\section{The ALICE Collaboration}

\begingroup
\small
\begin{flushleft}
D.~Adamov\'{a}$^\textrm{\scriptsize 87}$,
M.M.~Aggarwal$^\textrm{\scriptsize 91}$,
G.~Aglieri Rinella$^\textrm{\scriptsize 34}$,
M.~Agnello$^\textrm{\scriptsize 30}$\textsuperscript{,}$^\textrm{\scriptsize 113}$,
N.~Agrawal$^\textrm{\scriptsize 47}$,
Z.~Ahammed$^\textrm{\scriptsize 139}$,
S.~Ahmad$^\textrm{\scriptsize 17}$,
S.U.~Ahn$^\textrm{\scriptsize 69}$,
S.~Aiola$^\textrm{\scriptsize 143}$,
A.~Akindinov$^\textrm{\scriptsize 54}$,
S.N.~Alam$^\textrm{\scriptsize 139}$,
D.S.D.~Albuquerque$^\textrm{\scriptsize 124}$,
D.~Aleksandrov$^\textrm{\scriptsize 83}$,
B.~Alessandro$^\textrm{\scriptsize 113}$,
D.~Alexandre$^\textrm{\scriptsize 104}$,
R.~Alfaro Molina$^\textrm{\scriptsize 64}$,
A.~Alici$^\textrm{\scriptsize 12}$\textsuperscript{,}$^\textrm{\scriptsize 107}$,
A.~Alkin$^\textrm{\scriptsize 3}$,
J.~Alme$^\textrm{\scriptsize 21}$\textsuperscript{,}$^\textrm{\scriptsize 36}$,
T.~Alt$^\textrm{\scriptsize 41}$,
S.~Altinpinar$^\textrm{\scriptsize 21}$,
I.~Altsybeev$^\textrm{\scriptsize 138}$,
C.~Alves Garcia Prado$^\textrm{\scriptsize 123}$,
M.~An$^\textrm{\scriptsize 7}$,
C.~Andrei$^\textrm{\scriptsize 80}$,
H.A.~Andrews$^\textrm{\scriptsize 104}$,
A.~Andronic$^\textrm{\scriptsize 100}$,
V.~Anguelov$^\textrm{\scriptsize 96}$,
C.~Anson$^\textrm{\scriptsize 90}$,
T.~Anti\v{c}i\'{c}$^\textrm{\scriptsize 101}$,
F.~Antinori$^\textrm{\scriptsize 110}$,
P.~Antonioli$^\textrm{\scriptsize 107}$,
R.~Anwar$^\textrm{\scriptsize 126}$,
L.~Aphecetche$^\textrm{\scriptsize 116}$,
H.~Appelsh\"{a}user$^\textrm{\scriptsize 60}$,
S.~Arcelli$^\textrm{\scriptsize 26}$,
R.~Arnaldi$^\textrm{\scriptsize 113}$,
O.W.~Arnold$^\textrm{\scriptsize 97}$\textsuperscript{,}$^\textrm{\scriptsize 35}$,
I.C.~Arsene$^\textrm{\scriptsize 20}$,
M.~Arslandok$^\textrm{\scriptsize 60}$,
B.~Audurier$^\textrm{\scriptsize 116}$,
A.~Augustinus$^\textrm{\scriptsize 34}$,
R.~Averbeck$^\textrm{\scriptsize 100}$,
M.D.~Azmi$^\textrm{\scriptsize 17}$,
A.~Badal\`{a}$^\textrm{\scriptsize 109}$,
Y.W.~Baek$^\textrm{\scriptsize 68}$,
S.~Bagnasco$^\textrm{\scriptsize 113}$,
R.~Bailhache$^\textrm{\scriptsize 60}$,
R.~Bala$^\textrm{\scriptsize 93}$,
A.~Baldisseri$^\textrm{\scriptsize 65}$,
M.~Ball$^\textrm{\scriptsize 44}$,
R.C.~Baral$^\textrm{\scriptsize 57}$,
A.M.~Barbano$^\textrm{\scriptsize 25}$,
R.~Barbera$^\textrm{\scriptsize 27}$,
F.~Barile$^\textrm{\scriptsize 32}$,
L.~Barioglio$^\textrm{\scriptsize 25}$,
G.G.~Barnaf\"{o}ldi$^\textrm{\scriptsize 142}$,
L.S.~Barnby$^\textrm{\scriptsize 104}$\textsuperscript{,}$^\textrm{\scriptsize 34}$,
V.~Barret$^\textrm{\scriptsize 71}$,
P.~Bartalini$^\textrm{\scriptsize 7}$,
K.~Barth$^\textrm{\scriptsize 34}$,
J.~Bartke$^\textrm{\scriptsize 120}$\Aref{0},
E.~Bartsch$^\textrm{\scriptsize 60}$,
M.~Basile$^\textrm{\scriptsize 26}$,
N.~Bastid$^\textrm{\scriptsize 71}$,
S.~Basu$^\textrm{\scriptsize 139}$,
B.~Bathen$^\textrm{\scriptsize 61}$,
G.~Batigne$^\textrm{\scriptsize 116}$,
A.~Batista Camejo$^\textrm{\scriptsize 71}$,
B.~Batyunya$^\textrm{\scriptsize 67}$,
P.C.~Batzing$^\textrm{\scriptsize 20}$,
I.G.~Bearden$^\textrm{\scriptsize 84}$,
H.~Beck$^\textrm{\scriptsize 96}$,
C.~Bedda$^\textrm{\scriptsize 30}$,
N.K.~Behera$^\textrm{\scriptsize 50}$,
I.~Belikov$^\textrm{\scriptsize 135}$,
F.~Bellini$^\textrm{\scriptsize 26}$,
H.~Bello Martinez$^\textrm{\scriptsize 2}$,
R.~Bellwied$^\textrm{\scriptsize 126}$,
L.G.E.~Beltran$^\textrm{\scriptsize 122}$,
V.~Belyaev$^\textrm{\scriptsize 76}$,
G.~Bencedi$^\textrm{\scriptsize 142}$,
S.~Beole$^\textrm{\scriptsize 25}$,
A.~Bercuci$^\textrm{\scriptsize 80}$,
Y.~Berdnikov$^\textrm{\scriptsize 89}$,
D.~Berenyi$^\textrm{\scriptsize 142}$,
R.A.~Bertens$^\textrm{\scriptsize 53}$\textsuperscript{,}$^\textrm{\scriptsize 129}$,
D.~Berzano$^\textrm{\scriptsize 34}$,
L.~Betev$^\textrm{\scriptsize 34}$,
A.~Bhasin$^\textrm{\scriptsize 93}$,
I.R.~Bhat$^\textrm{\scriptsize 93}$,
A.K.~Bhati$^\textrm{\scriptsize 91}$,
B.~Bhattacharjee$^\textrm{\scriptsize 43}$,
J.~Bhom$^\textrm{\scriptsize 120}$,
L.~Bianchi$^\textrm{\scriptsize 126}$,
N.~Bianchi$^\textrm{\scriptsize 73}$,
C.~Bianchin$^\textrm{\scriptsize 141}$,
J.~Biel\v{c}\'{\i}k$^\textrm{\scriptsize 38}$,
J.~Biel\v{c}\'{\i}kov\'{a}$^\textrm{\scriptsize 87}$,
A.~Bilandzic$^\textrm{\scriptsize 35}$\textsuperscript{,}$^\textrm{\scriptsize 97}$,
G.~Biro$^\textrm{\scriptsize 142}$,
R.~Biswas$^\textrm{\scriptsize 4}$,
S.~Biswas$^\textrm{\scriptsize 4}$,
J.T.~Blair$^\textrm{\scriptsize 121}$,
D.~Blau$^\textrm{\scriptsize 83}$,
C.~Blume$^\textrm{\scriptsize 60}$,
G.~Boca$^\textrm{\scriptsize 136}$,
F.~Bock$^\textrm{\scriptsize 75}$\textsuperscript{,}$^\textrm{\scriptsize 96}$,
A.~Bogdanov$^\textrm{\scriptsize 76}$,
L.~Boldizs\'{a}r$^\textrm{\scriptsize 142}$,
M.~Bombara$^\textrm{\scriptsize 39}$,
G.~Bonomi$^\textrm{\scriptsize 137}$,
M.~Bonora$^\textrm{\scriptsize 34}$,
J.~Book$^\textrm{\scriptsize 60}$,
H.~Borel$^\textrm{\scriptsize 65}$,
A.~Borissov$^\textrm{\scriptsize 99}$,
M.~Borri$^\textrm{\scriptsize 128}$,
E.~Botta$^\textrm{\scriptsize 25}$,
C.~Bourjau$^\textrm{\scriptsize 84}$,
P.~Braun-Munzinger$^\textrm{\scriptsize 100}$,
M.~Bregant$^\textrm{\scriptsize 123}$,
T.A.~Broker$^\textrm{\scriptsize 60}$,
T.A.~Browning$^\textrm{\scriptsize 98}$,
M.~Broz$^\textrm{\scriptsize 38}$,
E.J.~Brucken$^\textrm{\scriptsize 45}$,
E.~Bruna$^\textrm{\scriptsize 113}$,
G.E.~Bruno$^\textrm{\scriptsize 32}$,
D.~Budnikov$^\textrm{\scriptsize 102}$,
H.~Buesching$^\textrm{\scriptsize 60}$,
S.~Bufalino$^\textrm{\scriptsize 30}$\textsuperscript{,}$^\textrm{\scriptsize 25}$,
P.~Buhler$^\textrm{\scriptsize 115}$,
S.A.I.~Buitron$^\textrm{\scriptsize 62}$,
P.~Buncic$^\textrm{\scriptsize 34}$,
O.~Busch$^\textrm{\scriptsize 132}$,
Z.~Buthelezi$^\textrm{\scriptsize 66}$,
J.B.~Butt$^\textrm{\scriptsize 15}$,
J.T.~Buxton$^\textrm{\scriptsize 18}$,
J.~Cabala$^\textrm{\scriptsize 118}$,
D.~Caffarri$^\textrm{\scriptsize 34}$,
H.~Caines$^\textrm{\scriptsize 143}$,
A.~Caliva$^\textrm{\scriptsize 53}$,
E.~Calvo Villar$^\textrm{\scriptsize 105}$,
P.~Camerini$^\textrm{\scriptsize 24}$,
A.A.~Capon$^\textrm{\scriptsize 115}$,
F.~Carena$^\textrm{\scriptsize 34}$,
W.~Carena$^\textrm{\scriptsize 34}$,
F.~Carnesecchi$^\textrm{\scriptsize 26}$\textsuperscript{,}$^\textrm{\scriptsize 12}$,
J.~Castillo Castellanos$^\textrm{\scriptsize 65}$,
A.J.~Castro$^\textrm{\scriptsize 129}$,
E.A.R.~Casula$^\textrm{\scriptsize 23}$\textsuperscript{,}$^\textrm{\scriptsize 108}$,
C.~Ceballos Sanchez$^\textrm{\scriptsize 9}$,
P.~Cerello$^\textrm{\scriptsize 113}$,
B.~Chang$^\textrm{\scriptsize 127}$,
S.~Chapeland$^\textrm{\scriptsize 34}$,
M.~Chartier$^\textrm{\scriptsize 128}$,
J.L.~Charvet$^\textrm{\scriptsize 65}$,
S.~Chattopadhyay$^\textrm{\scriptsize 139}$,
S.~Chattopadhyay$^\textrm{\scriptsize 103}$,
A.~Chauvin$^\textrm{\scriptsize 97}$\textsuperscript{,}$^\textrm{\scriptsize 35}$,
M.~Cherney$^\textrm{\scriptsize 90}$,
C.~Cheshkov$^\textrm{\scriptsize 134}$,
B.~Cheynis$^\textrm{\scriptsize 134}$,
V.~Chibante Barroso$^\textrm{\scriptsize 34}$,
D.D.~Chinellato$^\textrm{\scriptsize 124}$,
S.~Cho$^\textrm{\scriptsize 50}$,
P.~Chochula$^\textrm{\scriptsize 34}$,
K.~Choi$^\textrm{\scriptsize 99}$,
M.~Chojnacki$^\textrm{\scriptsize 84}$,
S.~Choudhury$^\textrm{\scriptsize 139}$,
P.~Christakoglou$^\textrm{\scriptsize 85}$,
C.H.~Christensen$^\textrm{\scriptsize 84}$,
P.~Christiansen$^\textrm{\scriptsize 33}$,
T.~Chujo$^\textrm{\scriptsize 132}$,
S.U.~Chung$^\textrm{\scriptsize 99}$,
C.~Cicalo$^\textrm{\scriptsize 108}$,
L.~Cifarelli$^\textrm{\scriptsize 12}$\textsuperscript{,}$^\textrm{\scriptsize 26}$,
F.~Cindolo$^\textrm{\scriptsize 107}$,
J.~Cleymans$^\textrm{\scriptsize 92}$,
F.~Colamaria$^\textrm{\scriptsize 32}$,
D.~Colella$^\textrm{\scriptsize 55}$\textsuperscript{,}$^\textrm{\scriptsize 34}$,
A.~Collu$^\textrm{\scriptsize 75}$,
M.~Colocci$^\textrm{\scriptsize 26}$,
G.~Conesa Balbastre$^\textrm{\scriptsize 72}$,
Z.~Conesa del Valle$^\textrm{\scriptsize 51}$,
M.E.~Connors$^\textrm{\scriptsize 143}$\Aref{idp1764384},
J.G.~Contreras$^\textrm{\scriptsize 38}$,
T.M.~Cormier$^\textrm{\scriptsize 88}$,
Y.~Corrales Morales$^\textrm{\scriptsize 113}$,
I.~Cort\'{e}s Maldonado$^\textrm{\scriptsize 2}$,
P.~Cortese$^\textrm{\scriptsize 31}$,
M.R.~Cosentino$^\textrm{\scriptsize 125}$,
F.~Costa$^\textrm{\scriptsize 34}$,
S.~Costanza$^\textrm{\scriptsize 136}$,
J.~Crkovsk\'{a}$^\textrm{\scriptsize 51}$,
P.~Crochet$^\textrm{\scriptsize 71}$,
E.~Cuautle$^\textrm{\scriptsize 62}$,
L.~Cunqueiro$^\textrm{\scriptsize 61}$,
T.~Dahms$^\textrm{\scriptsize 35}$\textsuperscript{,}$^\textrm{\scriptsize 97}$,
A.~Dainese$^\textrm{\scriptsize 110}$,
M.C.~Danisch$^\textrm{\scriptsize 96}$,
A.~Danu$^\textrm{\scriptsize 58}$,
