da a poin .
is called he “co ona.” The co e e ol es hyd odynamically
and subsequen ly had onizes o o m he bulk o he sys em
whe eas he s ings in he co ona egion b eak h ough he
p oduc ion o qua k-an iqua k pai s, which had onize as ag-
men a ion p ocesses in acuum. EPOS-LHC [31] is a une
o EPOS1.99 [73] ha inco po a es a pa ame iza ion o low
based on LHC da a. The EPOS1.99 model is di e en om
EPOS2.x [74] and EPOS3.x [69] as i does no use he com-
ple e 3D hyd o calcula ion ollowed by he had onic cascade
bu ins ead elies on he as co a ian app oach. I desc ibes
a ious obse ables in minimum bias hea y-ion collisions
as well as small collision sys ems up o a ew GeV/ca
LHC ene gies. DPMJET is a QCD-inspi ed dual pa on model
based on he G ibo -Glaube app oach ha ea s he so
and ha d sca e ing in e ac ion p ocesses di e en ly. HIJING
combines he pe u ba i e QCD p ocess wi h so exci a ion,
he p oduc ion o mul iple minije s, he in e ac ions o je s
in dense had onic ma e , and nuclea shadowing o pa on
dis ibu ion unc ions. Fo he K∗0 esonance, a low pT(<1
GeV/c), DPMJET and HIJING models o e es ima e he da a,
whe eas EPOS-LHC model gi es a good desc ip ion o he
pTspec um. A pT>1GeV/c, DPMJET and EPOS-LHC
unde es ima e and close o he da a, howe e HIJING model
unde es ima es (simila o he DPMJET and EPOS-LHC) o
1<pT<5GeV/c and o e es ima es o pT>5GeV/c.
The EPOS-LHC model desc ibes he φpTspec um ela i ely
be e han he DPMJET and HIJING o all pT. Howe e ,
HIJING model gi es a good desc ip ion o pTdis ibu on
o φ esonance o pT>6GeV/c. The EPOS-LHC model,
whe e a di e en pa ame iza ion o low is in oduced in
small collision sys ems like pp han he la ge olume p o-
duced in hea y-ion collisions, gi es a be e desc ip ion o
he ans e se momen um dis ibu ions o bo h K∗0and
φin p-Pb collisions. Figu e 3shows he √sNN dependence
o he ans e se momen um spec a o K∗0and φ o NSD
e en s in p-Pb collisions. The uppe panels o Fig. 3show a
compa ison o he ans e se momen um spec a o K∗0and φ
a √sNN =5.02 and 8.16 TeV, whe eas he lowe panels show
he a io o he pT-di e en ial yield a √sNN =8.16 o 5.02
TeV and i s compa ison wi h he esul s ob ained om models
[31–33,69]. The unce ain ies o he a ios a e ob ained as he
sum in quad a u e o he unce ain ies o he spec a a he wo
ene gies, which a e la gely unco ela ed. Up o pT1GeV/c,
he di e en ial yield a io seems o independen o pTand
collision ene gy. The alues a e consis en wi h uni y wi hin
unce ain ies. I sugges s ha he pa icle p oduc ion in he
so sca e ing egion is no s ongly dependen on collision
ene gy. The di e en ial yield a ios inc eases as a unc ion
o pT o pT1GeV/c. Simila beha io is also obse ed
in pp collisions in Re . [21]. The pTdi e en ial yield a ios
055201-6
K∗(892)0AND φ(1020) PRODUCTION IN p-Pb COLLISIONS … PHYSICAL REVIEW C 107, 055201 (2023)
FIG. 3. Top panels: Ene gy dependence compa ison o he ans e se momen um spec a o K∗0(le ) and φ( igh ) as a unc ion o pT o
he NSD e en s, measu ed in he apidi y in e al −0.5 <y<0 o p-Pb collisions a √sNN =5.02 and 8.16 TeV. Bo om panels: The a io
o pTspec um a √sNN =8.16 TeV o he pTspec um a √sNN =5.02 TeV. The a io is compa ed wi h he p edic ions om EPOS-LHC
[31,69], DPMJET [32], and HIJING [33]. The s a is ical and sys ema ic unce ain ies a e shown as ba s and boxes, espec i ely.
ob ained om EPOS-LHC, DPMJET, and HIJING a e
consis en wi h he measu emen s wi hin he sys ema ic unce -
ain ies and ep oduce well he ene gy dependence end o
K∗0and φin p-Pb collisions. Figu e 4shows he ans e se
momen um dis ibu ions o K∗0(le panel) and φ( igh panel)
in a ious mul iplici y classes. The a ios o pTspec a in a i-
ous mul iplici y classes o he pTspec um o NSD e en s a e
shown in he bo om panels o Fig. 4.Fo pT4GeV/c, he
slopes o he pTspec a inc ease om low o high mul iplici y
classes, whe eas he spec al shapes a e simila a high pT
o all mul iplici y classes. This indica es ha p ocesses like
adial low, which lead o a change in he shape o he pT
spec a o a ious mul iplici y classes, domina e mainly a
low pT[36]. The inc ease in he slope o pTspec um wi h
mul iplici y is e lec ed in Fig. 5 o pTas a unc ion o
mul iplici y. A simila beha io was also obse ed o K∗0and
φin p-Pb collisions [23]a √sNN =5.02 TeV. The ha dening
o he pTspec a wi h cha ged pa icle mul iplici y was also
epo ed o inclusi e cha ged had on spec a, π,K,p,K
0
S,
,, and in pp collisions a LHC ene gies [20,22,34,75],
whe e di e en models wi h mul ipa on in e ac ions we e
shown o desc ibe hese e ec s.
B. In eg a ed pa icle yield and mean ans e se momen um
The pT-in eg a ed yields and mean ans e se momen um
a e ex ac ed om ans e se momen um spec a in he mea-
su ed ange and using he i unc ion in he unmeasu ed
egion. The φyield is ex apola ed in he unmeasu ed e-
gion (pT<0.4 GeV/c) by i ing a Lé y-Tsallis unc ions
[76] o he measu ed pTspec a in all mul iplici y classes.
The di e ence in he yield con ibu ion a low pTdue o
di e en i ing unc ions (i.e., exponen ial, Bol zmann, mT-
exponen ial, Bose-Eins ein and Bol zmann-Gibbs Blas -Wa e
unc ion in Re . [46]) om he Lé y-Tsallis unc ion is
included in he sys ema ic unce ain ies. The low-pTex apo-
la ion accoun s o 8.9% (14.1%) o he o al yield in he 0–5%
(80–100%) mul iplici y class. The K∗0spec a a e measu ed
om pT=0, so low-pTex apola ion is no needed. The
con ibu ion o he ex apola ed ac ion o he yield is negli-
gible o pT>20 GeV/c(16GeV/c) o K∗0(φ). The alues
o dN/dy and pTo K∗0and φ o a ious mul iplici y
classes a e summa ized in he Table III. The mul iplici y-
scaled in eg a ed yields [(dN/dy)/(dNch/dη|η|<0.5)] o K∗0
and φa e shown in he uppe panels o Fig. 5as a unc ion
o dNch/dη|η|<0.5. These esul s a e compa ed wi h o he
ALICE measu emen s in pp collisions a √s=7 and 13 TeV
[20,22], in p-Pb collisions a √sNN =5.02 TeV [23], and in
Pb-Pb collisions a √sNN =2.76 and 5.02 TeV [15,18,19].
The scaled in eg a ed yields e ol e smoo hly as a unc ion o
mul iplici y om pp,p-Pb o Pb-Pb collisions. Fo simila
dNch/dη|η|<0.5, hese alues a e consis en wi hin unce -
ain ies o di e en colliding sys ems and a a ious LHC
ene gies. This indica es ha e en mul iplici y d i es he es-
onance p oduc ion, i espec i e o he colliding sys ems and
ene gies [20,22,23].
