The p
seudorapidity (
η ) and tran
sver
se-momentum (<
span id="mm
lsi11" c
la
ss="mathm
lsrc"><
span c
la
ss="formu
latext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0370269315009788&_mathId=
si11.gif&_u
ser=111111111&_pii=S0370269315009788&_rdoc=1&_i
ssn=03702693&md5=d2d211c01f252a712c30ecfd5b464626" tit
le="C
lick to view the MathML
source">p<
sub>T
sub>
span><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span>) di
stribution
s of charged partic
le
s produced in proton&nda
sh;proton co
lli
sion
s are mea
sured at the centre-of-ma
ss energy <
span id="mm
lsi1" c
la
ss="mathm
lsrc">
le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269315009788&_mathId=si1.gif&_user=111111111&_pii=S0370269315009788&_rdoc=1&_issn=03702693&md5=1ea0c32d11bede802a71b9050704e35b">lass="imgLazyJSB inlineImage" height="15" width="79" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269315009788-si1.gif">script>style="vertical-align:bottom" width="79" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.com/content/image/1-s2.0-S0370269315009788-si1.gif">script><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span>. The p
seudorapidity di
stribution in <
span id="mm
lsi3" c
la
ss="mathm
lsrc"><
span c
la
ss="formu
latext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0370269315009788&_mathId=
si3.gif&_u
ser=111111111&_pii=S0370269315009788&_rdoc=1&_i
ssn=03702693&md5=f3c0006de24526029765aef4a509f38a" tit
le="C
lick to view the MathML
source">|η|&
lt;1.8
span><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span> i
s reported for ine
la
stic event
s and for event
s with at
lea
st one charged partic
le in <
span id="mm
lsi10" c
la
ss="mathm
lsrc"><
span c
la
ss="formu
latext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0370269315009788&_mathId=
si10.gif&_u
ser=111111111&_pii=S0370269315009788&_rdoc=1&_i
ssn=03702693&md5=ffa3efaf5d78e7cf227c9338e0b447bc" tit
le="C
lick to view the MathML
source">|η|&
lt;1
span><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span>. The p
seudorapidity den
sity of charged partic
le
s produced in the p
seudorapidity region <
span id="mm
lsi5" c
la
ss="mathm
lsrc"><
span c
la
ss="formu
latext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0370269315009788&_mathId=
si5.gif&_u
ser=111111111&_pii=S0370269315009788&_rdoc=1&_i
ssn=03702693&md5=046778b78971197d660a2ce4616fb836" tit
le="C
lick to view the MathML
source">|η|&
lt;0.5
span><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span> i
s <
span id="mm
lsi50" c
la
ss="mathm
lsrc"><
span c
la
ss="formu
latext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0370269315009788&_mathId=
si50.gif&_u
ser=111111111&_pii=S0370269315009788&_rdoc=1&_i
ssn=03702693&md5=67195bec065de1d377ce9cca73c70f72" tit
le="C
lick to view the MathML
source">5.31&p
lu
smn;0.18
span><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span> and <
span id="mm
lsi7" c
la
ss="mathm
lsrc"><
span c
la
ss="formu
latext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0370269315009788&_mathId=
si7.gif&_u
ser=111111111&_pii=S0370269315009788&_rdoc=1&_i
ssn=03702693&md5=d099703854200f5ec6c39aa88b544fd2" tit
le="C
lick to view the MathML
source">6.46&p
lu
smn;0.19
span><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span> for the two event c
la
sse
s, re
spective
ly. The tran
sver
se-momentum di
stribution of charged partic
le
s i
s mea
sured in the range <
span id="mm
lsi8" c
la
ss="mathm
lsrc"><
span c
la
ss="formu
latext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0370269315009788&_mathId=
si8.gif&_u
ser=111111111&_pii=S0370269315009788&_rdoc=1&_i
ssn=03702693&md5=9bd5846240873d3ceeb5fa7b3a2e2b00" tit
le="C
lick to view the MathML
source">0.15&
lt;p<
sub>T
sub>&
lt;20 GeV/c
span><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span> and <
span id="mm
lsi15" c
la
ss="mathm
lsrc"><
span c
la
ss="formu
latext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0370269315009788&_mathId=
si15.gif&_u
ser=111111111&_pii=S0370269315009788&_rdoc=1&_i
ssn=03702693&md5=cf7c1ef2e614bae11d3efe4193af5556" tit
le="C
lick to view the MathML
source">|η|&
lt;0.8
span><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span> for event
s with at
lea
st one charged partic
le in <
span id="mm
lsi10" c
la
ss="mathm
lsrc"><
span c
la
ss="formu
latext
stixSupport mathImg" data-mathURL="/
science?_ob=MathURL&_method=retrieve&_eid=1-
s2.0-S0370269315009788&_mathId=
si10.gif&_u
ser=111111111&_pii=S0370269315009788&_rdoc=1&_i
ssn=03702693&md5=ffa3efaf5d78e7cf227c9338e0b447bc" tit
le="C
lick to view the MathML
source">|η|&
lt;1
span><
span c
la
ss="mathContainer hidden"><
span c
la
ss="mathCode">
span>
span>
span>. The evo
lution of the tran
sver
se momentum
spectra of charged partic
le
s i
s a
lso inve
stigated a
s a function of event mu
ltip
licity. The re
su
lt
s are compared with ca
lcu
lation
s from PYTHIA and EPOS Monte Car
lo generator
s.