D.~Das$^\textrm{\scriptsize 103}$,
I.~Das$^\textrm{\scriptsize 103}$,
S.~Das$^\textrm{\scriptsize 4}$,
A.~Dash$^\textrm{\scriptsize 81}$,
S.~Dash$^\textrm{\scriptsize 47}$,
S.~De$^\textrm{\scriptsize 48}$\textsuperscript{,}$^\textrm{\scriptsize 123}$,
A.~De Caro$^\textrm{\scriptsize 29}$,
G.~de Cataldo$^\textrm{\scriptsize 106}$,
C.~de Conti$^\textrm{\scriptsize 123}$,
J.~de Cuveland$^\textrm{\scriptsize 41}$,
A.~De Falco$^\textrm{\scriptsize 23}$,
D.~De Gruttola$^\textrm{\scriptsize 12}$\textsuperscript{,}$^\textrm{\scriptsize 29}$,
N.~De Marco$^\textrm{\scriptsize 113}$,
S.~De Pasquale$^\textrm{\scriptsize 29}$,
R.D.~De Souza$^\textrm{\scriptsize 124}$,
H.F.~Degenhardt$^\textrm{\scriptsize 123}$,
A.~Deisting$^\textrm{\scriptsize 100}$\textsuperscript{,}$^\textrm{\scriptsize 96}$,
A.~Deloff$^\textrm{\scriptsize 79}$,
C.~Deplano$^\textrm{\scriptsize 85}$,
P.~Dhankher$^\textrm{\scriptsize 47}$,
D.~Di Bari$^\textrm{\scriptsize 32}$,
A.~Di Mauro$^\textrm{\scriptsize 34}$,
P.~Di Nezza$^\textrm{\scriptsize 73}$,
B.~Di Ruzza$^\textrm{\scriptsize 110}$,
M.A.~Diaz Corchero$^\textrm{\scriptsize 10}$,
T.~Dietel$^\textrm{\scriptsize 92}$,
P.~Dillenseger$^\textrm{\scriptsize 60}$,
R.~Divi\`{a}$^\textrm{\scriptsize 34}$,
{\O}.~Djuvsland$^\textrm{\scriptsize 21}$,
A.~Dobrin$^\textrm{\scriptsize 58}$\textsuperscript{,}$^\textrm{\scriptsize 34}$,
D.~Domenicis Gimenez$^\textrm{\scriptsize 123}$,
B.~D\"{o}nigus$^\textrm{\scriptsize 60}$,
O.~Dordic$^\textrm{\scriptsize 20}$,
T.~Drozhzhova$^\textrm{\scriptsize 60}$,
A.K.~Dubey$^\textrm{\scriptsize 139}$,
A.~Dubla$^\textrm{\scriptsize 100}$,
L.~Ducroux$^\textrm{\scriptsize 134}$,
A.K.~Duggal$^\textrm{\scriptsize 91}$,
P.~Dupieux$^\textrm{\scriptsize 71}$,
R.J.~Ehlers$^\textrm{\scriptsize 143}$,
D.~Elia$^\textrm{\scriptsize 106}$,
E.~Endress$^\textrm{\scriptsize 105}$,
H.~Engel$^\textrm{\scriptsize 59}$,
E.~Epple$^\textrm{\scriptsize 143}$,
B.~Erazmus$^\textrm{\scriptsize 116}$,
F.~Erhardt$^\textrm{\scriptsize 133}$,
B.~Espagnon$^\textrm{\scriptsize 51}$,
S.~Esumi$^\textrm{\scriptsize 132}$,
G.~Eulisse$^\textrm{\scriptsize 34}$,
J.~Eum$^\textrm{\scriptsize 99}$,
D.~Evans$^\textrm{\scriptsize 104}$,
S.~Evdokimov$^\textrm{\scriptsize 114}$,
L.~Fabbietti$^\textrm{\scriptsize 35}$\textsuperscript{,}$^\textrm{\scriptsize 97}$,
D.~Fabris$^\textrm{\scriptsize 110}$,
J.~Faivre$^\textrm{\scriptsize 72}$,
A.~Fantoni$^\textrm{\scriptsize 73}$,
M.~Fasel$^\textrm{\scriptsize 88}$\textsuperscript{,}$^\textrm{\scriptsize 75}$,
L.~Feldkamp$^\textrm{\scriptsize 61}$,
A.~Feliciello$^\textrm{\scriptsize 113}$,
G.~Feofilov$^\textrm{\scriptsize 138}$,
J.~Ferencei$^\textrm{\scriptsize 87}$,
A.~Fern\'{a}ndez T\'{e}llez$^\textrm{\scriptsize 2}$,
E.G.~Ferreiro$^\textrm{\scriptsize 16}$,
A.~Ferretti$^\textrm{\scriptsize 25}$,
A.~Festanti$^\textrm{\scriptsize 28}$,
V.J.G.~Feuillard$^\textrm{\scriptsize 71}$\textsuperscript{,}$^\textrm{\scriptsize 65}$,
J.~Figiel$^\textrm{\scriptsize 120}$,
M.A.S.~Figueredo$^\textrm{\scriptsize 123}$,
S.~Filchagin$^\textrm{\scriptsize 102}$,
D.~Finogeev$^\textrm{\scriptsize 52}$,
F.M.~Fionda$^\textrm{\scriptsize 23}$,
E.M.~Fiore$^\textrm{\scriptsize 32}$,
M.~Floris$^\textrm{\scriptsize 34}$,
S.~Foertsch$^\textrm{\scriptsize 66}$,
P.~Foka$^\textrm{\scriptsize 100}$,
S.~Fokin$^\textrm{\scriptsize 83}$,
E.~Fragiacomo$^\textrm{\scriptsize 112}$,
A.~Francescon$^\textrm{\scriptsize 34}$,
A.~Francisco$^\textrm{\scriptsize 116}$,
U.~Frankenfeld$^\textrm{\scriptsize 100}$,
G.G.~Fronze$^\textrm{\scriptsize 25}$,
U.~Fuchs$^\textrm{\scriptsize 34}$,
C.~Furget$^\textrm{\scriptsize 72}$,
A.~Furs$^\textrm{\scriptsize 52}$,
M.~Fusco Girard$^\textrm{\scriptsize 29}$,
J.J.~Gaardh{\o}je$^\textrm{\scriptsize 84}$,
M.~Gagliardi$^\textrm{\scriptsize 25}$,
A.M.~Gago$^\textrm{\scriptsize 105}$,
K.~Gajdosova$^\textrm{\scriptsize 84}$,
M.~Gallio$^\textrm{\scriptsize 25}$,
C.D.~Galvan$^\textrm{\scriptsize 122}$,
D.R.~Gangadharan$^\textrm{\scriptsize 75}$,
P.~Ganoti$^\textrm{\scriptsize 78}$,
C.~Gao$^\textrm{\scriptsize 7}$,
C.~Garabatos$^\textrm{\scriptsize 100}$,
E.~Garcia-Solis$^\textrm{\scriptsize 13}$,
K.~Garg$^\textrm{\scriptsize 27}$,
P.~Garg$^\textrm{\scriptsize 48}$,
C.~Gargiulo$^\textrm{\scriptsize 34}$,
P.~Gasik$^\textrm{\scriptsize 35}$\textsuperscript{,}$^\textrm{\scriptsize 97}$,
E.F.~Gauger$^\textrm{\scriptsize 121}$,
M.B.~Gay Ducati$^\textrm{\scriptsize 63}$,
M.~Germain$^\textrm{\scriptsize 116}$,
P.~Ghosh$^\textrm{\scriptsize 139}$,
S.K.~Ghosh$^\textrm{\scriptsize 4}$,
P.~Gianotti$^\textrm{\scriptsize 73}$,
P.~Giubellino$^\textrm{\scriptsize 34}$\textsuperscript{,}$^\textrm{\scriptsize 113}$,
P.~Giubilato$^\textrm{\scriptsize 28}$,
E.~Gladysz-Dziadus$^\textrm{\scriptsize 120}$,
P.~Gl\"{a}ssel$^\textrm{\scriptsize 96}$,
D.M.~Gom\'{e}z Coral$^\textrm{\scriptsize 64}$,
A.~Gomez Ramirez$^\textrm{\scriptsize 59}$,
A.S.~Gonzalez$^\textrm{\scriptsize 34}$,
V.~Gonzalez$^\textrm{\scriptsize 10}$,
P.~Gonz\'{a}lez-Zamora$^\textrm{\scriptsize 10}$,
S.~Gorbunov$^\textrm{\scriptsize 41}$,
L.~G\"{o}rlich$^\textrm{\scriptsize 120}$,
S.~Gotovac$^\textrm{\scriptsize 119}$,
V.~Grabski$^\textrm{\scriptsize 64}$,
L.K.~Graczykowski$^\textrm{\scriptsize 140}$,
K.L.~Graham$^\textrm{\scriptsize 104}$,
J.L.~Gramling$^\textrm{\scriptsize 96}$,
L.~Greiner$^\textrm{\scriptsize 75}$,
A.~Grelli$^\textrm{\scriptsize 53}$,
C.~Grigoras$^\textrm{\scriptsize 34}$,
V.~Grigoriev$^\textrm{\scriptsize 76}$,
A.~Grigoryan$^\textrm{\scriptsize 1}$,
S.~Grigoryan$^\textrm{\scriptsize 67}$,
N.~Grion$^\textrm{\scriptsize 112}$,
J.M.~Gronefeld$^\textrm{\scriptsize 100}$,
F.~Grosa$^\textrm{\scriptsize 30}$,
J.F.~Grosse-Oetringhaus$^\textrm{\scriptsize 34}$,
R.~Grosso$^\textrm{\scriptsize 100}$,
L.~Gruber$^\textrm{\scriptsize 115}$,
F.R.~Grull$^\textrm{\scriptsize 59}$,
F.~Guber$^\textrm{\scriptsize 52}$,
R.~Guernane$^\textrm{\scriptsize 34}$\textsuperscript{,}$^\textrm{\scriptsize 72}$,
B.~Guerzoni$^\textrm{\scriptsize 26}$,
K.~Gulbrandsen$^\textrm{\scriptsize 84}$,
T.~Gunji$^\textrm{\scriptsize 131}$,
A.~Gupta$^\textrm{\scriptsize 93}$,
R.~Gupta$^\textrm{\scriptsize 93}$,
I.B.~Guzman$^\textrm{\scriptsize 2}$,
R.~Haake$^\textrm{\scriptsize 34}$\textsuperscript{,}$^\textrm{\scriptsize 61}$,
C.~Hadjidakis$^\textrm{\scriptsize 51}$,
H.~Hamagaki$^\textrm{\scriptsize 77}$\textsuperscript{,}$^\textrm{\scriptsize 131}$,
G.~Hamar$^\textrm{\scriptsize 142}$,
J.C.~Hamon$^\textrm{\scriptsize 135}$,
J.W.~Harris$^\textrm{\scriptsize 143}$,
A.~Harton$^\textrm{\scriptsize 13}$,
D.~Hatzifotiadou$^\textrm{\scriptsize 107}$,
S.~Hayashi$^\textrm{\scriptsize 131}$,
S.T.~Heckel$^\textrm{\scriptsize 60}$,
E.~Hellb\"{a}r$^\textrm{\scriptsize 60}$,
H.~Helstrup$^\textrm{\scriptsize 36}$,
A.~Herghelegiu$^\textrm{\scriptsize 80}$,
G.~Herrera Corral$^\textrm{\scriptsize 11}$,
F.~Herrmann$^\textrm{\scriptsize 61}$,
B.A.~Hess$^\textrm{\scriptsize 95}$,
K.F.~Hetland$^\textrm{\scriptsize 36}$,
H.~Hillemanns$^\textrm{\scriptsize 34}$,
B.~Hippolyte$^\textrm{\scriptsize 135}$,
J.~Hladky$^\textrm{\scriptsize 56}$,
D.~Horak$^\textrm{\scriptsize 38}$,
R.~Hosokawa$^\textrm{\scriptsize 132}$,
P.~Hristov$^\textrm{\scriptsize 34}$,
C.~Hughes$^\textrm{\scriptsize 129}$,
T.J.~Humanic$^\textrm{\scriptsize 18}$,
N.~Hussain$^\textrm{\scriptsize 43}$,
T.~Hussain$^\textrm{\scriptsize 17}$,
D.~Hutter$^\textrm{\scriptsize 41}$,
D.S.~Hwang$^\textrm{\scriptsize 19}$,
R.~Ilkaev$^\textrm{\scriptsize 102}$,
M.~Inaba$^\textrm{\scriptsize 132}$,
M.~Ippolitov$^\textrm{\scriptsize 83}$\textsuperscript{,}$^\textrm{\scriptsize 76}$,
M.~Irfan$^\textrm{\scriptsize 17}$,
V.~Isakov$^\textrm{\scriptsize 52}$,
M.S.~Islam$^\textrm{\scriptsize 48}$,
M.~Ivanov$^\textrm{\scriptsize 34}$\textsuperscript{,}$^\textrm{\scriptsize 100}$,
V.~Ivanov$^\textrm{\scriptsize 89}$,
V.~Izucheev$^\textrm{\scriptsize 114}$,
B.~Jacak$^\textrm{\scriptsize 75}$,
N.~Jacazio$^\textrm{\scriptsize 26}$,
P.M.~Jacobs$^\textrm{\scriptsize 75}$,
M.B.~Jadhav$^\textrm{\scriptsize 47}$,
S.~Jadlovska$^\textrm{\scriptsize 118}$,
J.~Jadlovsky$^\textrm{\scriptsize 118}$,
C.~Jahnke$^\textrm{\scriptsize 35}$,
M.J.~Jakubowska$^\textrm{\scriptsize 140}$,
M.A.~Janik$^\textrm{\scriptsize 140}$,
P.H.S.Y.~Jayarathna$^\textrm{\scriptsize 126}$,
C.~Jena$^\textrm{\scriptsize 81}$,
S.~Jena$^\textrm{\scriptsize 126}$,
M.~Jercic$^\textrm{\scriptsize 133}$,
R.T.~Jimenez Bustamante$^\textrm{\scriptsize 100}$,
P.G.~Jones$^\textrm{\scriptsize 104}$,
A.~Jusko$^\textrm{\scriptsize 104}$,
P.~Kalinak$^\textrm{\scriptsize 55}$,
A.~Kalweit$^\textrm{\scriptsize 34}$,
J.H.~Kang$^\textrm{\scriptsize 144}$,
V.~Kaplin$^\textrm{\scriptsize 76}$,
S.~Kar$^\textrm{\scriptsize 139}$,
A.~Karasu Uysal$^\textrm{\scriptsize 70}$,
O.~Karavichev$^\textrm{\scriptsize 52}$,
T.~Karavicheva$^\textrm{\scriptsize 52}$,