The scaled in eg a ed yields o φshow a sligh inc ease
wi h mul iplici y om pp collisions o mid-cen al Pb-Pb
055201-7
S. ACHARYA e al. PHYSICAL REVIEW C 107, 055201 (2023)
FIG. 4. Top panels: The ans e se momen um spec a o K∗0(le ) and φ( igh ) o a ious mul iplici y classes, measu ed in he apidi y
in e al −0.5<y<0 o p-Pb collisions a √sNN =8.16 TeV. Bo om panels: The a ios o pTspec a o gi en e en mul iplici y classes o
he NSD spec a a e shown. The s a is ical and sys ema ic unce ain ies a e shown as ba s and boxes, espec i ely.
collisions. The o al inc ease is 12% wi h a 1.5σsigni i-
cance be ween he lowes mul iplici y bin and he highes
mul iplici y bin in p-Pb collisions a √sNN =8.16 TeV. Sim-
ila ly scaled in eg a ed yields o K∗0show a sligh dec ease
wi h mul iplici y o all h ee collision sys ems and he o al
dec ease is 12% wi h a 1.8σsigni icance o p-Pb collisions
a √sNN =8.16 TeV. The signi icance is calcula ed using s a-
is ical and mul iplici y unco ela ed sys ema ic unce ain ies,
added in quad a u e. The in eg a ed yield a ios o esonances
ela i e o hose o longe li ed pa icles, π, K, and pa e
compu ed o s udy hei p oduc ion mechanism. The K∗0/K
(φ/π) a io measu ed in p-Pb collisions a √sNN =5.02
TeV [23] shows a dec easing (inc easing) end going om
he lowes mul iplici y o he highes mul iplici y bin wi h a
signi icance o 2.6σ(1.5σ) which is discussed in he con ex
o a hin o a e-sca e ing (s angeness enhancemen ) e ec .
Fu u e measu emen s o πand K yields in p-Pb collisions
a √sNN =8.16 TeV will be use ul o s udy hese e ec s
a highe cen e -o -mass ene gy and up o la ge mul iplic-
i y. The model compa ison wi h he p-Pb da a shows ha
EPOS-LHC desc ibes he scaled in eg a ed yields o bo h
K∗0and φwhe eas HIJING o e es ima es he da a o all
mul iplici ies. The DPMJET model desc ibes he scaled in-
eg a ed yield o φa highe mul iplici ies bu o e es ima es
he K∗0a all mul iplici ies. The pTexhibi s an inc easing
end as a unc ion o dNch/dη|η|<0.5 o K∗0and φin a ious
colliding sys ems and ene gies as shown in he bo om panels
o Fig 5. The inc ease in pTis as e o pp and p-Pb han
Pb-Pb and o a common mul iplici y co e age he alues
o pTin pp and p-Pb a e la ge han Pb-Pb. A simila
mul iplici y (dNch/dη|η|<0.5≈40), he di e ence in pT
alues among Pb-Pb, p-Pb and pp collisions indica e ha he
geome y and dynamics o he collision sys ems a e di e en ,
while he scaled in eg a ed yields o K∗0and φa e simila
o all colliding sys ems and ene gies. This indica es ha he
high mul iplici y e en sample in small collision sys ems has
a dominan ly la ge ac ion o ha de e en s.
Simila s udies a e epo ed in Re s. [23,77], whe e he
mode a e inc ease o pTin Pb-Pb collisions was e-
la ed o collec i e low. The s ong inc ease o pTwi h
dNch/dη|η|<0.5in small collision sys ems can be u he
in es iga ed by sys ema ic s udies o pT om di e en mod-
els in pp and p-Pb collisions ha inco po a e p ocesses like
colo econnec ion, be ween s ings p oduced in mul ipa on
in e ac ions, di e en s ing agmen a ion p ocesses and he
co e-co ona mechanism. I was obse ed in Re . [22] ha
he PYTHIA8 model wi h colo econnec ion, which in o-
duces a lowlike e ec , and he EPOS-LHC model, which
uses pa ame e ized low, a e able o ep oduce he inc easing
end o pTas a unc ion o mul iplici y o K∗0and φin
pp collisions a √s=13 TeV. The p-Pb measu emen s a e
impo an , as in Re . [77] i is shown ha he pTo cha ged
had ons as a unc ion o mul iplici y shows a simila beha io
as in pp collisions a low mul iplici y, whe eas i seems o
app oach a simila bu less p ominen end o sa u a ion as in
Pb-Pb collisions a high mul iplici y.
The model compa ison wi h p-Pb da a shows ha EPOS-
LHC desc ibes he inc easing end o pTwi h mul iplici y
055201-8
K∗(892)0AND φ(1020) PRODUCTION IN p-Pb COLLISIONS … PHYSICAL REVIEW C 107, 055201 (2023)
ans e se momen um in p-Pb collisions a √sNN =5.02 TeV,
Phys. Le . B 760, 720 (2016).
[27] J. Adam e al. (ALICE Collabo a ion), Mul i-s ange ba yon
p oduc ion in p-Pb collisions a √sNN =5.02 TeV, Phys. Le .
B758, 389 (2016).
[28] S. Acha ya e al. (ALICE Collabo a ion), Measu emen o
(1520) p oduc ion in pp collisions a √s=7 TeV and p-
Pb collisions a √sNN =5.02 TeV, Eu . Phys. J. C 80, 160
(2020).
[29] D. Adamo a e al. (ALICE Collabo a ion), P oduc ion o
(1385)±and (1530)0in p-Pb collisions a √sNN =
5.02 TeV, Eu .Phys.J.C77, 389 (2017).
[30] B. B. Abele e al. (ALICE Collabo a ion), P oduc ion o
(1385)±and (1530)0in p o on-p o on collisions a √s=
7 TeV, Eu .Phys.J.C75, 1 (2015).
[31] T. Pie og, I. Ka penko, J. M. Ka zy, E. Ya senko, and K.
We ne , EPOS LHC: Tes o collec i e had oniza ion wi h da a
measu ed a he CERN La ge Had on Collide , Phys. Re . C 92,
034906 (2015).
[32] S. Roesle , R. Engel, and J. Ran , The Mon e Ca lo e en
gene a o DPMJET-III, in Ad anced Mon e Ca lo o Radia ion
Physics, Pa icle T anspo Simula ion and Applica ions, edi ed
by A. Kling, F. J. C. Ba äo, M. Nakagawa, L. Tá o a, and P. Vaz
(Sp inge , Be lin, Heidelbe g, 2001), pp. 1033–1038.
[33] M. Gyulassy and X.-N. Wang, HIJING 1.0: A Mon e Ca lo
p og am o pa on and pa icle p oduc ion in high-ene gy
had onic and nuclea collisions, Compu . Phys. Commun. 83,
307 (1994).
[34] S. Acha ya e al. (ALICE Collabo a ion), Mul iplici y depen-
dence o (mul i)s ange had on p oduc ion in p o on-p o on
collisions a √s=13 TeV, Eu . Phys. J. C 80, 167 (2020).
[35] B. Abele e al. (ALICE Collabo a ion), Cen ali y dependence
o π,K,pp oduc ion in Pb-Pb collisions a √sNN =2.76 TeV,
Phys. Re . C 88, 044910 (2013).
[36] S. Acha ya e al. (ALICE Collabo a ion), P oduc ion o cha ged
pions, kaons, and (an i)p o ons in Pb-Pb and inelas ic pp
collisions a √sNN =5.02 TeV, Phys.Re .C101, 044907
(2020).
[37] J. C. Collins, D. E. Sope , and G. F. S e man, Fac o iza ion o
ha d p ocesses in QCD, Ad . Se . Di ec . High Ene gy Phys. 5,
1 (1989).
[38] D. de Flo ian, R. Sasso , M. Epele, R. J. He nández-Pin o, and
M. S a mann, Pa on- o-pion agmen a ion eloaded, Phys.
Re . D 91, 014035 (2015).
[39] S. J. B odsky, H. J. Pi ne , and J. Rau eisen, Scaling p ope ies
o high pTinclusi e had on p oduc ion, Phys. Le . B 637,58
(2006).
[40] F. A leo, S. J. B odsky, D. S. Hwang, and A. M. Sickles,
Highe -Twis Dynamics in La ge T ans e se Momen um
Had on P oduc ion, Phys.Re .Le .105, 062002 (2010).
[41] T. Aal onen e al. (CDF Collabo a ion), Measu emen o pa -
icle p oduc ion and inclusi e di e en ial c oss sec ions in p¯p
collisions a √s=1.96 TeV, Phys. Re . D 79, 112005 (2009);
82, 119903(E) (2010).
[42] D. Acos a e al. (CDF Collabo a ion), So and ha d in e ac ions
in p¯pcollisions a √s=1800 and 630 GeV, Phys. Re . D 65,
072005 (2002).
[43] F. Abe e al. (CDF Collabo a ion), T ans e se Momen um
Dis ibu ions o Cha ged Pa icles P oduced in ¯pp In e ac-
ions a √s=630 and 1800 GeV, Phys. Re . Le . 61, 1819
(1988).
[44] C. Albaja e al. (UA1 Collabo a ion), A s udy o he gene al
cha ac e is ics o p¯pcollisions a √s=0.2 o 0.9 TeV, Nucl.
Phys. B 335, 261 (1990).
[45] J. Adams e al. (STAR Collabo a ion), Iden i ied had on
spec a a la ge ans e se momen um in p+pand d+Au
collisions a √sNN =200 GeV, Phys. Le . B 637, 161
(2006).
[46] S. Acha ya e al. (ALICE Collabo a ion), P oduc ion o ligh -
la o had ons in pp collisions a √s=7and√s=13 TeV,
Eu . Phys. J. C 81, 256 (2021).
[47] S. Cha chyan e al. (CMS Collabo a ion), Cha ged pa icle
ans e se momen um spec a in pp collisions a √s=0.9and
7 TeV, J. High Ene g. Phys. 08 (2011) 086.
[48] S. Acha ya e al. (ALICE Collabo a ion), T ans e se mo-
men um spec a and nuclea modi ica ion ac o s o cha ged
pa icles in pp,p-Pb, and Pb-Pb collisions a he LHC, J. High
Ene g. Phys. 11 (2018) 013.
[49] A. M. Si unyan e al. (CMS Collabo a ion), S ange had on
p oduc ion in ppand pPb collisions a √sNN =5.02 TeV, Phys.
Re . C 101, 064906 (2020).
[50] V. Khacha yan e al. (CMS Collabo a ion), Mul iplici y and
apidi y dependence o s ange had on p oduc ion in pp,pPb,
and PbPb collisions a he LHC, Phys. Le . B 768, 103
(2017).
[51] B. B. Abele e al. (ALICE Collabo a ion), Mul iplici y De-
pendence o Pion, Kaon, P o on and lambda p oduc ion in
p-Pb collisions a √sNN =5.02 TeV, Phys. Le . B 728,25
(2014).
[52] T. Sjös and, S. Ask, J. R. Ch is iansen, R. Co ke, N. Desai, P.
Il en, S. M enna, S. P es el, C. O. Rasmussen, and P. Z. Skands,
An in oduc ion o PYTHIA 8.2, Compu . Phys. Commun. 191,
159 (2015).
[53] S. Acha ya e al. (ALICE Collabo a ion), Nuclea modi ica ion
ac o o ligh neu al-meson spec a up o high ans e se mo-
men um in p-Pb collisions a √sNN =8.16 TeV, Phys. Le . B
827, 136943 (2022).
[54] R. J. F ies, B. Mulle , C. Nonaka, and S. A. Bass, Had oniza ion
in Hea y-Ion Collisions: Recombina ion and F agmen a ion o
Pa ons, Phys.Re .Le .90, 202303 (2003).
[55] Z.-B. Kang, I. Vi e , and H. Xing, Nuclea modi ica ion
o high ans e se momen um pa icle p oduc ion in p+A
collisions a RHIC and LHC, Phys. Le . B 718, 482
(2012).
[56] B. Z. Kopelio ich, J. Nemchik, A. Scha e , and A. V. Ta aso ,
C onin E ec in Had on P oduc ion o Nuclei, Phys. Re . Le .
88, 232303 (2002).
[57] J. W. C onin, H. J. F isch, M. J. Shoche , J. P. Boymond, P. A.
Pi oue, and R. L. Sumne , P oduc ion o Had ons wi h La ge
T ans e se Momen um a 200 and 300 GeV, Phys. Re . Le .
31, 1426 (1973).
[58] J. W. C onin, H. J. F isch, M. J. Shoche , J. P. Boymond, R.
Me mod, P. A. Pi oue, and R. L. Sumne , P oduc ion o had ons
wi h la ge ans e se momen um a 200, 300, and 400 GeV,
Phys.Re .D11, 3105 (1975).
[59] K. Aamod e al. (ALICE Collabo a ion), The ALICE expe i-
men a he CERN LHC, JINST 3, S08002 (2008).
[60] B. Abele e al. (ALICE Collabo a ion), Pe o mance o he
ALICE expe imen a he CERN LHC, In . J. Mod. Phys. A
29, 1430044 (2014).
[61] E. Abbas e al. (ALICE Collabo a ion), Pe o mance o he
ALICE VZERO sys em, J. Ins . 8, P10016 (2013).
055201-15

S. ACHARYA e al. PHYSICAL REVIEW C 107, 055201 (2023)
[62] S. Acha ya e al. (ALICE Collabo a ion), Cha ged-pa icle
pseudo apidi y densi y a mid- apidi y in p-Pb collisions a
√sNN =8.16 TeV, Eu .Phys.J.C79, 307 (2019).
[63] K. Aamod e al. (ALICE Collabo a ion), Alignmen o he
ALICE inne acking sys em wi h cosmic- ay acks, JINST
5, P03003 (2010).
[64] J. Alme e al., The ALICE TPC, a la ge 3-dimensional acking
de ice wi h as eadou o ul a-high mul iplici y e en s, Nucl.
Ins um. Me hods Phys. Res., Sec . A 622, 316 (2010).
[65] J. Adam e al. (ALICE Collabo a ion), Measu emen o pion,
kaon, and p o on p oduc ion in p o on–p o on collisions a
√s=7 TeV, Eu .Phys.J.C75, 226 (2015).
[66] A. Akindino e al., Pe o mance o he ALICE Time-O -Fligh
de ec o a he LHC, Eu .Phys.J.Plus128, 44 (2013).
[67] M. Tanabashi e al. (Pa icle Da a G oup Collabo a ion), Re-
iew o Pa icle Physics, Phys.Re .D98, 030001 (2018).
[68] R. B un, F. B uyan , M. Mai e, A. C. McPhe son, and P.
Zana ini, GEANT 3: Use ’s guide Gean 3.10, Gean 3.11;
e . e sion (CERN, Gene a, 1987), h ps://cds.ce n.ch/ eco d/
1119728.
[69] K. We ne , B. Guio , I. Ka penko, and T. Pie og, Analyzing
adial low ea u es in p-Pb and p-pcollisions a se e al TeV by
s udying iden i ied-pa icle p oduc ion wi h he e en gene a o
EPOS3, Phys.Re .C89, 064903 (2014).
[70] K. We ne , I. Ka penko, M. Bleiche , and T. Pie og, The physics
o EPOS, EPJ Web Con . 52, 05001 (2013).
[71] H. J. D esche , M. Hladik, S. Os apchenko, T. Pie og, and K.
We ne , Pa on-based G ibo -Regge heo y, Phys. Rep. 350,93
(2001).
[72] K. We ne , Co e-Co ona Sepa a ion in Ul a ela i is ic Hea y
Ion Collisions, Phys. Re . Le . 98, 152301 (2007).
[73] T. Pie og and K. We ne , EPOS model and ul a high ene gy
cosmic ays, Nucl. Phys. B, P oc. Suppl. 196, 102 (2009).
[74] K. We ne , I. Ka penko, T. Pie og, M. Bleiche , and K.
Mikhailo , E en -by-e en simula ion o he h ee-dimensional
hyd odynamic e olu ion om lux ube ini ial condi ions in
ul a ela i is ic hea y ion collisions, Phys.Re .C82, 044904
(2010).
[75] S. Acha ya e al. (ALICE Collabo a ion), Cha ged-pa icle p o-
duc ion as a unc ion o mul iplici y and ans e se sphe oci y
in pp collisions a √s=5.02 and 13 TeV, Eu .Phys.J.C79,
857 (2019).
[76] C. Tsallis, Possible gene aliza ion o Bol zmann-Gibbs s a is-
ics, J. S a . Phys. 52, 479 (1988).
[77] B. Abele e al. (ALICE Collabo a ion), Mul iplici y depen-
dence o he a e age ans e se momen um in pp,p-Pb,
and Pb-Pb collisions a he LHC, Phys. Le . B 727, 371
(2013).
[78] C. Loizides, J. Kamin, and D. d’En e ia, Imp o ed
Mon e Ca lo Glaube p edic ions a p esen and
u u e nuclea collide s, Phys.Re .C97, 054910
(2018);99, 019901(E) (2019).