L.~Karayan$^\textrm{\scriptsize 100}$\textsuperscript{,}$^\textrm{\scriptsize 96}$,
E.~Karpechev$^\textrm{\scriptsize 52}$,
U.~Kebschull$^\textrm{\scriptsize 59}$,
R.~Keidel$^\textrm{\scriptsize 145}$,
D.L.D.~Keijdener$^\textrm{\scriptsize 53}$,
M.~Keil$^\textrm{\scriptsize 34}$,
B.~Ketzer$^\textrm{\scriptsize 44}$,
M. Mohisin~Khan$^\textrm{\scriptsize 17}$\Aref{idp3207120},
P.~Khan$^\textrm{\scriptsize 103}$,
S.A.~Khan$^\textrm{\scriptsize 139}$,
A.~Khanzadeev$^\textrm{\scriptsize 89}$,
Y.~Kharlov$^\textrm{\scriptsize 114}$,
A.~Khatun$^\textrm{\scriptsize 17}$,
A.~Khuntia$^\textrm{\scriptsize 48}$,
M.M.~Kielbowicz$^\textrm{\scriptsize 120}$,
B.~Kileng$^\textrm{\scriptsize 36}$,
D.W.~Kim$^\textrm{\scriptsize 42}$,
D.J.~Kim$^\textrm{\scriptsize 127}$,
D.~Kim$^\textrm{\scriptsize 144}$,
H.~Kim$^\textrm{\scriptsize 144}$,
J.S.~Kim$^\textrm{\scriptsize 42}$,
J.~Kim$^\textrm{\scriptsize 96}$,
M.~Kim$^\textrm{\scriptsize 50}$,
M.~Kim$^\textrm{\scriptsize 144}$,
S.~Kim$^\textrm{\scriptsize 19}$,
T.~Kim$^\textrm{\scriptsize 144}$,
S.~Kirsch$^\textrm{\scriptsize 41}$,
I.~Kisel$^\textrm{\scriptsize 41}$,
S.~Kiselev$^\textrm{\scriptsize 54}$,
A.~Kisiel$^\textrm{\scriptsize 140}$,
G.~Kiss$^\textrm{\scriptsize 142}$,
J.L.~Klay$^\textrm{\scriptsize 6}$,
C.~Klein$^\textrm{\scriptsize 60}$,
J.~Klein$^\textrm{\scriptsize 34}$,
C.~Klein-B\"{o}sing$^\textrm{\scriptsize 61}$,
S.~Klewin$^\textrm{\scriptsize 96}$,
A.~Kluge$^\textrm{\scriptsize 34}$,
M.L.~Knichel$^\textrm{\scriptsize 96}$,
A.G.~Knospe$^\textrm{\scriptsize 126}$,
C.~Kobdaj$^\textrm{\scriptsize 117}$,
M.~Kofarago$^\textrm{\scriptsize 34}$,
T.~Kollegger$^\textrm{\scriptsize 100}$,
A.~Kolojvari$^\textrm{\scriptsize 138}$,
V.~Kondratiev$^\textrm{\scriptsize 138}$,
N.~Kondratyeva$^\textrm{\scriptsize 76}$,
E.~Kondratyuk$^\textrm{\scriptsize 114}$,
A.~Konevskikh$^\textrm{\scriptsize 52}$,
M.~Kopcik$^\textrm{\scriptsize 118}$,
M.~Kour$^\textrm{\scriptsize 93}$,
C.~Kouzinopoulos$^\textrm{\scriptsize 34}$,
O.~Kovalenko$^\textrm{\scriptsize 79}$,
V.~Kovalenko$^\textrm{\scriptsize 138}$,
M.~Kowalski$^\textrm{\scriptsize 120}$,
G.~Koyithatta Meethaleveedu$^\textrm{\scriptsize 47}$,
I.~Kr\'{a}lik$^\textrm{\scriptsize 55}$,
A.~Krav\v{c}\'{a}kov\'{a}$^\textrm{\scriptsize 39}$,
M.~Krivda$^\textrm{\scriptsize 55}$\textsuperscript{,}$^\textrm{\scriptsize 104}$,
F.~Krizek$^\textrm{\scriptsize 87}$,
E.~Kryshen$^\textrm{\scriptsize 89}$,
M.~Krzewicki$^\textrm{\scriptsize 41}$,
A.M.~Kubera$^\textrm{\scriptsize 18}$,
V.~Ku\v{c}era$^\textrm{\scriptsize 87}$,
C.~Kuhn$^\textrm{\scriptsize 135}$,
P.G.~Kuijer$^\textrm{\scriptsize 85}$,
A.~Kumar$^\textrm{\scriptsize 93}$,
J.~Kumar$^\textrm{\scriptsize 47}$,
L.~Kumar$^\textrm{\scriptsize 91}$,
S.~Kumar$^\textrm{\scriptsize 47}$,
S.~Kundu$^\textrm{\scriptsize 81}$,
P.~Kurashvili$^\textrm{\scriptsize 79}$,
A.~Kurepin$^\textrm{\scriptsize 52}$,
A.B.~Kurepin$^\textrm{\scriptsize 52}$,
A.~Kuryakin$^\textrm{\scriptsize 102}$,
S.~Kushpil$^\textrm{\scriptsize 87}$,
M.J.~Kweon$^\textrm{\scriptsize 50}$,
Y.~Kwon$^\textrm{\scriptsize 144}$,
S.L.~La Pointe$^\textrm{\scriptsize 41}$,
P.~La Rocca$^\textrm{\scriptsize 27}$,
C.~Lagana Fernandes$^\textrm{\scriptsize 123}$,
I.~Lakomov$^\textrm{\scriptsize 34}$,
R.~Langoy$^\textrm{\scriptsize 40}$,
K.~Lapidus$^\textrm{\scriptsize 143}$,
C.~Lara$^\textrm{\scriptsize 59}$,
A.~Lardeux$^\textrm{\scriptsize 20}$\textsuperscript{,}$^\textrm{\scriptsize 65}$,
A.~Lattuca$^\textrm{\scriptsize 25}$,
E.~Laudi$^\textrm{\scriptsize 34}$,
R.~Lavicka$^\textrm{\scriptsize 38}$,
L.~Lazaridis$^\textrm{\scriptsize 34}$,
R.~Lea$^\textrm{\scriptsize 24}$,
L.~Leardini$^\textrm{\scriptsize 96}$,
S.~Lee$^\textrm{\scriptsize 144}$,
F.~Lehas$^\textrm{\scriptsize 85}$,
S.~Lehner$^\textrm{\scriptsize 115}$,
J.~Lehrbach$^\textrm{\scriptsize 41}$,
R.C.~Lemmon$^\textrm{\scriptsize 86}$,
V.~Lenti$^\textrm{\scriptsize 106}$,
E.~Leogrande$^\textrm{\scriptsize 53}$,
I.~Le\'{o}n Monz\'{o}n$^\textrm{\scriptsize 122}$,
P.~L\'{e}vai$^\textrm{\scriptsize 142}$,
S.~Li$^\textrm{\scriptsize 7}$,
X.~Li$^\textrm{\scriptsize 14}$,
J.~Lien$^\textrm{\scriptsize 40}$,
R.~Lietava$^\textrm{\scriptsize 104}$,
S.~Lindal$^\textrm{\scriptsize 20}$,
V.~Lindenstruth$^\textrm{\scriptsize 41}$,
C.~Lippmann$^\textrm{\scriptsize 100}$,
M.A.~Lisa$^\textrm{\scriptsize 18}$,
V.~Litichevskyi$^\textrm{\scriptsize 45}$,
H.M.~Ljunggren$^\textrm{\scriptsize 33}$,
W.J.~Llope$^\textrm{\scriptsize 141}$,
D.F.~Lodato$^\textrm{\scriptsize 53}$,
V.R.~Loggins$^\textrm{\scriptsize 141}$,
P.I.~Loenne$^\textrm{\scriptsize 21}$,
V.~Loginov$^\textrm{\scriptsize 76}$,
C.~Loizides$^\textrm{\scriptsize 75}$,
P.~Loncar$^\textrm{\scriptsize 119}$,
X.~Lopez$^\textrm{\scriptsize 71}$,
E.~L\'{o}pez Torres$^\textrm{\scriptsize 9}$,
A.~Lowe$^\textrm{\scriptsize 142}$,
P.~Luettig$^\textrm{\scriptsize 60}$,
M.~Lunardon$^\textrm{\scriptsize 28}$,
G.~Luparello$^\textrm{\scriptsize 24}$,
M.~Lupi$^\textrm{\scriptsize 34}$,
T.H.~Lutz$^\textrm{\scriptsize 143}$,
A.~Maevskaya$^\textrm{\scriptsize 52}$,
M.~Mager$^\textrm{\scriptsize 34}$,
S.~Mahajan$^\textrm{\scriptsize 93}$,
S.M.~Mahmood$^\textrm{\scriptsize 20}$,
A.~Maire$^\textrm{\scriptsize 135}$,
R.D.~Majka$^\textrm{\scriptsize 143}$,
M.~Malaev$^\textrm{\scriptsize 89}$,
I.~Maldonado Cervantes$^\textrm{\scriptsize 62}$,
L.~Malinina$^\textrm{\scriptsize 67}$\Aref{idp3984928},
D.~Mal'Kevich$^\textrm{\scriptsize 54}$,
P.~Malzacher$^\textrm{\scriptsize 100}$,
A.~Mamonov$^\textrm{\scriptsize 102}$,
V.~Manko$^\textrm{\scriptsize 83}$,
F.~Manso$^\textrm{\scriptsize 71}$,
V.~Manzari$^\textrm{\scriptsize 106}$,
Y.~Mao$^\textrm{\scriptsize 7}$,
M.~Marchisone$^\textrm{\scriptsize 66}$\textsuperscript{,}$^\textrm{\scriptsize 130}$,
J.~Mare\v{s}$^\textrm{\scriptsize 56}$,
G.V.~Margagliotti$^\textrm{\scriptsize 24}$,
A.~Margotti$^\textrm{\scriptsize 107}$,
J.~Margutti$^\textrm{\scriptsize 53}$,
A.~Mar\'{\i}n$^\textrm{\scriptsize 100}$,
C.~Markert$^\textrm{\scriptsize 121}$,
M.~Marquard$^\textrm{\scriptsize 60}$,
N.A.~Martin$^\textrm{\scriptsize 100}$,
P.~Martinengo$^\textrm{\scriptsize 34}$,
J.A.L.~Martinez$^\textrm{\scriptsize 59}$,
M.I.~Mart\'{\i}nez$^\textrm{\scriptsize 2}$,
G.~Mart\'{\i}nez Garc\'{\i}a$^\textrm{\scriptsize 116}$,
M.~Martinez Pedreira$^\textrm{\scriptsize 34}$,
A.~Mas$^\textrm{\scriptsize 123}$,
S.~Masciocchi$^\textrm{\scriptsize 100}$,
M.~Masera$^\textrm{\scriptsize 25}$,
A.~Masoni$^\textrm{\scriptsize 108}$,
A.~Mastroserio$^\textrm{\scriptsize 32}$,
A.M.~Mathis$^\textrm{\scriptsize 97}$\textsuperscript{,}$^\textrm{\scriptsize 35}$,
A.~Matyja$^\textrm{\scriptsize 120}$\textsuperscript{,}$^\textrm{\scriptsize 129}$,
C.~Mayer$^\textrm{\scriptsize 120}$,
J.~Mazer$^\textrm{\scriptsize 129}$,
M.~Mazzilli$^\textrm{\scriptsize 32}$,
M.A.~Mazzoni$^\textrm{\scriptsize 111}$,
F.~Meddi$^\textrm{\scriptsize 22}$,
Y.~Melikyan$^\textrm{\scriptsize 76}$,
A.~Menchaca-Rocha$^\textrm{\scriptsize 64}$,
E.~Meninno$^\textrm{\scriptsize 29}$,
J.~Mercado P\'erez$^\textrm{\scriptsize 96}$,
M.~Meres$^\textrm{\scriptsize 37}$,
S.~Mhlanga$^\textrm{\scriptsize 92}$,
Y.~Miake$^\textrm{\scriptsize 132}$,
M.M.~Mieskolainen$^\textrm{\scriptsize 45}$,
D.~Mihaylov$^\textrm{\scriptsize 97}$,
K.~Mikhaylov$^\textrm{\scriptsize 67}$\textsuperscript{,}$^\textrm{\scriptsize 54}$,
L.~Milano$^\textrm{\scriptsize 75}$,
J.~Milosevic$^\textrm{\scriptsize 20}$,
A.~Mischke$^\textrm{\scriptsize 53}$,
A.N.~Mishra$^\textrm{\scriptsize 48}$,
D.~Mi\'{s}kowiec$^\textrm{\scriptsize 100}$,
J.~Mitra$^\textrm{\scriptsize 139}$,
C.M.~Mitu$^\textrm{\scriptsize 58}$,
N.~Mohammadi$^\textrm{\scriptsize 53}$,
B.~Mohanty$^\textrm{\scriptsize 81}$,
E.~Montes$^\textrm{\scriptsize 10}$,
D.A.~Moreira De Godoy$^\textrm{\scriptsize 61}$,
L.A.P.~Moreno$^\textrm{\scriptsize 2}$,
S.~Moretto$^\textrm{\scriptsize 28}$,
A.~Morreale$^\textrm{\scriptsize 116}$,
A.~Morsch$^\textrm{\scriptsize 34}$,
V.~Muccifora$^\textrm{\scriptsize 73}$,
E.~Mudnic$^\textrm{\scriptsize 119}$,
D.~M{\"u}hlheim$^\textrm{\scriptsize 61}$,
S.~Muhuri$^\textrm{\scriptsize 139}$,
M.~Mukherjee$^\textrm{\scriptsize 139}$,
J.D.~Mulligan$^\textrm{\scriptsize 143}$,
M.G.~Munhoz$^\textrm{\scriptsize 123}$,
K.~M\"{u}nning$^\textrm{\scriptsize 44}$,
R.H.~Munzer$^\textrm{\scriptsize 35}$\textsuperscript{,}$^\textrm{\scriptsize 97}$\textsuperscript{,}$^\textrm{\scriptsize 60}$,
H.~Murakami$^\textrm{\scriptsize 131}$,
S.~Murray$^\textrm{\scriptsize 66}$,
L.~Musa$^\textrm{\scriptsize 34}$,
J.~Musinsky$^\textrm{\scriptsize 55}$,
C.J.~Myers$^\textrm{\scriptsize 126}$,
B.~Naik$^\textrm{\scriptsize 47}$,
R.~Nair$^\textrm{\scriptsize 79}$,
B.K.~Nandi$^\textrm{\scriptsize 47}$,
R.~Nania$^\textrm{\scriptsize 107}$,
E.~Nappi$^\textrm{\scriptsize 106}$,
M.U.~Naru$^\textrm{\scriptsize 15}$,
H.~Natal da Luz$^\textrm{\scriptsize 123}$,
C.~Nattrass$^\textrm{\scriptsize 129}$,
S.R.~Navarro$^\textrm{\scriptsize 2}$,
K.~Nayak$^\textrm{\scriptsize 81}$,
R.~Nayak$^\textrm{\scriptsize 47}$,
T.K.~Nayak$^\textrm{\scriptsize 139}$,
S.~Nazarenko$^\textrm{\scriptsize 102}$,
A.~Nedosekin$^\textrm{\scriptsize 54}$,
R.A.~Negrao De Oliveira$^\textrm{\scriptsize 34}$,
L.~Nellen$^\textrm{\scriptsize 62}$,
S.V.~Nesbo$^\textrm{\scriptsize 36}$,
F.~Ng$^\textrm{\scriptsize 126}$,
M.~Nicassio$^\textrm{\scriptsize 100}$,
M.~Niculescu$^\textrm{\scriptsize 58}$,
J.~Niedziela$^\textrm{\scriptsize 34}$,
B.S.~Nielsen$^\textrm{\scriptsize 84}$,
S.~Nikolaev$^\textrm{\scriptsize 83}$,
S.~Nikulin$^\textrm{\scriptsize 83}$,
V.~Nikulin$^\textrm{\scriptsize 89}$,
F.~Noferini$^\textrm{\scriptsize 107}$\textsuperscript{,}$^\textrm{\scriptsize 12}$,
P.~Nomokonov$^\textrm{\scriptsize 67}$,
G.~Nooren$^\textrm{\scriptsize 53}$,
J.C.C.~Noris$^\textrm{\scriptsize 2}$,
J.~Norman$^\textrm{\scriptsize 128}$,
A.~Nyanin$^\textrm{\scriptsize 83}$,
J.~Nystrand$^\textrm{\scriptsize 21}$,
H.~Oeschler$^\textrm{\scriptsize 96}$,
S.~Oh$^\textrm{\scriptsize 143}$,
A.~Ohlson$^\textrm{\scriptsize 96}$\textsuperscript{,}$^\textrm{\scriptsize 34}$,
T.~Okubo$^\textrm{\scriptsize 46}$,
L.~Olah$^\textrm{\scriptsize 142}$,
J.~Oleniacz$^\textrm{\scriptsize 140}$,
A.C.~Oliveira Da Silva$^\textrm{\scriptsize 123}$,
M.H.~Oliver$^\textrm{\scriptsize 143}$,
J.~Onderwaater$^\textrm{\scriptsize 100}$,
C.~Oppedisano$^\textrm{\scriptsize 113}$,
R.~Orava$^\textrm{\scriptsize 45}$,
M.~Oravec$^\textrm{\scriptsize 118}$,
A.~Ortiz Velasquez$^\textrm{\scriptsize 62}$,
A.~Oskarsson$^\textrm{\scriptsize 33}$,
J.~Otwinowski$^\textrm{\scriptsize 120}$,
K.~Oyama$^\textrm{\scriptsize 77}$,
M.~Ozdemir$^\textrm{\scriptsize 60}$,
Y.~Pachmayer$^\textrm{\scriptsize 96}$,
V.~Pacik$^\textrm{\scriptsize 84}$,
D.~Pagano$^\textrm{\scriptsize 137}$,
P.~Pagano$^\textrm{\scriptsize 29}$,
G.~Pai\'{c}$^\textrm{\scriptsize 62}$,
S.K.~Pal$^\textrm{\scriptsize 139}$,
P.~Palni$^\textrm{\scriptsize 7}$,
J.~Pan$^\textrm{\scriptsize 141}$,
A.K.~Pandey$^\textrm{\scriptsize 47}$,
S.~Panebianco$^\textrm{\scriptsize 65}$,
V.~Papikyan$^\textrm{\scriptsize 1}$,
G.S.~Pappalardo$^\textrm{\scriptsize 109}$,
P.~Pareek$^\textrm{\scriptsize 48}$,
J.~Park$^\textrm{\scriptsize 50}$,
W.J.~Park$^\textrm{\scriptsize 100}$,
S.~Parmar$^\textrm{\scriptsize 91}$,
A.~Passfeld$^\textrm{\scriptsize 61}$,
S.P.~Pathak$^\textrm{\scriptsize 126}$,
V.~Paticchio$^\textrm{\scriptsize 106}$,
R.N.~Patra$^\textrm{\scriptsize 139}$,
B.~Paul$^\textrm{\scriptsize 113}$,
H.~Pei$^\textrm{\scriptsize 7}$,
T.~Peitzmann$^\textrm{\scriptsize 53}$,
X.~Peng$^\textrm{\scriptsize 7}$,
L.G.~Pereira$^\textrm{\scriptsize 63}$,
H.~Pereira Da Costa$^\textrm{\scriptsize 65}$,
D.~Peresunko$^\textrm{\scriptsize 83}$\textsuperscript{,}$^\textrm{\scriptsize 76}$,
E.~Perez Lezama$^\textrm{\scriptsize 60}$,
V.~Peskov$^\textrm{\scriptsize 60}$,
Y.~Pestov$^\textrm{\scriptsize 5}$,
V.~Petr\'{a}\v{c}ek$^\textrm{\scriptsize 38}$,
V.~Petrov$^\textrm{\scriptsize 114}$,
M.~Petrovici$^\textrm{\scriptsize 80}$,
C.~Petta$^\textrm{\scriptsize 27}$,
R.P.~Pezzi$^\textrm{\scriptsize 63}$,
S.~Piano$^\textrm{\scriptsize 112}$,
M.~Pikna$^\textrm{\scriptsize 37}$,
P.~Pillot$^\textrm{\scriptsize 116}$,
L.O.D.L.~Pimentel$^\textrm{\scriptsize 84}$,
O.~Pinazza$^\textrm{\scriptsize 107}$\textsuperscript{,}$^\textrm{\scriptsize 34}$,
L.~Pinsky$^\textrm{\scriptsize 126}$,
D.B.~Piyarathna$^\textrm{\scriptsize 126}$,
M.~P\l osko\'{n}$^\textrm{\scriptsize 75}$,
M.~Planinic$^\textrm{\scriptsize 133}$,
J.~Pluta$^\textrm{\scriptsize 140}$,
S.~Pochybova$^\textrm{\scriptsize 142}$,
P.L.M.~Podesta-Lerma$^\textrm{\scriptsize 122}$,
M.G.~Poghosyan$^\textrm{\scriptsize 88}$,
B.~Polichtchouk$^\textrm{\scriptsize 114}$,
N.~Poljak$^\textrm{\scriptsize 133}$,
W.~Poonsawat$^\textrm{\scriptsize 117}$,
A.~Pop$^\textrm{\scriptsize 80}$,
H.~Poppenborg$^\textrm{\scriptsize 61}$,
S.~Porteboeuf-Houssais$^\textrm{\scriptsize 71}$,
J.~Porter$^\textrm{\scriptsize 75}$,
J.~Pospisil$^\textrm{\scriptsize 87}$,
V.~Pozdniakov$^\textrm{\scriptsize 67}$,
S.K.~Prasad$^\textrm{\scriptsize 4}$,
R.~Preghenella$^\textrm{\scriptsize 34}$\textsuperscript{,}$^\textrm{\scriptsize 107}$,
F.~Prino$^\textrm{\scriptsize 113}$,
C.A.~Pruneau$^\textrm{\scriptsize 141}$,
I.~Pshenichnov$^\textrm{\scriptsize 52}$,
M.~Puccio$^\textrm{\scriptsize 25}$,
G.~Puddu$^\textrm{\scriptsize 23}$,
P.~Pujahari$^\textrm{\scriptsize 141}$,
V.~Punin$^\textrm{\scriptsize 102}$,
J.~Putschke$^\textrm{\scriptsize 141}$,
H.~Qvigstad$^\textrm{\scriptsize 20}$,
A.~Rachevski$^\textrm{\scriptsize 112}$,
S.~Raha$^\textrm{\scriptsize 4}$,
S.~Rajput$^\textrm{\scriptsize 93}$,
J.~Rak$^\textrm{\scriptsize 127}$,
A.~Rakotozafindrabe$^\textrm{\scriptsize 65}$,
L.~Ramello$^\textrm{\scriptsize 31}$,
F.~Rami$^\textrm{\scriptsize 135}$,
D.B.~Rana$^\textrm{\scriptsize 126}$,
R.~Raniwala$^\textrm{\scriptsize 94}$,
S.~Raniwala$^\textrm{\scriptsize 94}$,
S.S.~R\"{a}s\"{a}nen$^\textrm{\scriptsize 45}$,
B.T.~Rascanu$^\textrm{\scriptsize 60}$,
D.~Rathee$^\textrm{\scriptsize 91}$,
V.~Ratza$^\textrm{\scriptsize 44}$,
I.~Ravasenga$^\textrm{\scriptsize 30}$,
K.F.~Read$^\textrm{\scriptsize 88}$\textsuperscript{,}$^\textrm{\scriptsize 129}$,
K.~Redlich$^\textrm{\scriptsize 79}$,
A.~Rehman$^\textrm{\scriptsize 21}$,
P.~Reichelt$^\textrm{\scriptsize 60}$,
F.~Reidt$^\textrm{\scriptsize 34}$,
X.~Ren$^\textrm{\scriptsize 7}$,
R.~Renfordt$^\textrm{\scriptsize 60}$,
A.R.~Reolon$^\textrm{\scriptsize 73}$,
A.~Reshetin$^\textrm{\scriptsize 52}$,
K.~Reygers$^\textrm{\scriptsize 96}$,
V.~Riabov$^\textrm{\scriptsize 89}$,
R.A.~Ricci$^\textrm{\scriptsize 74}$,
T.~Richert$^\textrm{\scriptsize 53}$\textsuperscript{,}$^\textrm{\scriptsize 33}$,
M.~Richter$^\textrm{\scriptsize 20}$,
P.~Riedler$^\textrm{\scriptsize 34}$,
W.~Riegler$^\textrm{\scriptsize 34}$,
F.~Riggi$^\textrm{\scriptsize 27}$,
C.~Ristea$^\textrm{\scriptsize 58}$,
M.~Rodr\'{i}guez Cahuantzi$^\textrm{\scriptsize 2}$,
K.~R{\o}ed$^\textrm{\scriptsize 20}$,
E.~Rogochaya$^\textrm{\scriptsize 67}$,
D.~Rohr$^\textrm{\scriptsize 41}$,
D.~R\"ohrich$^\textrm{\scriptsize 21}$,
P.S.~Rokita$^\textrm{\scriptsize 140}$,
F.~Ronchetti$^\textrm{\scriptsize 34}$\textsuperscript{,}$^\textrm{\scriptsize 73}$,
L.~Ronflette$^\textrm{\scriptsize 116}$,
P.~Rosnet$^\textrm{\scriptsize 71}$,
A.~Rossi$^\textrm{\scriptsize 28}$,
A.~Rotondi$^\textrm{\scriptsize 136}$,
F.~Roukoutakis$^\textrm{\scriptsize 78}$,
A.~Roy$^\textrm{\scriptsize 48}$,
C.~Roy$^\textrm{\scriptsize 135}$,
P.~Roy$^\textrm{\scriptsize 103}$,
A.J.~Rubio Montero$^\textrm{\scriptsize 10}$,
R.~Rui$^\textrm{\scriptsize 24}$,
R.~Russo$^\textrm{\scriptsize 25}$,
A.~Rustamov$^\textrm{\scriptsize 82}$,
E.~Ryabinkin$^\textrm{\scriptsize 83}$,
Y.~Ryabov$^\textrm{\scriptsize 89}$,
A.~Rybicki$^\textrm{\scriptsize 120}$,
S.~Saarinen$^\textrm{\scriptsize 45}$,
S.~Sadhu$^\textrm{\scriptsize 139}$,
S.~Sadovsky$^\textrm{\scriptsize 114}$,
K.~\v{S}afa\v{r}\'{\i}k$^\textrm{\scriptsize 34}$,
S.K.~Saha$^\textrm{\scriptsize 139}$,
B.~Sahlmuller$^\textrm{\scriptsize 60}$,
B.~Sahoo$^\textrm{\scriptsize 47}$,
P.~Sahoo$^\textrm{\scriptsize 48}$,
R.~Sahoo$^\textrm{\scriptsize 48}$,
S.~Sahoo$^\textrm{\scriptsize 57}$,
P.K.~Sahu$^\textrm{\scriptsize 57}$,
J.~Saini$^\textrm{\scriptsize 139}$,
S.~Sakai$^\textrm{\scriptsize 73}$\textsuperscript{,}$^\textrm{\scriptsize 132}$,
M.A.~Saleh$^\textrm{\scriptsize 141}$,
J.~Salzwedel$^\textrm{\scriptsize 18}$,
S.~Sambyal$^\textrm{\scriptsize 93}$,
V.~Samsonov$^\textrm{\scriptsize 76}$\textsuperscript{,}$^\textrm{\scriptsize 89}$,
A.~Sandoval$^\textrm{\scriptsize 64}$,
D.~Sarkar$^\textrm{\scriptsize 139}$,
N.~Sarkar$^\textrm{\scriptsize 139}$,
P.~Sarma$^\textrm{\scriptsize 43}$,
M.H.P.~Sas$^\textrm{\scriptsize 53}$,
E.~Scapparone$^\textrm{\scriptsize 107}$,
F.~Scarlassara$^\textrm{\scriptsize 28}$,
R.P.~Scharenberg$^\textrm{\scriptsize 98}$,
H.S.~Scheid$^\textrm{\scriptsize 60}$,
C.~Schiaua$^\textrm{\scriptsize 80}$,
R.~Schicker$^\textrm{\scriptsize 96}$,
C.~Schmidt$^\textrm{\scriptsize 100}$,
H.R.~Schmidt$^\textrm{\scriptsize 95}$,
M.O.~Schmidt$^\textrm{\scriptsize 96}$,
M.~Schmidt$^\textrm{\scriptsize 95}$,
J.~Schukraft$^\textrm{\scriptsize 34}$,
Y.~Schutz$^\textrm{\scriptsize 116}$\textsuperscript{,}$^\textrm{\scriptsize 135}$\textsuperscript{,}$^\textrm{\scriptsize 34}$,
K.~Schwarz$^\textrm{\scriptsize 100}$,
K.~Schweda$^\textrm{\scriptsize 100}$,
G.~Scioli$^\textrm{\scriptsize 26}$,
E.~Scomparin$^\textrm{\scriptsize 113}$,
R.~Scott$^\textrm{\scriptsize 129}$,
M.~\v{S}ef\v{c}\'ik$^\textrm{\scriptsize 39}$,
J.E.~Seger$^\textrm{\scriptsize 90}$,
Y.~Sekiguchi$^\textrm{\scriptsize 131}$,
D.~Sekihata$^\textrm{\scriptsize 46}$,
I.~Selyuzhenkov$^\textrm{\scriptsize 76}$\textsuperscript{,}$^\textrm{\scriptsize 100}$,