[79] B. Abele e al. (ALICE Collabo a ion), Mul i-s ange ba yon
p oduc ion a mid- apidi y in Pb-Pb collisions a √sNN =2.76
TeV, Phys. Le . B 728, 216 (2014);734, 314(E) (2014).
[80] B. Abele e al. (ALICE Collabo a ion), Mul i-s ange ba yon
p oduc ion in pp collisions a √s=7 TeV wi h ALICE, Phys.
Le . B 712, 309 (2012).
S. Acha ya,142 D. Adamo á,97 A. Adle ,75 J. Adol sson,82 G. Aglie i Rinella,34 M. Agnello,30 N. Ag awal,54 Z. Ahammed,142
S. Ahmad,16 S. U. Ahn,77 I. Ahuja,38 Z. Akba ,51 A. Akindino ,94 M. Al-Tu any,109 S. N. Alam,16 D. Aleksand o ,90
B. Alessand o,60 H. M. Al anda,7R. Al a o Molina,72 B. Ali,16 Y. Ali,14 A. Alici,25 N. Alizadeh andchali,126 A. Alkin,34
J. Alme,21 T. Al ,69 I. Al sybee ,114 M. N. Anaam,7C. And ei,48 D. And eou,92 A. And onic,145 M. Angele i,34
V. Anguelo ,106 F. An ino i,57 P. An onioli,54 C. Anuj,16 N. Apadula,81 L. Aphece che,116 H. Appelshäuse ,69 S. A celli,25
R. A naldi,60 I. C. A sene,20 M. A slandok,147 A. Augus inus,34 R. A e beck,109 S. Aziz,79 M. D. Azmi,16 A. Badalà,56
Y. W. Baek,41 X. Bai,130,109 R. Bailhache,69 Y. Bailung,50 R. Bala,103 A. Balbino,30 A. Baldisse i,139 B. Balis,2D. Bane jee,4
R. Ba be a,26 L. Ba ioglio,107 M. Ba lou,86 G. G. Ba na öldi,146 L. S. Ba nby,96 V. Ba e ,136 C. Ba els,129 K. Ba h,34
E. Ba sch,69 F. Ba u aldi,27 N. Bas id,136 S. Basu,82 G. Ba igne,116 B. Ba yunya,76 D. Bau i,49 J. L. Bazo Alba,113
I. G. Bea den,91 C. Bea ie,147 I. Beliko ,138 A. D. C. Bell Hecha a ia,145 F. Bellini,25 R. Bellwied,126 S. Beloku o a,114
V. Belyae ,95 G. Bencedi,146,70 S. Beole,24 A. Be cuci,48 Y. Be dniko ,100 A. Be dniko a,106 L. Be gmann,106 M. G. Besoiu,68
L. Be e ,34 P. P. Bhadu i,142 A. Bhasin,103 I. R. Bha ,103 M. A. Bha ,4B. Bha acha jee,42 P. Bha acha ya,22 L. Bianchi,24
N. Bianchi,52 J. Bielˇ
cík,37 J. Bielˇ
cíko á,97 J. Bie na ,119 A. Bilandzic,107 G. Bi o,146 S. Biswas,4J. T. Blai ,120 D. Blau,90,83
M. B. Blida u,109 C. Blume,69 G. Boca,28,58 F. Bock,98 A. Bogdano ,95 S. Boi,22 J. Bok,62 L. Boldizsá ,146 A. Bolozdynya,95
M. Bomba a,38 P. M. Bond,34 G. Bonomi,141,58 H. Bo el,139 A. Bo isso ,83 H. Bossi,147 E. Bo a,24 L. B a ud,69
P. B aun-Munzinge ,109 M. B egan ,122 M. B oz,37 G. E. B uno,108,33 M. D. Buckland,129 D. Budniko ,110 H. Buesching,69
S. Bu alino,30 O. Bugnon,116 P. Buhle ,115 Z. Bu helezi,73,133 J. B. Bu ,14 A. Bylinkin,128 S. A. Bysiak,119 M. Cai,27,7
H. Caines,147 A. Cali a,109 E. Cal o Villa ,113 J. M. M Camacho,121 R. S. Camacho,45 P. Came ini,23 F. D. M Canedo,122
F. Ca nesecchi,34,25 R. Ca on,139 J. Cas illo Cas ellanos,139 E. A. R Casula,22 F. Ca alano,30 C. Ceballos Sanchez,76
P. Chak abo y,49 S. Chand a,142 S. Chapeland,34 M. Cha ie ,129 S. Cha opadhyay,142 S. Cha opadhyay,111 A. Chau in,22
T. G. Cha ez,45 T. Cheng,7C. Cheshko ,137 B. Cheynis,137 V. Chiban e Ba oso,34 D. D. Chinella o,123 S. Cho,62 P. Chochula,34
P. Ch is akoglou,92 C. H. Ch is ensen,91 P. Ch is iansen,82 T. Chujo,135 C. Cicalo,55 L. Ci a elli,25 F. Cindolo,54
M. R. Ciupek,109 G. Clai,54,aJ. Cleymans,125,bF. Colama ia,53 J. S. Colbu n,112 D. Colella,53,108,33 A. Collu,81 M. Colocci,34
M. Concas,60,cG. Conesa Balbas e,80 Z. Conesa del Valle,79 G. Con in,23 J. G. Con e as,37 M. L. Coque ,139 T. M. Co mie ,98
P. Co ese,31 M. R. Cosen ino,124 F. Cos a,34 S. Cos anza,28,58 P. C oche ,136 R. C uz-To es,81 E. Cuau le,70 P. Cui,7
L. Cunquei o,98 A. Dainese,57 M. C. Danisch,106 A. Danu,68 P. Das,88 P. Das,4S. Das,4S. Dash,49 A. De Ca o,29
G. de Ca aldo,53 L. De Cilladi,24 J. de Cu eland,39 A. De Falco,22 D. De G u ola,29 N. De Ma co,60 C. De Ma in,23
055201-16
K∗(892)0AND φ(1020) PRODUCTION IN p-Pb COLLISIONS … PHYSICAL REVIEW C 107, 055201 (2023)
S. De Pasquale,29 S. Deb,50 H. F. Degenha d ,122 K. R. Deja,143 L. Dello S i o,29 W. Deng,7P. Dhankhe ,19 D. Di Ba i,33
A. Di Mau o,34 R. A. Diaz,8T. Die el,125 Y. Ding,137,7R. Di ià,34 D. U. Dixi ,19 Ø. Dju sland,21 U. Dmi ie a,64 J. Do,62
A. Dob in,68 B. Dönigus,69 A. K. Dubey,142 A. Dubla,109,92 S. Dudi,102 P. Dupieux,136 N. Dzalaio a,13 T. M. Ede ,145
R. J. Ehle s,98 V. N. Eikeland,21 F. Eisenhu ,69 D. Elia,53 B. E azmus,116 F. E colessi,25 F. E ha d ,101 A. E okhin,114
M. R. E sdal,21 B. Espagnon,79 G. Eulisse,34 D. E ans,112 S. E dokimo ,93 L. Fabbie i,107 M. Faggin,27 J. Fai e,80 F. Fan,7
A. Fan oni,52 M. Fasel,98 P. Fecchio,30 A. Feliciello,60 G. Feo ilo ,114 A. Fe nández Téllez,45 A. Fe e o,139 A. Fe e i,24
V. J. G Feuilla d,106 J. Figiel,119 S. Filchagin,110 D. Finogee ,64 F. M. Fionda,55,21 G. Fio enza,34,108 F. Flo ,126 A. N. Flo es,120
S. Foe sch,73 S. Fokin,90 E. F agiacomo,61 E. F ajna,146 U. Fuchs,34 N. Funicello,29 C. Fu ge ,80 A. Fu s,64 J. J. Gaa dhøje,91
M. Gaglia di,24 A. M. Gago,113 A. Gal,138 C. D. Gal an,121 P. Gano i,86 C. Ga aba os,109 J. R. A Ga cia,45 E. Ga cia-Solis,10
K. Ga g,116 C. Ga giulo,34 A. Ga ibli,89 K. Ga ne ,145 P. Gasik,109 E. F. Gauge ,120 A. Gau am,128 M. B. Gay Duca i,71
M. Ge main,116 P. Ghosh,142 S. K. Ghosh,4M. Giacalone,25 P. Giano i,52 P. Giubellino,109,60 P. Giubila o,27
A. M. C Glaenze ,139 P. Glässel,106 D. J. Q Goh,84 V. Gonzalez,144 L. H. González-T ueba,72 S. Go buno ,39 M. Go gon,2
L. Gö lich,119 S. Go o ac,35 V. G abski,72 L. K. G aczykowski,143 L. G eine ,81 A. G elli,63 C. G igo as,34 V. G igo ie ,95
S. G igo yan,76,1F. G osa,34,60 J. F. G osse-Oe inghaus,34 R. G osso,109 G. G. Gua diano,123 R. Gue nane,80 M. Guilbaud,116