K.~Senosi$^\textrm{\scriptsize 66}$,
S.~Senyukov$^\textrm{\scriptsize 3}$\textsuperscript{,}$^\textrm{\scriptsize 135}$\textsuperscript{,}$^\textrm{\scriptsize 34}$,
E.~Serradilla$^\textrm{\scriptsize 64}$\textsuperscript{,}$^\textrm{\scriptsize 10}$,
P.~Sett$^\textrm{\scriptsize 47}$,
A.~Sevcenco$^\textrm{\scriptsize 58}$,
A.~Shabanov$^\textrm{\scriptsize 52}$,
A.~Shabetai$^\textrm{\scriptsize 116}$,
O.~Shadura$^\textrm{\scriptsize 3}$,
R.~Shahoyan$^\textrm{\scriptsize 34}$,
A.~Shangaraev$^\textrm{\scriptsize 114}$,
A.~Sharma$^\textrm{\scriptsize 93}$,
A.~Sharma$^\textrm{\scriptsize 91}$,
M.~Sharma$^\textrm{\scriptsize 93}$,
M.~Sharma$^\textrm{\scriptsize 93}$,
N.~Sharma$^\textrm{\scriptsize 129}$\textsuperscript{,}$^\textrm{\scriptsize 91}$,
A.I.~Sheikh$^\textrm{\scriptsize 139}$,
K.~Shigaki$^\textrm{\scriptsize 46}$,
Q.~Shou$^\textrm{\scriptsize 7}$,
K.~Shtejer$^\textrm{\scriptsize 25}$\textsuperscript{,}$^\textrm{\scriptsize 9}$,
Y.~Sibiriak$^\textrm{\scriptsize 83}$,
S.~Siddhanta$^\textrm{\scriptsize 108}$,
K.M.~Sielewicz$^\textrm{\scriptsize 34}$,
T.~Siemiarczuk$^\textrm{\scriptsize 79}$,
D.~Silvermyr$^\textrm{\scriptsize 33}$,
C.~Silvestre$^\textrm{\scriptsize 72}$,
G.~Simatovic$^\textrm{\scriptsize 133}$,
G.~Simonetti$^\textrm{\scriptsize 34}$,
R.~Singaraju$^\textrm{\scriptsize 139}$,
R.~Singh$^\textrm{\scriptsize 81}$,
V.~Singhal$^\textrm{\scriptsize 139}$,
T.~Sinha$^\textrm{\scriptsize 103}$,
B.~Sitar$^\textrm{\scriptsize 37}$,
M.~Sitta$^\textrm{\scriptsize 31}$,
T.B.~Skaali$^\textrm{\scriptsize 20}$,
M.~Slupecki$^\textrm{\scriptsize 127}$,
N.~Smirnov$^\textrm{\scriptsize 143}$,
R.J.M.~Snellings$^\textrm{\scriptsize 53}$,
T.W.~Snellman$^\textrm{\scriptsize 127}$,
J.~Song$^\textrm{\scriptsize 99}$,
M.~Song$^\textrm{\scriptsize 144}$,
F.~Soramel$^\textrm{\scriptsize 28}$,
S.~Sorensen$^\textrm{\scriptsize 129}$,
F.~Sozzi$^\textrm{\scriptsize 100}$,
E.~Spiriti$^\textrm{\scriptsize 73}$,
I.~Sputowska$^\textrm{\scriptsize 120}$,
B.K.~Srivastava$^\textrm{\scriptsize 98}$,
J.~Stachel$^\textrm{\scriptsize 96}$,
I.~Stan$^\textrm{\scriptsize 58}$,
P.~Stankus$^\textrm{\scriptsize 88}$,
E.~Stenlund$^\textrm{\scriptsize 33}$,
J.H.~Stiller$^\textrm{\scriptsize 96}$,
D.~Stocco$^\textrm{\scriptsize 116}$,
P.~Strmen$^\textrm{\scriptsize 37}$,
A.A.P.~Suaide$^\textrm{\scriptsize 123}$,
T.~Sugitate$^\textrm{\scriptsize 46}$,
C.~Suire$^\textrm{\scriptsize 51}$,
M.~Suleymanov$^\textrm{\scriptsize 15}$,
M.~Suljic$^\textrm{\scriptsize 24}$,
R.~Sultanov$^\textrm{\scriptsize 54}$,
M.~\v{S}umbera$^\textrm{\scriptsize 87}$,
S.~Sumowidagdo$^\textrm{\scriptsize 49}$,
K.~Suzuki$^\textrm{\scriptsize 115}$,
S.~Swain$^\textrm{\scriptsize 57}$,
A.~Szabo$^\textrm{\scriptsize 37}$,
I.~Szarka$^\textrm{\scriptsize 37}$,
A.~Szczepankiewicz$^\textrm{\scriptsize 140}$,
M.~Szymanski$^\textrm{\scriptsize 140}$,
U.~Tabassam$^\textrm{\scriptsize 15}$,
J.~Takahashi$^\textrm{\scriptsize 124}$,
G.J.~Tambave$^\textrm{\scriptsize 21}$,
N.~Tanaka$^\textrm{\scriptsize 132}$,
M.~Tarhini$^\textrm{\scriptsize 51}$,
M.~Tariq$^\textrm{\scriptsize 17}$,
M.G.~Tarzila$^\textrm{\scriptsize 80}$,
A.~Tauro$^\textrm{\scriptsize 34}$,
G.~Tejeda Mu\~{n}oz$^\textrm{\scriptsize 2}$,
A.~Telesca$^\textrm{\scriptsize 34}$,
K.~Terasaki$^\textrm{\scriptsize 131}$,
C.~Terrevoli$^\textrm{\scriptsize 28}$,
B.~Teyssier$^\textrm{\scriptsize 134}$,
D.~Thakur$^\textrm{\scriptsize 48}$,
S.~Thakur$^\textrm{\scriptsize 139}$,
D.~Thomas$^\textrm{\scriptsize 121}$,
R.~Tieulent$^\textrm{\scriptsize 134}$,
A.~Tikhonov$^\textrm{\scriptsize 52}$,
A.R.~Timmins$^\textrm{\scriptsize 126}$,
A.~Toia$^\textrm{\scriptsize 60}$,
S.~Tripathy$^\textrm{\scriptsize 48}$,
S.~Trogolo$^\textrm{\scriptsize 25}$,
G.~Trombetta$^\textrm{\scriptsize 32}$,
V.~Trubnikov$^\textrm{\scriptsize 3}$,
W.H.~Trzaska$^\textrm{\scriptsize 127}$,
B.A.~Trzeciak$^\textrm{\scriptsize 53}$,
T.~Tsuji$^\textrm{\scriptsize 131}$,
A.~Tumkin$^\textrm{\scriptsize 102}$,
R.~Turrisi$^\textrm{\scriptsize 110}$,
T.S.~Tveter$^\textrm{\scriptsize 20}$,
K.~Ullaland$^\textrm{\scriptsize 21}$,
E.N.~Umaka$^\textrm{\scriptsize 126}$,
A.~Uras$^\textrm{\scriptsize 134}$,
G.L.~Usai$^\textrm{\scriptsize 23}$,
A.~Utrobicic$^\textrm{\scriptsize 133}$,
M.~Vala$^\textrm{\scriptsize 118}$\textsuperscript{,}$^\textrm{\scriptsize 55}$,
J.~Van Der Maarel$^\textrm{\scriptsize 53}$,
J.W.~Van Hoorne$^\textrm{\scriptsize 34}$,
M.~van Leeuwen$^\textrm{\scriptsize 53}$,
T.~Vanat$^\textrm{\scriptsize 87}$,
P.~Vande Vyvre$^\textrm{\scriptsize 34}$,
D.~Varga$^\textrm{\scriptsize 142}$,
A.~Vargas$^\textrm{\scriptsize 2}$,
M.~Vargyas$^\textrm{\scriptsize 127}$,
R.~Varma$^\textrm{\scriptsize 47}$,
M.~Vasileiou$^\textrm{\scriptsize 78}$,
A.~Vasiliev$^\textrm{\scriptsize 83}$,
A.~Vauthier$^\textrm{\scriptsize 72}$,
O.~V\'azquez Doce$^\textrm{\scriptsize 97}$\textsuperscript{,}$^\textrm{\scriptsize 35}$,
V.~Vechernin$^\textrm{\scriptsize 138}$,
A.M.~Veen$^\textrm{\scriptsize 53}$,
A.~Velure$^\textrm{\scriptsize 21}$,
E.~Vercellin$^\textrm{\scriptsize 25}$,
S.~Vergara Lim\'on$^\textrm{\scriptsize 2}$,
R.~Vernet$^\textrm{\scriptsize 8}$,
R.~V\'ertesi$^\textrm{\scriptsize 142}$,
L.~Vickovic$^\textrm{\scriptsize 119}$,
S.~Vigolo$^\textrm{\scriptsize 53}$,
J.~Viinikainen$^\textrm{\scriptsize 127}$,
Z.~Vilakazi$^\textrm{\scriptsize 130}$,
O.~Villalobos Baillie$^\textrm{\scriptsize 104}$,
A.~Villatoro Tello$^\textrm{\scriptsize 2}$,
A.~Vinogradov$^\textrm{\scriptsize 83}$,
L.~Vinogradov$^\textrm{\scriptsize 138}$,
T.~Virgili$^\textrm{\scriptsize 29}$,
V.~Vislavicius$^\textrm{\scriptsize 33}$,
A.~Vodopyanov$^\textrm{\scriptsize 67}$,
M.A.~V\"{o}lkl$^\textrm{\scriptsize 96}$,
K.~Voloshin$^\textrm{\scriptsize 54}$,
S.A.~Voloshin$^\textrm{\scriptsize 141}$,
G.~Volpe$^\textrm{\scriptsize 32}$,
B.~von Haller$^\textrm{\scriptsize 34}$,
I.~Vorobyev$^\textrm{\scriptsize 97}$\textsuperscript{,}$^\textrm{\scriptsize 35}$,
D.~Voscek$^\textrm{\scriptsize 118}$,
D.~Vranic$^\textrm{\scriptsize 34}$\textsuperscript{,}$^\textrm{\scriptsize 100}$,
J.~Vrl\'{a}kov\'{a}$^\textrm{\scriptsize 39}$,
B.~Wagner$^\textrm{\scriptsize 21}$,
J.~Wagner$^\textrm{\scriptsize 100}$,
H.~Wang$^\textrm{\scriptsize 53}$,
M.~Wang$^\textrm{\scriptsize 7}$,
D.~Watanabe$^\textrm{\scriptsize 132}$,
Y.~Watanabe$^\textrm{\scriptsize 131}$,
M.~Weber$^\textrm{\scriptsize 115}$,
S.G.~Weber$^\textrm{\scriptsize 100}$,
D.F.~Weiser$^\textrm{\scriptsize 96}$,
J.P.~Wessels$^\textrm{\scriptsize 61}$,
U.~Westerhoff$^\textrm{\scriptsize 61}$,
A.M.~Whitehead$^\textrm{\scriptsize 92}$,
J.~Wiechula$^\textrm{\scriptsize 60}$,
J.~Wikne$^\textrm{\scriptsize 20}$,
G.~Wilk$^\textrm{\scriptsize 79}$,
J.~Wilkinson$^\textrm{\scriptsize 96}$,
G.A.~Willems$^\textrm{\scriptsize 61}$,
M.C.S.~Williams$^\textrm{\scriptsize 107}$,
B.~Windelband$^\textrm{\scriptsize 96}$,
W.E.~Witt$^\textrm{\scriptsize 129}$,
S.~Yalcin$^\textrm{\scriptsize 70}$,
P.~Yang$^\textrm{\scriptsize 7}$,
S.~Yano$^\textrm{\scriptsize 46}$,
Z.~Yin$^\textrm{\scriptsize 7}$,
H.~Yokoyama$^\textrm{\scriptsize 132}$\textsuperscript{,}$^\textrm{\scriptsize 72}$,
I.-K.~Yoo$^\textrm{\scriptsize 34}$\textsuperscript{,}$^\textrm{\scriptsize 99}$,
J.H.~Yoon$^\textrm{\scriptsize 50}$,
V.~Yurchenko$^\textrm{\scriptsize 3}$,
V.~Zaccolo$^\textrm{\scriptsize 84}$\textsuperscript{,}$^\textrm{\scriptsize 113}$,
A.~Zaman$^\textrm{\scriptsize 15}$,
C.~Zampolli$^\textrm{\scriptsize 34}$,
H.J.C.~Zanoli$^\textrm{\scriptsize 123}$,
S.~Zaporozhets$^\textrm{\scriptsize 67}$,
N.~Zardoshti$^\textrm{\scriptsize 104}$,
A.~Zarochentsev$^\textrm{\scriptsize 138}$,
P.~Z\'{a}vada$^\textrm{\scriptsize 56}$,
N.~Zaviyalov$^\textrm{\scriptsize 102}$,
H.~Zbroszczyk$^\textrm{\scriptsize 140}$,
M.~Zhalov$^\textrm{\scriptsize 89}$,
H.~Zhang$^\textrm{\scriptsize 21}$\textsuperscript{,}$^\textrm{\scriptsize 7}$,
X.~Zhang$^\textrm{\scriptsize 7}$\textsuperscript{,}$^\textrm{\scriptsize 75}$,
Y.~Zhang$^\textrm{\scriptsize 7}$,
C.~Zhang$^\textrm{\scriptsize 53}$,
Z.~Zhang$^\textrm{\scriptsize 7}$,
C.~Zhao$^\textrm{\scriptsize 20}$,
N.~Zhigareva$^\textrm{\scriptsize 54}$,
D.~Zhou$^\textrm{\scriptsize 7}$,
Y.~Zhou$^\textrm{\scriptsize 84}$,
Z.~Zhou$^\textrm{\scriptsize 21}$,
H.~Zhu$^\textrm{\scriptsize 21}$\textsuperscript{,}$^\textrm{\scriptsize 7}$,
J.~Zhu$^\textrm{\scriptsize 7}$\textsuperscript{,}$^\textrm{\scriptsize 116}$,
X.~Zhu$^\textrm{\scriptsize 7}$,
A.~Zichichi$^\textrm{\scriptsize 12}$\textsuperscript{,}$^\textrm{\scriptsize 26}$,
A.~Zimmermann$^\textrm{\scriptsize 96}$,
M.B.~Zimmermann$^\textrm{\scriptsize 34}$\textsuperscript{,}$^\textrm{\scriptsize 61}$,
S.~Zimmermann$^\textrm{\scriptsize 115}$,
G.~Zinovjev$^\textrm{\scriptsize 3}$,
J.~Zmeskal$^\textrm{\scriptsize 115}$
\renewcommand\labelenumi{\textsuperscript{\theenumi}~}

\section*{Affiliation notes}
\renewcommand\theenumi{\roman{enumi}}
\begin{Authlist}
\item \Adef{0}Deceased
\item \Adef{idp1764384}{Also at: Georgia State University, Atlanta, Georgia, United States}
\item \Adef{idp3207120}{Also at: Also at Department of Applied Physics, Aligarh Muslim University, Aligarh, India}
\item \Adef{idp3984928}{Also at: M.V. Lomonosov Moscow State University, D.V. Skobeltsyn Institute of Nuclear, Physics, Moscow, Russia}
\end{Authlist}

\section*{Collaboration Institutes}
\renewcommand\theenumi{\arabic{enumi}~}

$^{1}$A.I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia
\\
$^{2}$Benem\'{e}rita Universidad Aut\'{o}noma de Puebla, Puebla, Mexico
\\
$^{3}$Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
\\
$^{4}$Bose Institute, Department of Physics 
and Centre for Astroparticle Physics and Space Science (CAPSS), Kolkata, India
\\
$^{5}$Budker Institute for Nuclear Physics, Novosibirsk, Russia
\\
$^{6}$California Polytechnic State University, San Luis Obispo, California, United States
\\
$^{7}$Central China Normal University, Wuhan, China
\\
$^{8}$Centre de Calcul de l'IN2P3, Villeurbanne, Lyon, France
\\
$^{9}$Centro de Aplicaciones Tecnol\'{o}gicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
\\
$^{10}$Centro de Investigaciones Energ\'{e}ticas Medioambientales y Tecnol\'{o}gicas (CIEMAT), Madrid, Spain
\\
$^{11}$Centro de Investigaci\'{o}n y de Estudios Avanzados (CINVESTAV), Mexico City and M\'{e}rida, Mexico
\\
$^{12}$Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche ``Enrico Fermi', Rome, Italy
\\
$^{13}$Chicago State University, Chicago, Illinois, United States
\\
$^{14}$China Institute of Atomic Energy, Beijing, China
\\
$^{15}$COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
\\
$^{16}$Departamento de F\'{\i}sica de Part\'{\i}culas and IGFAE, Universidad de Santiago de Compostela, Santiago de Compostela, Spain
\\
$^{17}$Department of Physics, Aligarh Muslim University, Aligarh, India
\\
$^{18}$Department of Physics, Ohio State University, Columbus, Ohio, United States
\\
$^{19}$Department of Physics, Sejong University, Seoul, South Korea
\\
$^{20}$Department of Physics, University of Oslo, Oslo, Norway
\\
$^{21}$Department of Physics and Technology, University of Bergen, Bergen, Norway
\\
$^{22}$Dipartimento di Fisica dell'Universit\`{a} 'La Sapienza'
and Sezione INFN, Rome, Italy
\\
$^{23}$Dipartimento di Fisica dell'Universit\`{a}
and Sezione INFN, Cagliari, Italy
\\
$^{24}$Dipartimento di Fisica dell'Universit\`{a}
and Sezione INFN, Trieste, Italy
\\
$^{25}$Dipartimento di Fisica dell'Universit\`{a}
and Sezione INFN, Turin, Italy
\\
$^{26}$Dipartimento di Fisica e Astronomia dell'Universit\`{a}
and Sezione INFN, Bologna, Italy
\\
$^{27}$Dipartimento di Fisica e Astronomia dell'Universit\`{a}
and Sezione INFN, Catania, Italy
\\
$^{28}$Dipartimento di Fisica e Astronomia dell'Universit\`{a}
and Sezione INFN, Padova, Italy
\\
$^{29}$Dipartimento di Fisica `E.R.~Caianiello' dell'Universit\`{a}
and Gruppo Collegato INFN, Salerno, Italy
\\
$^{30}$Dipartimento DISAT del Politecnico and Sezione INFN, Turin, Italy
\\
$^{31}$Dipartimento di Scienze e Innovazione Tecnologica dell'Universit\`{a} del Piemonte Orientale and INFN Sezione di Torino, Alessandria, Italy
\\
$^{32}$Dipartimento Interateneo di Fisica `M.~Merlin'
and Sezione INFN, Bari, Italy
\\
$^{33}$Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
\\
$^{34}$European Organization for Nuclear Research (CERN), Geneva, Switzerland
\\
$^{35}$Excellence Cluster Universe, Technische Universit\"{a}t M\"{u}nchen, Munich, Germany
\\
$^{36}$Faculty of Engineering, Bergen University College, Bergen, Norway
\\
$^{37}$Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
\\
$^{38}$Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
\\
$^{39}$Faculty of Science, P.J.~\v{S}af\'{a}rik University, Ko\v{s}ice, Slovakia
\\
$^{40}$Faculty of Technology, Buskerud and Vestfold University College, Tonsberg, Norway
\\
$^{41}$Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universit\"{a}t Frankfurt, Frankfurt, Germany
\\
$^{42}$Gangneung-Wonju National University, Gangneung, South Korea
\\
$^{43}$Gauhati University, Department of Physics, Guwahati, India
\\
$^{44}$Helmholtz-Institut f\"{u}r Strahlen- und Kernphysik, Rheinische Friedrich-Wilhelms-Universit\"{a}t Bonn, Bonn, Germany
\\
$^{45}$Helsinki Institute of Physics (HIP), Helsinki, Finland
\\
$^{46}$Hiroshima University, Hiroshima, Japan
\\
$^{47}$Indian Institute of Technology Bombay (IIT), Mumbai, India
\\
$^{48}$Indian Institute of Technology Indore, Indore, India
\\
$^{49}$Indonesian Institute of Sciences, Jakarta, Indonesia
\\
$^{50}$Inha University, Incheon, South Korea
\\
$^{51}$Institut de Physique Nucl\'eaire d'Orsay (IPNO), Universit\'e Paris-Sud, CNRS-IN2P3, Orsay, France
\\
$^{52}$Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
\\
$^{53}$Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
\\
$^{54}$Institute for Theoretical and Experimental Physics, Moscow, Russia
\\
$^{55}$Institute of Experimental Physics, Slovak Academy of Sciences, Ko\v{s}ice, Slovakia
\\
$^{56}$Institute of Physics, Academy of Sciences of the Czech Republic, Prague, Czech Republic
\\
$^{57}$Institute of Physics, Bhubaneswar, India
\\
$^{58}$Institute of Space Science (ISS), Bucharest, Romania
\\
$^{59}$Institut f\"{u}r Informatik, Johann Wolfgang Goethe-Universit\"{a}t Frankfurt, Frankfurt, Germany
\\
$^{60}$Institut f\"{u}r Kernphysik, Johann Wolfgang Goethe-Universit\"{a}t Frankfurt, Frankfurt, Germany
\\
$^{61}$Institut f\"{u}r Kernphysik, Westf\"{a}lische Wilhelms-Universit\"{a}t M\"{u}nster, M\"{u}nster, Germany
\\
$^{62}$Instituto de Ciencias Nucleares, Universidad Nacional Aut\'{o}noma de M\'{e}xico, Mexico City, Mexico
\\
$^{63}$Instituto de F\'{i}sica, Universidade Federal do Rio Grande do Sul (UFRGS), Porto Alegre, Brazil
\\
$^{64}$Instituto de F\'{\i}sica, Universidad Nacional Aut\'{o}noma de M\'{e}xico, Mexico City, Mexico
\\
$^{65}$IRFU, CEA, Universit\'{e} Paris-Saclay, F-91191 Gif-sur-Yvette, France, Saclay, France
\\
$^{66}$iThemba LABS, National Research Foundation, Somerset West, South Africa
\\
$^{67}$Joint Institute for Nuclear Research (JINR), Dubna, Russia
\\
$^{68}$Konkuk University, Seoul, South Korea
\\
$^{69}$Korea Institute of Science and Technology Information, Daejeon, South Korea
\\
$^{70}$KTO Karatay University, Konya, Turkey
\\
$^{71}$Laboratoire de Physique Corpusculaire (LPC), Clermont Universit\'{e}, Universit\'{e} Blaise Pascal, CNRS--IN2P3, Clermont-Ferrand, France
\\
$^{72}$Laboratoire de Physique Subatomique et de Cosmologie, Universit\'{e} Grenoble-Alpes, CNRS-IN2P3, Grenoble, France
\\
$^{73}$Laboratori Nazionali di Frascati, INFN, Frascati, Italy
\\
$^{74}$Laboratori Nazionali di Legnaro, INFN, Legnaro, Italy
\\
$^{75}$Lawrence Berkeley National Laboratory, Berkeley, California, United States
\\
$^{76}$Moscow Engineering Physics Institute, Moscow, Russia
\\
$^{77}$Nagasaki Institute of Applied Science, Nagasaki, Japan
\\
$^{78}$National and Kapodistrian University of Athens, Physics Department, Athens, Greece, Athens, Greece
\\
$^{79}$National Centre for Nuclear Studies, Warsaw, Poland
\\
$^{80}$National Institute for Physics and Nuclear Engineering, Bucharest, Romania
\\
$^{81}$National Institute of Science Education and Research, Bhubaneswar, India
\\
$^{82}$National Nuclear Research Center, Baku, Azerbaijan
\\
$^{83}$National Research Centre Kurchatov Institute, Moscow, Russia
\\
$^{84}$Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
\\
$^{85}$Nikhef, Nationaal instituut voor subatomaire fysica, Amsterdam, Netherlands
\\
$^{86}$Nuclear Physics Group, STFC Daresbury Laboratory, Daresbury, United Kingdom
\\
$^{87}$Nuclear Physics Institute, Academy of Sciences of the Czech Republic, \v{R}e\v{z} u Prahy, Czech Republic
\\
$^{88}$Oak Ridge National Laboratory, Oak Ridge, Tennessee, United States
\\
$^{89}$Petersburg Nuclear Physics Institute, Gatchina, Russia
\\
$^{90}$Physics Department, Creighton University, Omaha, Nebraska, United States
\\
$^{91}$Physics Department, Panjab University, Chandigarh, India
\\
$^{92}$Physics Department, University of Cape Town, Cape Town, South Africa
\\
$^{93}$Physics Department, University of Jammu, Jammu, India
\\
$^{94}$Physics Department, University of Rajasthan, Jaipur, India
\\
$^{95}$Physikalisches Institut, Eberhard Karls Universit\"{a}t T\"{u}bingen, T\"{u}bingen, Germany
\\
$^{96}$Physikalisches Institut, Ruprecht-Karls-Universit\"{a}t Heidelberg, Heidelberg, Germany
\\
$^{97}$Physik Department, Technische Universit\"{a}t M\"{u}nchen, Munich, Germany
\\
$^{98}$Purdue University, West Lafayette, Indiana, United States
\\
$^{99}$Pusan National University, Pusan, South Korea