K. Gulb andsen,91 T. Gunji,134 W. Guo,7A. Gup a,103 R. Gup a,103 S. P. Guzman,45 L. Gyulai,146 M. K. Habib,109
C. Hadjidakis,79 H. Hamagaki,84 M. Hamid,7R. Hannigan,120 M. R. Haque,143 A. Ha lende o a,109 J. W. Ha is,147
A. Ha on,10 J. A. Hasenbichle ,34 H. Hassan,98 D. Ha zi o iadou,54 P. Haue ,43 L. B. Ha ene ,147 S. T. Heckel,107 E. Hellbä ,109
H. Hels up,36 T. He man,37 E. G. He nandez,45 G. He e a Co al,9F. He mann,145 K. F. He land,36 H. Hillemanns,34
C. Hills,129 B. Hippoly e,138 B. Ho man,63 B. Hohlwege ,92 J. Hone mann,145 G. H. Hong,148 D. Ho ak,37 S. Ho nung,109
A. Ho zyk,2R. Hosokawa,15 Y. Hou,7P. H is o ,34 C. Hughes,132 P. Huhn,69 L. M. Huh a,127 C. V. Hulse,79 T. J. Humanic,99
H. Hushnud,111 L. A. Huso a,145 A. Hu son,126 J. P. Iddon,34,129 R. Ilkae ,110 H. Ilyas,14 M. Inaba,135 G. M. Innocen i,34
M. Ippoli o ,90 A. Isako ,97 T. Isido i,128 M. S. Islam,111 M. I ano ,109 V. I ano ,100 V. Izuchee ,93 M. Jablonski,2B. Jacak,81
N. Jacazio,34 P. M. Jacobs,81 S. Jadlo ska,118 J. Jadlo sky,118 S. Jaelani,63 C. Jahnke,123,122 M. J. Jakubowska,143 A. Jalo a,103
M. A. Janik,143 T. Janson,75 M. Je cic,101 O. Je ons,112 A. A. P Jimenez,70 F. Jonas,98,145 P. G. Jones,112 J. M. Jowe ,34,109
J. Jung,69 M. Jung,69 A. Junique,34 A. Jusko,112 J. Kaewjai,117 P. Kalinak,65 A. S. Kal eye ,109 A. Kalwei ,34 V. Kaplin,95
A. Ka asu Uysal,78 D. Ka a o ic,101 O. Ka a iche ,64 T. Ka a iche a,64 P. Ka czma czyk,143 E. Ka peche ,64 V. Kashyap,88
A. Kazan se ,90 U. Kebschull,75 R. Keidel,47 D. L. D Keijdene ,63 M. Keil,34 B. Ke ze ,43 Z. Khabano a,92 A. M. Khan,7
S. Khan,16 A. Khanzadee ,100 Y. Kha lo ,93,83 A. Kha un,16 A. Khun ia,119 B. Kileng,36 B. Kim,17,62 C. Kim,17 D. J. Kim,127
E. J. Kim,74 J. Kim,148 J. S. Kim,41 J. Kim,106 J. Kim,74 M. Kim,106 S. Kim,18 T. Kim,148 S. Ki sch,69 I. Kisel,39 S. Kisele ,94
A. Kisiel,143 J. P. Ki owski,2J. L. Klay,6J. Klein,34 S. Klein,81 C. Klein-Bösing,145 M. Kleine ,69 T. Klemenz,107 A. Kluge,34
A. G. Knospe,126 C. Kobdaj,117 M. K. Köhle ,106 T. Kollegge ,109 A. Kond a ye ,76 N. Kond a ye a,95 E. Kond a yuk,93
J. Konig,69 S. A. Konigs o e ,107 P. J. Konopka,34 G. Ko nako ,143 S. D. Ko yciak,2A. Ko lia o ,97 O. Ko alenko,87
V. Ko alenko,114 M. Kowalski,119 I. K álik,65 A. K a ˇ
cáko á,38 L. K eis,109 M. K i da,112,65 F. K izek,97
K. K izko a Gajdoso a,37 M. K oesen,106 M. K üge ,69 E. K yshen,100 M. K zewicki,39 V. Ku ˇ
ce a,34 C. Kuhn,138
P. G. Kuije ,92 T. Kumaoka,135 D. Kuma ,142 L. Kuma ,102 N. Kuma ,102 S. Kundu,34 P. Ku ash ili,87 A. Ku epin,64
A. B. Ku epin,64 A. Ku yakin,110 S. Kushpil,97 J. K apil,112 M. J. Kweon,62 J. Y. Kwon,62 Y. Kwon,148 S. L. La Poin e,39
P. La Rocca,26 Y. S. Lai,81 A. Lak a hok,117 M. Lamanna,34 R. Langoy,131 K. Lapidus,34 P. La iono ,34,52 E. Laudi,34
L. Lau ne ,34,107 R. La icka,115,37 T. Laza e a,114 R. Lea,141,23,58 J. Leh bach,39 R. C. Lemmon,96 I. León Monzón,121
E. D. Lesse ,19 M. Le ich,34,107 P. Lé ai,146 X. Li,11 X. L. Li,7J. Lien,131 R. Lie a a,112 B. Lim,17 S. H. Lim,17
V. Lindens u h,39 A. Lindne ,48 C. Lippmann,109 A. Liu,19 D. H. Liu,7J. Liu,129 I. M. Lo nes,21 V. Logino ,95 C. Loizides,98
P. Lonca ,35 J. A. Lopez,106 X. Lopez,136 E. López To es,8J. R. Luhde ,145 M. Luna don,27 G. Lupa ello,61 Y. G. Ma,40
A. Mae skaya,64 M. Mage ,34 T. Mahmoud,43 A. Mai e,138 M. Malae ,100 N. M. Malik,103 Q. W. Malik,20 S. K. Malik,103
L. Malinina,76,dD. Mal’Ke ich,94 D. Mallick,88 N. Mallick,50 G. Mandaglio,32,56 V. Manko,90 F. Manso,136 V. Manza i,53
Y. Mao,7G. V. Ma gaglio i,23 A. Ma go i,54 A. Ma ín,109 C. Ma ke ,120 M. Ma qua d,69 N. A. Ma in,106 P. Ma inengo,34
J. L. Ma inez,126 M. I. Ma ínez,45 G. Ma ínez Ga cía,116 S. Masciocchi,109 M. Mase a,24 A. Masoni,55 L. Massac ie ,79
A. Mas ose io,140,53 A. M. Ma his,107 O. Ma onoha,82 P. F. T Ma uoka,122 A. Ma yja,119 C. Maye ,119 A. L. Mazuecos,34
F. Mazzaschi,24 M. Mazzilli,34 M. A. Mazzoni,59,bJ. E. Mdhluli,133 A. F. Mechle ,69 Y. Melikyan,64 A. Menchaca-Rocha,72
E. Meninno,115,29 A. S. Menon,126 M. Me es,13 S. Mhlanga,125,73 Y. Miake,135 L. Michele i,60 L. C. Miglio in,137
D. L. Mihaylo ,107 K. Mikhaylo ,76,94 A. N. Mish a,146 D. Mi´
skowiec,109 A. Modak,4A. P. Mohan y,63 B. Mohan y,88
M. Mohisin Khan,16,eM. A. Molande ,44 Z. Mo a co a,91 C. Mo dasini,107 D. A. Mo ei a De Godoy,145 I. Mo ozo ,64
A. Mo sch,34 T. M nja ac,34 V. Mucci o a,52 E. Mudnic,35 D. Mühlheim,145 S. Muhu i,142 J. D. Mulligan,81 A. Mulli i,22
M. G. Munhoz,122 R. H. Munze ,69 H. Mu akami,134 S. Mu ay,125 L. Musa,34 J. Musinsky,65 J. W. My cha,143 B. Naik,133,49
R. Nai ,87 B. K. Nandi,49 R. Nania,54 E. Nappi,53 A. F. Nassi pou ,82 A. Na h,106 C. Na ass,132 A. Neagu,20 L. Nellen,70
S. V. Nesbo,36 G. Nesko ic,39 D. Nes e o ,114 B. S. Nielsen,91 S. Nikolae ,90 S. Nikulin,90 V. Nikulin,100 F. No e ini,54
S. Noh,12 P. Nomokono ,76 J. No man,129 N. No i zky,135 P. Nowakowski,143 A. Nyanin,90 J. Nys and,21 M. Ogino,84
A. Ohlson,82 V. A. Oko oko ,95 J. Oleniacz,143 A. C. Oli ei a Da Sil a,132 M. H. Oli e ,147 A. Onne s ad,127 C. Oppedisano,60
A. O iz Velasquez,70 T. Osako,46 A. Oska sson,82 J. O winowski,119 M. Oya,46 K. Oyama,84 Y. Pachmaye ,106 S. Padhan,49
D. Pagano,141,58 G. Pai´
c,70 A. Palasciano,53 J. Pan,144 S. Panebianco,139 J. Pa k,62 J. E. Pa kkila,127 S. P. Pa hak,126
055201-17
S. ACHARYA e al. PHYSICAL REVIEW C 107, 055201 (2023)