\\
$^{100}$Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum f\"ur Schwerionenforschung GmbH, Darmstadt, Germany
\\
$^{101}$Rudjer Bo\v{s}kovi\'{c} Institute, Zagreb, Croatia
\\
$^{102}$Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
\\
$^{103}$Saha Institute of Nuclear Physics, Kolkata, India
\\
$^{104}$School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
\\
$^{105}$Secci\'{o}n F\'{\i}sica, Departamento de Ciencias, Pontificia Universidad Cat\'{o}lica del Per\'{u}, Lima, Peru
\\
$^{106}$Sezione INFN, Bari, Italy
\\
$^{107}$Sezione INFN, Bologna, Italy
\\
$^{108}$Sezione INFN, Cagliari, Italy
\\
$^{109}$Sezione INFN, Catania, Italy
\\
$^{110}$Sezione INFN, Padova, Italy
\\
$^{111}$Sezione INFN, Rome, Italy
\\
$^{112}$Sezione INFN, Trieste, Italy
\\
$^{113}$Sezione INFN, Turin, Italy
\\
$^{114}$SSC IHEP of NRC Kurchatov institute, Protvino, Russia
\\
$^{115}$Stefan Meyer Institut f\"{u}r Subatomare Physik (SMI), Vienna, Austria
\\
$^{116}$SUBATECH, Ecole des Mines de Nantes, Universit\'{e} de Nantes, CNRS-IN2P3, Nantes, France
\\
$^{117}$Suranaree University of Technology, Nakhon Ratchasima, Thailand
\\
$^{118}$Technical University of Ko\v{s}ice, Ko\v{s}ice, Slovakia
\\
$^{119}$Technical University of Split FESB, Split, Croatia
\\
$^{120}$The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
\\
$^{121}$The University of Texas at Austin, Physics Department, Austin, Texas, United States
\\
$^{122}$Universidad Aut\'{o}noma de Sinaloa, Culiac\'{a}n, Mexico
\\
$^{123}$Universidade de S\~{a}o Paulo (USP), S\~{a}o Paulo, Brazil
\\
$^{124}$Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
\\
$^{125}$Universidade Federal do ABC, Santo Andre, Brazil
\\
$^{126}$University of Houston, Houston, Texas, United States
\\
$^{127}$University of Jyv\"{a}skyl\"{a}, Jyv\"{a}skyl\"{a}, Finland
\\
$^{128}$University of Liverpool, Liverpool, United Kingdom
\\
$^{129}$University of Tennessee, Knoxville, Tennessee, United States
\\
$^{130}$University of the Witwatersrand, Johannesburg, South Africa
\\
$^{131}$University of Tokyo, Tokyo, Japan
\\
$^{132}$University of Tsukuba, Tsukuba, Japan
\\
$^{133}$University of Zagreb, Zagreb, Croatia
\\
$^{134}$Universit\'{e} de Lyon, Universit\'{e} Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, Lyon, France
\\
$^{135}$Universit\'{e} de Strasbourg, CNRS, IPHC UMR 7178, F-67000 Strasbourg, France, Strasbourg, France
\\
$^{136}$Universit\`{a} degli Studi di Pavia, Pavia, Italy
\\
$^{137}$Universit\`{a} di Brescia, Brescia, Italy
\\
$^{138}$V.~Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
\\
$^{139}$Variable Energy Cyclotron Centre, Kolkata, India
\\
$^{140}$Warsaw University of Technology, Warsaw, Poland
\\
$^{141}$Wayne State University, Detroit, Michigan, United States
\\
$^{142}$Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
\\
$^{143}$Yale University, New Haven, Connecticut, United States
\\
$^{144}$Yonsei University, Seoul, South Korea
\\
$^{145}$Zentrum f\"{u}r Technologietransfer und Telekommunikation (ZTT), Fachhochschule Worms, Worms, Germany
\endgroup


\section{Experiment and data analysis}

The data were recorded in 2011 during the second~{Pb--Pb}\ running period
of the LHC. Approximately 2 million minimum bias
events, 29.2 million central trigger events, and 34.1 million
semi-central trigger events were used in this analysis.  A detailed description of the ALICE
detector can be found in~\cite{ALICE_exp_1,Abelev:2014ffa}.
The Time Projection Chamber (TPC) has full azimuthal coverage and allows
charged-particle track reconstruction in the pseudorapidity
range $|\eta|<~0.8$, as well as particle identification
via the specific ionization energy loss $\mathrm{d}E/\mathrm{d}x$ associated with each track.  In addition to the TPC, the
Time-Of-Flight (TOF) detector was used for identification of particles
with transverse momentum~$p_{\rm{T}}$~~$>$~0.5~{\rm GeV/{\it c}}.

The minimum bias, semi-central, and central triggers used in this analysis all require a signal in both V0
detectors~\cite{Abbas:2013taa}.  The V0 is a small angle detector
of scintillator arrays covering pseudorapidity ranges $2.8<\eta<5.1$
and $-3.7<\eta<-1.7$ for a collision vertex occurring at the center of
the ALICE detector.  The V0 detector was also used for the
centrality determination~\cite{Aamodt:2010cz}. The results of this analysis
are reported for collision centrality classes expressed as ranges of
the fraction of the inelastic {Pb--Pb}~cross-section: 0--5\%, 5--10\%,
10--20\%, 20--30\%, 30--40\%, and 40--50\%. The position of the
primary event vertex along the beam direction $V_{z}$ was determined
for each event.  Events with $|V_{z}|<8$~cm were used in this analysis
to ensure a uniform pseudorapidity acceptance.

The TPC has 18 sectors covering full azimuth with 159 pad rows
radially placed in each sector. Tracks with at least 80 space points
in the TPC have been used in this analysis.  Tracks compatible with a decay in flight (kink topology) were rejected.
The track quality was determined
by the $\chi^{2}$ of the Kalman filter fit to the reconstructed TPC
clusters.  The $\chi^2$ per degrees of freedom was
required to be less than 4.  For primary track selection, only
trajectories passing within 3.2~cm from the primary vertex in the
longitudinal direction and 2.4~cm in the transverse direction were
used.  Based on the specific ionization energy loss in the TPC gas
compared with the corresponding Bethe-Bloch curve, and the time of
flight in TOF, a probability for each track to be a pion, kaon,
proton, or electron was determined. Particles for which the pion
probability was the largest were used in this analysis.  Pions were
selected in the pseudorapidity range $|\eta|<0.8$ and 0.15 $<$ $p_{\rm{T}}$~$<$
1.5~{\rm GeV/{\it c}}.




The correlation function $C({\bq})$ was calculated as
\begin{eqnarray}
  C({\bq})=\frac{ A({\bq})} { B({\bq})},
\end{eqnarray}
where $\bq=\bp_1-\bp_2$ is the relative momentum of two pions,
$A(\bq)$ is the same-event distribution of particle pairs, and
$B(\bq)$ is the background distribution of uncorrelated particle
pairs. Both the $A({\bq})$ and $B({\bq})$ distributions were measured
differentially with respect to the second harmonic event-plane angle
$\Psi_{\mathrm{EP},2}$. The second harmonic event-plane angle $\Psi_{\mathrm{EP},2}$ was determined using TPC tracks. To avoid
self-correlation, each event was split into two subevents
($-0.8<\eta<0$ and $0<\eta<0.8$). Pairs were chosen from one subevent
and the second harmonic event-plane angle $\Psi_{\mathrm{EP},2}$ was determined using
the other subevent particles, and vice-versa, with the event plane
resolution determined from the correlations between the event planes
determined in different subevents~\cite{Poskanzer:1998yz}.
The background distribution is built by using the mixed-event
technique~\cite{Kopylov:1974th} in which pairs are made out of
particles from two different events with similar centrality (less than
2\% difference), event-plane angle (less than 10$^\circ$ difference),
and event vertex position along the beam direction (less than 4~cm
difference).  Requiring a minimum value in the
two-track separation parameters $\Delta \varphi^*$ and $\Delta\eta$
controls two-track reconstruction effects such as track splitting or
track merging.  The quantity $\varphi^{*}$ is defined in this analysis
as the azimuthal angle of the track in the laboratory frame at the
radial position of 1.6~m inside the TPC. Splitting is the effect when
one track is reconstructed as two tracks, and merging is the effect of
two tracks being reconstructed as one. Also, to reduce the splitting
effect, pairs that share more than 5\% of the TPC clusters were
removed from the analysis. It is observed that at large relative
momentum the correlation function is a constant, and the background
pair distribution is normalized such that this constant is unity.  The
analysis was performed for different collision centralities in several
ranges of $k_\rT$, the magnitude of the pion-pair transverse momentum
$\bk_\rT=(\bp_{\rT,1}+\bp_{\rT,2})/2$, and in bins of $\Delta\varphi=
\mathrm{\varphi_{pair}}-\Psi_{\mathrm{EP},2}$, defined in the range (0,~$\pi$) where
$\mathrm{\varphi_{pair}}$ is the pair azimuthal angle.  The
Bertsch-Pratt~\cite{Pratt:1986cc,Bertsch:1988db} out--side--long
coordinate system was used with the {\it long} direction pointing
along the beam axis, {\it out} along the transverse pair momentum, and
{\it side} being perpendicular to the other two.  The
three-dimensional correlation function was analyzed in the
Longitudinally Co-Moving System (LCMS), in which the total
longitudinal momentum of the pair is zero,
${p_{1,\mathrm{L}}}=-{p_{2,\mathrm{L}}}$.