R. N. Pa a,103,34 B. Paul,22 H. Pei,7T. Pei zmann,63 X. Peng,7L. G. Pe ei a,71 H. Pe ei a Da Cos a,139 D. Pe esunko,90,83
G. M. Pe ez,8S. Pe in,139 Y. Pes o ,5V. Pe áˇ
cek,37 M. Pe o ici,48 R. P. Pezzi,116,71 S. Piano,61 M. Pikna,13 P. Pillo ,116
O. Pinazza,54,34 L. Pinsky,126 C. Pin o,26 S. Pisano,52 M. Płosko´
n,81 M. Planinic,101 F. Plique ,69 M. G. Poghosyan,98
B. Polich chouk,93 S. Poli ano,30 N. Poljak,101 A. Pop,48 S. Po eboeu -Houssais,136 J. Po e ,81 V. Pozdniako ,76 S. K. P asad,4
R. P eghenella,54 F. P ino,60 C. A. P uneau,144 I. Pshenichno ,64 M. Puccio,34 S. Qiu,92 L. Quaglia,24 R. E. Quishpe,126
S. Ragoni,112 A. Rako oza ind abe,139 L. Ramello,31 F. Rami,138 S. A. R. Rami ez,45 A. G. T. Ramos,33 T. A. Rancien,80
R. Raniwala,104 S. Raniwala,104 S. S. Räsänen,44 R. Ra h,50 I. Ra asenga,92 K. F. Read,98,132 A. R. Redelbach,39 K. Redlich,87,
A. Rehman,21 P. Reichel ,69 F. Reid ,34 H. A. Reme-ness,36 Z. Rescako a,38 K. Reyge s,106 A. Riabo ,100 V. Riabo ,100
T. Riche ,82 M. Rich e ,20 W. Riegle ,34 F. Riggi,26 C. Ris ea,68 M. Rod íguez Cahuan zi,45 K. Røed,20 R. Rogale ,93
E. Rogochaya,76 T. S. Rogoschinski,69 D. Roh ,34 D. Röh ich,21 P. F. Rojas,45 P. S. Roki a,143 F. Ronche i,52 A. Rosano,32,56
E. D. Rosas,70 A. Rossi,57 A. Roy,50 P. Roy,111 S. Roy,49 N. Rubini,25 O. V. Rueda,82 D. Ruggiano,143 R. Rui,23
B. Rumyan se ,76 P. G. Russek,2R. Russo,92 A. Rus amo ,89 E. Ryabinkin,90 Y. Ryabo ,100 A. Rybicki,119 H. Ry konen,127
W. Rzesa,143 O. A. M. Saa imaki,44 R. Sadek,116 S. Sado sky,93 J. Sae e,21 K. Ša aˇ
ík,37 S. K. Saha,142 S. Saha,88 B. Sahoo,49
P. Sahoo,49 R. Sahoo,50 S. Sahoo,66 D. Sahu,50 P. K. Sahu,66 J. Saini,142 S. Sakai,135 M. P. Sal an,109 S. Sambyal,103
V. Samsono ,100,95,bD. Sa ka ,144 N. Sa ka ,142 P. Sa ma,42 V. M. Sa i,107 M. H. P Sas,147 J. Schambach,98 H. S. Scheid,69
C. Schiaua,48 R. Schicke ,106 A. Schmah,106 C. Schmid ,109 H. R. Schmid ,105 M. O. Schmid ,34,106 M. Schmid ,105
N. V. Schmid ,98,69 A. R. Schmie ,132 R. Scho e ,138 J. Schuk a ,34 K. Schwa z,109 K. Schweda,109 G. Scioli,25
E. Scompa in,60 J. E. Sege ,15 Y. Sekiguchi,134 D. Sekiha a,134 I. Selyuzhenko ,109,95 S. Senyuko ,138 J. J. Seo,62
D. Se eb yako ,64 L. Še kšny ˙
e,107 A. Se cenco,68 T. J. Shaba,73 A. Shabano ,64 A. Shabe ai,116 R. Shahoyan,34 W. Shaikh,111
A. Shanga ae ,93 A. Sha ma,102 H. Sha ma,119 M. Sha ma,103 N. Sha ma,102 S. Sha ma,103 U. Sha ma,103 O. Sheibani,126
K. Shigaki,46 M. Shimomu a,85 S. Shi inkin,94 Q. Shou,40 Y. Sibi iak,90 S. Siddhan a,55 T. Siemia czuk,87 T. F. Sil a,122
D. Sil e my ,82 T. Siman a hammakul,117 G. Simone i,34 B. Singh,107 R. Singh,88 R. Singh,103 R. Singh,50 V. K. Singh,142
V. Singhal,142 T. Sinha,111 B. Si a ,13 M. Si a,31 T. B. Skaali,20 G. Sko odumo s,106 M. Slupecki,44 N. Smi no ,147
R. J. M Snellings,63 C. Soncco,113 J. Song,126 A. Songmoolnak,117 F. So amel,27 S. So ensen,132 I. Spu owska,119 J. S achel,106
I. S an,68 P. J. S e anic,132 S. F. S ie elmaie ,106 D. S occo,116 I. S o ehaug,20 M. M. S o e ed ,36 P. S a mann,145
C. P. S ylianidis,92 A. A. P. Suaide,122 C. Sui e,79 M. Sukhano ,64 M. Suljic,34 R. Sul ano ,94 V. Sumbe ia,103
S. Sumowidagdo,51 S. Swain,66 A. Szabo,13 I. Sza ka,13 U. Tabassam,14 S. F. Tagha i,107 G. Taillepied,136 J. Takahashi,123
G. J. Tamba e,21 S. Tang,136,7Z. Tang,130 J. D. Tapia Takaki,128,gM. Ta hini,116 M. G. Ta zila,48 A. Tau o,34
G. Tejeda Muñoz,45 A. Telesca,34 L. Te lizzi,24 C. Te e oli,126 G. Te simono ,3S. Thaku ,142 D. Thomas,120 R. Tieulen ,137
A. Tikhono ,64 A. R. Timmins,126 M. Tkacik,118 A. Toia,69 N. Topilskaya,64 M. Toppi,52 F. To ales-Acos a,19 T. To k,79
S. R. To es,37 A. T i i ó,32,56 S. T ipa hy,54,70 T. T ipa hy,49 S. T ogolo,34,27 V. T ubniko ,3W. H. T zaska,127
T. P. T zcinski,143 A. Tumkin,110 R. Tu isi,57 T. S. T e e ,20 K. Ullaland,21 A. U as,137 M. U ioni,58,141 G. L. Usai,22 M. Vala,38
N. Valle,28,58 S. Valle o,60 L. V. R an Do emalen,63 M. an Leeuwen,92 R. J. G. an Weelden,92 P. Vande Vy e,34 D. Va ga,146
Z. Va ga,146 M. Va ga-Ko a ago,146 M. Vasileiou,86 A. Vasilie ,90 O. Vázquez Doce,52,107 V. Veche nin,114 E. Ve cellin,24
S. Ve ga a Limón,45 L. Ve mun ,63 R. Vé esi,146 M. Ve weij,63 L. Vicko ic,35 Z. Vilakazi,133 O. Villalobos Baillie,112
G. Vino,53 A. Vinog ado ,90 T. Vi gili,29 V. Visla icius,91 A. Vodopyano ,76 B. Volkel,34,106 M. A. Völkl,106 K. Voloshin,94
S. A. Voloshin,144 G. Volpe,33 B. on Halle ,34 I. Vo obye ,107 D. Voscek,118 N. Vozniuk,64 J. V láko á,38 B. Wagne ,21
C. Wang,40 D. Wang,40 M. Webe ,115 A. Weg zynek,34 S. C. Wenzel,34 J. P. Wessels,145 J. Wiechula,69 J. Wikne,20 G. Wilk,87
J. Wilkinson,109 G. A. Willems,145 B. Windelband,106 M. Winn,139 W. E. Wi ,132 J. R. W igh ,120 W. Wu,40 Y. Wu,130 R. Xu,7
A. K. Yada ,142 S. Yalcin,78 Y. Yamaguchi,46 K. Yamakawa,46 S. Yang,21 S. Yano,46 Z. Yin,7I.-K. Yoo,17 J. H. Yoon,62
S. Yuan,21 A. Yuncu,106 V. Zaccolo,23 C. Zampolli,34 H. J. C Zanoli,63 N. Za dosh i,34 A. Za ochen se ,114 P. Zá ada,67
N. Za iyalo ,110 M. Zhalo ,100 B. Zhang,7S. Zhang,40 X. Zhang,7Y. Zhang,130 V. Zhe ebche skii,114 Y. Zhi,11 N. Zhiga e a,94
D. Zhou,7Y. Zhou,91 J. Zhu,109,7Y. Zhu,7G. Zino je ,3and N. Zu lo141,58
(ALICE Collabo a ion)
1A.I. Alikhanyan Na ional Science Labo a o y (Ye e an Physics Ins i u e) Founda ion, Ye e an, A menia
2AGH Uni e si y o Science and Technology, C acow, Poland
3Bogolyubo Ins i u e o Theo e ical Physics, Na ional Academy o Sciences o Uk aine, Kie , Uk aine
4Bose Ins i u e, Depa men o Physics and Cen e o As opa icle Physics and Space Science (CAPSS), Kolka a, India
5Budke Ins i u e o Nuclea Physics, No osibi sk, Russia
6Cali o nia Poly echnic S a e Uni e si y, San Luis Obispo, Cali o nia, USA
7Cen al China No mal Uni e si y, Wuhan, China
8Cen o de Aplicaciones Tecnológicas y Desa ollo Nuclea (CEADEN), Ha ana, Cuba
9Cen o de In es igación y de Es udios A anzados (CINVESTAV), Mexico Ci y and Mé ida, Mexico
10Chicago S a e Uni e si y, Chicago, Illinois, USA
11China Ins i u e o A omic Ene gy, Beijing, China
12Chungbuk Na ional Uni e si y, Cheongju, Republic o Ko ea
055201-18
K∗(892)0AND φ(1020) PRODUCTION IN p-Pb COLLISIONS … PHYSICAL REVIEW C 107, 055201 (2023)
13Comenius Uni e si y B a isla a, Facul y o Ma hema ics, Physics and In o ma ics, B a isla a, Slo akia
14COMSATS Uni e si y Islamabad, Islamabad, Pakis an
15C eigh on Uni e si y, Omaha, Neb aska, USA
16Depa men o Physics, Aliga h Muslim Uni e si y, Aliga h, India
17Depa men o Physics, Pusan Na ional Uni e si y, Pusan, Republic o Ko ea
18Depa men o Physics, Sejong Uni e si y, Seoul, Republic o Ko ea
19Depa men o Physics, Uni e si y o Cali o nia, Be keley, Cali o nia, USA
20Depa men o Physics, Uni e si y o Oslo, Oslo, No way
21Depa men o Physics and Technology, Uni e si y o Be gen, Be gen, No way
22Dipa imen o di Fisica dell’Uni e si à and Sezione INFN, Caglia i, I aly
23Dipa imen o di Fisica dell’Uni e si à and Sezione INFN, T ies e, I aly
24Dipa imen o di Fisica dell’Uni e si à and Sezione INFN, Tu in, I aly
25Dipa imen o di Fisica e As onomia dell’Uni e si à and Sezione INFN, Bologna, I aly
26Dipa imen o di Fisica e As onomia dell’Uni e si à and Sezione INFN, Ca ania, I aly
27Dipa imen o di Fisica e As onomia dell’Uni e si à and Sezione INFN, Pado a, I aly
28Dipa imen o di Fisica e Nuclea e e Teo ica, Uni e si à di Pa ia, Pa ia, I aly
29Dipa imen o di Fisica ‘E.R. Caianiello’ dell’Uni e si à and G uppo Collega o INFN, Sale no, I aly
30Dipa imen o DISAT del Poli ecnico and Sezione INFN, Tu in, I aly
31Dipa imen o di Scienze e Inno azione Tecnologica dell’Uni e si à del Piemon e O ien ale and INFN Sezione di To ino, Alessand ia, I aly
32Dipa imen o di Scienze MIFT, Uni e si à di Messina, Messina, I aly
33Dipa imen o In e a eneo di Fisica ‘M. Me lin’ and Sezione INFN, Ba i, I aly
34Eu opean O ganiza ion o Nuclea Resea ch (CERN), Gene a, Swi ze land
35Facul y o Elec ical Enginee ing, Mechanical Enginee ing and Na al A chi ec u e, Uni e si y o Spli , Spli , C oa ia
36Facul y o Enginee ing and Science, Wes e n No way Uni e si y o Applied Sciences, Be gen, No way
37Facul y o Nuclea Sciences and Physical Enginee ing, Czech Technical Uni e si y in P ague, P ague, Czech Republic
38Facul y o Science, P.J. Ša á ik Uni e si y, Košice, Slo akia
39F ank u Ins i u e o Ad anced S udies, Johann Wol gang Goe he-Uni e si ä F ank u , F ank u , Ge many
40Fudan Uni e si y, Shanghai, China
41Gangneung-Wonju Na ional Uni e si y, Gangneung, Republic o Ko ea
42Gauha i Uni e si y, Depa men o Physics, Guwaha i, India
43Helmhol z-Ins i u ü S ahlen- und Ke nphysik, Rheinische F ied ich-Wilhelms-Uni e si ä Bonn, Bonn, Ge many
44Helsinki Ins i u e o Physics (HIP), Helsinki, Finland
45High Ene gy Physics G oup, Uni e sidad Au ónoma de Puebla, Puebla, Mexico
46Hi oshima Uni e si y, Hi oshima, Japan
47Hochschule Wo ms, Zen um ü Technologie ans e und Telekommunika ion (ZTT), Wo ms, Ge many
48Ho ia Hulubei Na ional Ins i u e o Physics and Nuclea Enginee ing, Bucha es , Romania
49Indian Ins i u e o Technology Bombay (IIT), Mumbai, India
50Indian Ins i u e o Technology Indo e, Indo e, India
51Indonesian Ins i u e o Sciences, Jaka a, Indonesia
52INFN, Labo a o i Nazionali di F asca i, F asca i, I aly
53INFN, Sezione di Ba i, Ba i, I aly
54INFN, Sezione di Bologna, Bologna, I aly
55INFN, Sezione di Caglia i, Caglia i, I aly
56INFN, Sezione di Ca ania, Ca ania, I aly
57INFN, Sezione di Pado a, Pado a, I aly
58INFN, Sezione di Pa ia, Pa ia, I aly
59INFN, Sezione di Roma, Rome, I aly
60INFN, Sezione di To ino, Tu in, I aly
61INFN, Sezione di T ies e, T ies e, I aly
62Inha Uni e si y, Incheon, Republic o Ko ea
63Ins i u e o G a i a ional and Suba omic Physics (GRASP), U ech Uni e si y/Nikhe , U ech , Ne he lands
64Ins i u e o Nuclea Resea ch, Academy o Sciences, Moscow, Russia
65Ins i u e o Expe imen al Physics, Slo ak Academy o Sciences, Košice, Slo akia
66Ins i u e o Physics, Homi Bhabha Na ional Ins i u e, Bhubaneswa , India
67Ins i u e o Physics o he Czech Academy o Sciences, P ague, Czech Republic
68Ins i u e o Space Science (ISS), Bucha es , Romania
69Ins i u ü Ke nphysik, Johann Wol gang Goe he-Uni e si ä F ank u , F ank u , Ge many
70Ins i u o de Ciencias Nuclea es, Uni e sidad Nacional Au ónoma de México, Mexico Ci y, Mexico
71Ins i u o de Física, Uni e sidade Fede al do Rio G ande do Sul (UFRGS), Po o Aleg e, B azil
055201-19
S. ACHARYA e al. PHYSICAL REVIEW C 107, 055201 (2023)
72Ins i u o de Física, Uni e sidad Nacional Au ónoma de México, Mexico Ci y, Mexico
73iThemba LABS, Na ional Resea ch Founda ion, Some se Wes , Sou h A ica
74Jeonbuk Na ional Uni e si y, Jeonju, Republic o Ko ea
75Johann-Wol gang-Goe he Uni e si ä F ank u Ins i u ü In o ma ik, Fachbe eich In o ma ik und Ma hema ik, F ank u , Ge many
76Join Ins i u e o Nuclea Resea ch (JINR), Dubna, Russia