To isolate the Bose-Einstein contribution in the correlation function, effects due to final-state Coulomb
repulsion must be taken into account.  For that, the Bowler-Sinyukov fitting
procedure~\cite{Bowler:1991pi,Sinyukov:1998fc} was used in which the
Coulomb weight is only applied to the fraction of pairs ($\lambda$)
that participate in the Bose-Einstein correlation. In this approach,
the correlation function is fitted to
\begin{eqnarray}
 C({\bq},\Delta\varphi)=N[(1-\lambda)+\lambda K({\bq})(1+G({\bq},\Delta\varphi))],
\end{eqnarray}
where $N$ is the normalization factor. The function $G({\bq},\Delta\varphi)$
describes the Bose-Einstein correlations and $K({\bq})$ is the Coulomb
part of the two-pion wave function integrated over a source function
corresponding to $G({\bq})$.  In this analysis the Gaussian form of
$G({\bq},\Delta\varphi)$ was used~\cite{guassain}:
\begin{eqnarray}
 G(\bq,\Delta\varphi)=\exp
\left[
-q_{\rm out}^{2} R_{\rm out}^{2}(\Delta\varphi)-q_{\rm side}^{2} R_{\rm side}^{2}(\Delta\varphi) \right.
\nonumber
\\
\left.
-q_{\rm long}^{2} R_{\rm long}^{2}(\Delta\varphi)-2q_{\rm out} q_{\rm side} R_{\rm os}^{2}(\Delta\varphi) \right.
\nonumber
\\
\left.
-2q_{\rm side} q_{\rm long} R_{\rm sl}^{2}(\Delta\varphi)-2q_{\rm out} q_{\rm long} R_{\rm ol}^{2}(\Delta\varphi)
\right],
\end{eqnarray}
where the parameters $R_{\rm out}$, $R_{\rm side}$, and $R_{\rm long}$ are traditionally
called HBT radii in the {\it out}, {\it side}, and {\it long}
directions.  The cross-terms $R_{\rm os}^{2}$, $R_{\rm sl}^{2}$, and $R_{\rm ol}^{2}$
describe the correlation in the {\it out}-{\it side}, {\it side}-{\it
  long}, and {\it out}-{\it long}~directions, respectively.

The systematic errors on the extracted radii vary within 3--9\%
depending on $k_{\rm{T}}$ and centrality.  They include uncertainties related
to the tracking efficiency and track quality, momentum resolution
~\cite{Adam:2015vna}, different pair cuts ($\Delta \varphi^*$ and
$\Delta\eta$), and correlation function fit ranges.  Positive and
negative pion pairs as well as
data obtained with two opposite magnetic field polarities of the ALICE
L3 magnet
have been analyzed separately and a small
difference in the results (less than 3\%) has been also accounted for
in the systematic error. The total systematic errors were obtained
from adding the above systematic errors in quadrature.

Other than being differential in the event plane, this analysis is
similar in most aspects to the analysis reported
in~\cite{Adam:2015vna}, and further details can be found there.
The results reported below were obtained with the second harmonic
event plane~\cite{Poskanzer:1998yz} determined with the TPC tracks.
It was checked that they are consistent with the results obtained with
the event-plane angle determined with the V0 detector.


Figure~\ref{fig:ktdependence} presents the dependence of $R_{\rm out}^{2}$,
$R_{\rm side}^{2}$, $R_{\rm long}^{2}$, $R_{\rm os}^{2}$, and $\lambda$ on the pion
emission angle relative to the second harmonic event plane. The
results are shown for the centrality classes 20--30\% in four ranges of
$k_{\rm{T}}$: 0.2--0.3, 0.3--0.4, 0.4--0.5, and 0.5--0.7~{\rm GeV/{\it c}}.  $R_{\rm out}^2$
and $R_{\rm side}^2$ exhibit clear out-of-phase oscillations. No
oscillations for $R_{\rm long}^2$ and $\lambda$ are observed within the
uncertainties of the measurement. The parameter $R_{\rm os}^2$ shows very
similar oscillations for all $k_{\rm{T}}$ bins.  $R_{\rm ol}^2$ and $R_{\rm sl}^2$ (not
shown) are found to be consistent with zero, as expected due to
symmetry, and are not further investigated in this analysis. A
possible correlation between $\lambda$ and the extracted radii was
checked by fixing $\lambda$. No change in the radii has been
observed. The curves represent the fits to the data using the
functions~\cite{Voloshin:1995mc,Voloshin:1996ch}:
 \begin{eqnarray} \label{eq:radii_osc}
 R^{2}_{\mu}(\Delta\varphi)=R^{2}_{\mu,0}+2R^{2}_{\mu,2}\cos(2\Delta\varphi)~(\mu={\rm out,side,long,sl,ol}),
\nonumber
\\
\nonumber
R_{\rm os}^{2}(\Delta\varphi)=R^{2}_{{\rm os},0}+2 R^{2}_{{\rm os},2}\sin(2\Delta\varphi).
\end{eqnarray}
Fitting the radii's azimuthal dependence with the functional form of
Eq.~\ref{eq:radii_osc} allows us to extract the average radii and the
amplitudes of oscillations. The latter have to be corrected for the
finite event plane resolution. There exist several methods for such a
correction~\cite{Lisa:2005dd}, which produce very similar
results~\cite{Adamczyk:2014mxp} well within errors of this
analysis. The results shown below have been obtained with the simplest
method first used by the E895 Collaboration~\cite{Lisa:2000xj}, in
which the amplitude of oscillation is divided by the event plane
resolution factor.  The correction is about 5--15\%, depending
on centrality.
\begin{figure}[!ht]
 \centering
\hspace*{-5mm}
\includegraphics[width=11cm]{RModulation}
\hspace*{-5mm}
\caption{The azimuthal dependence of $R_{\rm out}^{2} $, $R_{\rm side}^{2}$,
  $R_{\rm long}^{2}$, $R_{\rm os}^{2}$, and
  $\lambda$ as a function of
  $\Delta\varphi=\mathrm{\varphi_{pair}}-\Psi_{\mathrm{EP},2}$ for the centrality 20--30\% and $k_\rT$
  ranges 0.2--0.3, 0.3--0.4, 0.4--0.5, and 0.5--0.7 GeV/$c$. Bands
  indicate the systematic errors. The results are not corrected for the
  event plane resolution of about 85--95\%.}
\label{fig:ktdependence}
\end{figure}
\begin{figure}[!ht]
\centering
\hspace*{-2mm}
\includegraphics[width=13cm]
{Raverage}
  \caption{ The average radii $R_{{\rm out},0}^{2} $, $R_{{\rm side},0}^{2}$,
    $R_{{\rm long},0}^{2}$, and $R_{{\rm os},0}^{2}$ as a function of centrality for
    different $k_{\rm{T}}$ ranges compared to hydrodynamical
    calculations~\cite{Bozek:2014hwa}. Square brackets indicate the
    systematic errors.  }
\label{fig:avg_radii}
\end{figure}
Figure~\ref{fig:avg_radii} shows the average radii for different $k_{\rm{T}}$
values as a function of centrality.  The average radii obtained in
this analysis are consistent with the results reported
in~\cite{Adam:2015vna}.  As expected, the radii are larger in more
central collisions and at smaller $k_{\rm{T}}$ values, the latter reflecting
the effect of radial flow~\cite{Lisa:2005dd,Retiere:2003kf}.  The
cross-term $R_{{\rm os},0}^2$ is consistent with zero, as expected due to the
symmetry of the system. Figure~\ref{fig:avg_radii} also shows the
average radii calculated for charged pions in the pseudorapidity range
$|\eta|<2$ from 3+1D hydrodynamic
calculations~\cite{Bozek:2014hwa}, assuming freeze-out temperature
$T_{f}$~=~150 MeV and a constant shear viscosity to entropy density
ratio $\eta/s$~= 0.08. The 3+1D hydrodynamic calculations,
while correctly describing the qualitative features of the average
radii dependence on centrality and $k_{\rm{T}}$, fail to describe our results
quantitatively.
\begin{figure}[!ht]
\hspace*{14mm}
\includegraphics[width=13cm,keepaspectratio]{Rratio}
  \caption{ Amplitudes of the relative radius oscillations~$R^{2}_{\rm
      out,2}/R^{2}_{\rm side,0}$,~$R^{2}_{\rm side,2}/R^{2}_{\rm
      side,0}$,~$R^{2}_{\rm long,2}/R^{2}_{\rm long,0}$,
    and~$R^{2}_{\rm os,2}/R^{2}_{\rm side,0}$ versus centrality for
    the $k_{\rm{T}}$ ranges 0.2--0.3, 0.3--0.4, 0.4--0.5, and 0.5--0.7~{\rm GeV/{\it c}}. The error
    bars indicate the statistical uncertainties and the square
    brackets show the systematic errors. The STAR data points, for 0--5\%, 5--10\%, 10--20\%, 20--30\% and 30--80\% Au--Au collisions, are slightly shifted for clarity.
  }
\label{fig:relative_Radii}
\end{figure}


Figure~\ref{fig:relative_Radii} shows the relative amplitudes of the
radius oscillations $R^{2}_{{\rm out},2}/R^{2}_{{\rm
    side},0}$,~$R^{2}_{{\rm side},2}/R^{2}_{{\rm side},0}$,
$R^{2}_{{\rm long},2}/R^{2}_{{\rm long},0}$, and $R^{2}_{{\rm
    os},2}/R^{2}_{{\rm side},0}$. When comparing our results to the
ones obtained by the STAR experiment, we observe similar relative
oscillations, however STAR results~\cite{Adams:2003ra,Adams:2004yc}
show on average larger oscillations for $R_{\rm side}^{2}$. Our relative
amplitudes for $R^{2}_{\rm out,2}/R^{2}_{\rm side,0}$, $R^{2}_{\rm
  side,2}/R^{2}_{\rm side,0}$, and $R^{2}_{{\rm os},2}/R^{2}_{{\rm
    side},0}$ show a clear centrality dependence, whereas the $R^{2}_{\rm long,2}/R^{2}_{\rm long,0}$
is very close to zero for all centralities, similarly to the results
from RHIC~\cite{Adams:2003ra,Adamczyk:2014mxp,Adare:2015bcj}.

The source eccentricity is usually defined as
$\eps=(R^2_y-R^2_x)/(R^2_y+R^2_x)$, where $R_{x}$ is the in-plane
radius of the (assumed) elliptical source and $R_y$ is the
out-of-plane radius.  As shown in~\cite{Retiere:2003kf} the relative
amplitudes of side radii oscillations are mostly determined by the
spatial source anisotropy and are less affected by dynamical effects
such as velocity gradients.  The source eccentricity at freeze-out
$\eps_{\rm final}$ can be estimated from $R^{2}_{\rm side}$
oscillations at small pion momenta with an accuracy within 20--30\% as
$\eps_{\rm final}\approx
2R_{{\rm side},2}^2/R_{{\rm side},0}^2$~\cite{Retiere:2003kf}.

Figure~\ref{fig:finaleccentricity} presents $2R_{{\rm side},2}^2/R_{{\rm side},0}^2$
for different $k_{\rm{T}}$ ranges as a function of the initial-state
eccentricity for six different centralities and four $k_{\rm{T}}$ bins.  For
the initial eccentricity we have used the nucleon participant
eccentricity from the Monte Carlo Glauber model for both,
Au--Au~collisions at \mbox{$\sqrt{s_{_{\rm NN}}}$}~=200~GeV~\cite{Adare:2014vax} and
{Pb--Pb}~collision at \mbox{$\sqrt{s_{_{\rm NN}}}$}~= 2.76~TeV~\cite{Ghosh:2016npo}. Our results for
all $k_{\rm{T}}$ bins are significantly below the values of the initial
eccentricity indicating a more intense expansion in the in-plane
direction. Due to relatively large uncertainties of the RHIC results
for narrow $k_{\rm{T}}$ bins, we compare our results only to the average STAR
data~\cite{Adams:2003ra} in $0.15<k_{\rm{T}} <0.6$~{\rm GeV/{\it c}}~ and to PHENIX
results~\cite{Adare:2014vax} corresponding to $0.2<k_{\rm{T}} <2.0$~{\rm GeV/{\it c}}~
($\mean{k_{\rm{T}}}=0.53$~{\rm GeV/{\it c}}). We find a smaller final-state anisotropy in
the LHC regime compared to RHIC energies. This trend is qualitatively
consistent with expectations from hydrodynamic and transport
models~\cite{Shen:2012us,Lisa:2011na}. The final-state eccentricity
remains positive also at the LHC, evidence of an out-of-plane
elongated source at freeze-out. In Fig.~\ref{fig:finaleccentricity},
we also compare our results to the 3+1D hydrodynamic
calculations~\cite{Bozek:2014hwa}, which were performed for similar
centralities and $k_{\rm{T}}$ ranges as in the experiment. This model
slightly underestimates the final source eccentricity.

\begin{figure}[!ht]
\centering
\includegraphics[width=11cm,keepaspectratio]
{Eccen_Bozek_STAR_PHENIX}
  \caption{An estimate of freeze-out eccentricity $2
    R^{2}_{\rm side,2}/R^{2}_{\rm side,0}$ for different $k_{\rm{T}}$ ranges vs.
    initial state eccentricity from Monte Carlo Glauber
    model~\cite{Ghosh:2016npo} for six centrality ranges, 0--5\%,
    5--10\%, 10--20\%, 20--30 \%, 30--40 \%, and 40--50\%.  The dashed line
    indicates $\eps_{\rm final}=\eps_{\rm init}$. Square brackets
    indicate systematic errors. }
\label{fig:finaleccentricity}
\end{figure}



In conclusion, we have performed a measurement of two-pion azimuthally
differential femtoscopy relative to the second harmonic flow plane in
{Pb--Pb}~collisions at \mbox{$\sqrt{s_{_{\rm NN}}}$}~= 2.76~TeV.  The out, side, and out-side radii
exhibit clear oscillations while the long radius is consistent with a
constant.  The relative amplitudes of oscillations only weakly depend
on $k_{\rm{T}}$, with the side-radii oscillation slightly increasing with
$k_{\rm{T}}$.  The final-state source eccentricity, estimated via side-radius
oscillations, is noticeably smaller than at lower collisions energies,
but still exhibits an out-of-plane elongated source at freeze-out even
after a stronger in-plane expansion. The final eccentricity is
slightly larger than that predicted by existing hydrodynamic
calculations.


\newenvironment{acknowledgement}{\relax}{\relax}
\begin{acknowledgement}
\section*{Acknowledgements}
\input{fa_2016-12-30.tex}
\end{acknowledgement}