77Ko ea Ins i u e o Science and Technology In o ma ion, Daejeon, Republic o Ko ea
78KTO Ka a ay Uni e si y, Konya, Tu key
79Labo a oi e de Physique des 2 In inis, I ène Jolio -Cu ie, O say, F ance
80Labo a oi e de Physique Suba omique e de Cosmologie, Uni e si é G enoble-Alpes, CNRS-IN2P3, G enoble, F ance
81Law ence Be keley Na ional Labo a o y, Be keley, Cali o nia, USA
82Lund Uni e si y Depa men o Physics, Di ision o Pa icle Physics, Lund, Sweden
83Moscow Ins i u e o Physics and Technology, Moscow, Russia
84Nagasaki Ins i u e o Applied Science, Nagasaki, Japan
85Na a Women’s Uni e si y (NWU), Na a, Japan
86Na ional and Kapodis ian Uni e si y o A hens, School o Science, Depa men o Physics, A hens, G eece
87Na ional Cen e o Nuclea Resea ch, Wa saw, Poland
88Na ional Ins i u e o Science Educa ion and Resea ch, Homi Bhabha Na ional Ins i u e, Ja ni, India
89Na ional Nuclea Resea ch Cen e , Baku, Aze baijan
90Na ional Resea ch Cen e Ku cha o Ins i u e, Moscow, Russia
91Niels Boh Ins i u e, Uni e si y o Copenhagen, Copenhagen, Denma k
92Nikhe , Na ional ins i u e o suba omic physics, Ams e dam, Ne he lands
93NRC Ku cha o Ins i u e IHEP, P o ino, Russia
94NRC Ku cha o Ins i u e - ITEP, Moscow, Russia
95NRNU Moscow Enginee ing Physics Ins i u e, Moscow, Russia
96Nuclea Physics G oup, STFC Da esbu y Labo a o y, Da esbu y, Uni ed Kingdom
97Nuclea Physics Ins i u e o he Czech Academy o Sciences, ˇ
Rež u P ahy, Czech Republic
98Oak Ridge Na ional Labo a o y, Oak Ridge, Tennessee, USA
99Ohio S a e Uni e si y, Columbus, Ohio, USA
100Pe e sbu g Nuclea Physics Ins i u e, Ga china, Russia
101Physics depa men , Facul y o science, Uni e si y o Zag eb, Zag eb, C oa ia
102Physics Depa men , Panjab Uni e si y, Chandiga h, India
103Physics Depa men , Uni e si y o Jammu, Jammu, India
104Physics Depa men , Uni e si y o Rajas han, Jaipu , India
105Physikalisches Ins i u , Ebe ha d-Ka ls-Uni e si ä Tübingen, Tübingen, Ge many
106Physikalisches Ins i u , Rup ech -Ka ls-Uni e si ä Heidelbe g, Heidelbe g, Ge many
107Physik Depa men , Technische Uni e si ä München, Munich, Ge many
108Poli ecnico di Ba i and Sezione INFN, Ba i, I aly
109Resea ch Di ision and Ex eMe Ma e Ins i u e EMMI, GSI Helmhol zzen um ü Schwe ionen o schung GmbH, Da ms ad , Ge many
110Russian Fede al Nuclea Cen e (VNIIEF), Sa o , Russia
111Saha Ins i u e o Nuclea Physics, Homi Bhabha Na ional Ins i u e, Kolka a, India
112School o Physics and As onomy, Uni e si y o Bi mingham, Bi mingham, Uni ed Kingdom
113Sección Física, Depa amen o de Ciencias, Pon i icia Uni e sidad Ca ólica del Pe ú, Lima, Pe u
114S . Pe e sbu g S a e Uni e si y, S . Pe e sbu g, Russia
115S e an Meye Ins i u ü Suba oma e Physik (SMI), Vienna, Aus ia
116SUBATECH, IMT A lan ique, Uni e si é de Nan es, CNRS-IN2P3, Nan es, F ance
117Su ana ee Uni e si y o Technology, Nakhon Ra chasima, Thailand
118Technical Uni e si y o Košice, Košice, Slo akia
119The Hen yk Niewodniczanski Ins i u e o Nuclea Physics, Polish Academy o Sciences, C acow, Poland
120The Uni e si y o Texas a Aus in, Aus in, Texas, USA
121Uni e sidad Au ónoma de Sinaloa, Culiacán, Mexico
122Uni e sidade de São Paulo (USP), São Paulo, B azil
123Uni e sidade Es adual de Campinas (UNICAMP), Campinas, B azil
124Uni e sidade Fede al do ABC, San o And e, B azil
125Uni e si y o Cape Town, Cape Town, Sou h A ica
126Uni e si y o Hous on, Hous on, Texas, USA
127Uni e si y o Jy äskylä, Jy äskylä, Finland
128Uni e si y o Kansas, Law ence, Kansas, USA
129Uni e si y o Li e pool, Li e pool, Uni ed Kingdom
130Uni e si y o Science and Technology o China, He ei, China
055201-20

K∗(892)0AND φ(1020) PRODUCTION IN p-Pb COLLISIONS … PHYSICAL REVIEW C 107, 055201 (2023)
131Uni e si y o Sou h-Eas e n No way, Tonsbe g, No way
132Uni e si y o Tennessee, Knox ille, Tennessee, USA
133Uni e si y o he Wi wa e s and, Johannesbu g, Sou h A ica
134Uni e si y o Tokyo, Tokyo, Japan
135Uni e si y o Tsukuba, Tsukuba, Japan
136Uni e si é Cle mon Au e gne, CNRS/IN2P3, LPC, Cle mon -Fe and, F ance
137Uni e si é de Lyon, CNRS/IN2P3, Ins i u de Physique des 2 In inis de Lyon, Lyon, F ance
138Uni e si é de S asbou g, CNRS, IPHC UMR 7178, F-67000 S asbou g, F ance, S asbou g, F ance
139Uni e si é Pa is-Saclay Cen e d’E udes de Saclay (CEA), IRFU, Dépa men de Physique Nucléai e (DPhN), Saclay, F ance
140Uni e si à degli S udi di Foggia, Foggia, I aly
141Uni e si à di B escia, B escia, I aly
142Va iable Ene gy Cyclo on Cen e, Homi Bhabha Na ional Ins i u e, Kolka a, India
143Wa saw Uni e si y o Technology, Wa saw, Poland
144Wayne S a e Uni e si y, De oi , Michigan, USA
145Wes älische Wilhelms-Uni e si ä Müns e , Ins i u ü Ke nphysik, Müns e , Ge many
146Wigne Resea ch Cen e o Physics, Budapes , Hunga y
147Yale Uni e si y, New Ha en, Connec icu , USA
148Yonsei Uni e si y, Seoul, Republic o Ko ea
aAlso a : I alian Na ional Agency o New Technologies, Ene gy and Sus ainable Economic De elopmen (ENEA), Bologna, I aly.
bDeceased.
cAlso a : Dipa imen o DET del Poli ecnico di To ino, Tu in, I aly.
dAlso a : M.V. Lomonoso Moscow S a e Uni e si y, D.V. Skobel syn Ins i u e o Nuclea , Physics, Moscow, Russia.
eAlso a : Depa men o Applied Physics, Aliga h Muslim Uni e si y, Aliga h, India.
Also a : Ins i u e o Theo e ical Physics, Uni e si y o W oclaw, Poland.
gAlso a : Uni e si y o Kansas, Law ence, Kansas, USA.
055201-21