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[email protected] http://fcxn.wordpress.com Social Dynamic Behavior Patterns @CeydaSanli CompleXity Networks August 31, 2015, Meeting.

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  • 5 mm

    Inset: The displacement field demonstrates local heterogeneities in the flow.

    A typical snapshot of an experiment: The white spots indicate the positions of the beads floating on surface waves.

    [email protected]

    http://fcxn.wordpress.com ! Month 6 General Meeting

    http://xn.unamur.be

    Fluctuations drive viral memes in online social media: Integrating criticality into network science

    Ceyda Sanl, Vsevolod Salnikov, Lionel Tabourier, and Renaud Lambiotte

    CompleXity Networks, naXys, University of Namur, Belgium.

    To spread our posts throughout online social network such as Twitter: When do we need to post? How often should a #hashtag be posted? These questions emphasize the time features of our twitting activity. They would be controlled much more easily compared to the followings: What we post and how many number of followers we have.

    To be mobile in dense granular media such as highly packed beads on surface waves: Do single beads move independently or form a group? Is the trajectory of each bead regular in time? The quantification of the bead dynamics shows that the beads perform heterogenous motion with a distinct time scale to characterize this heterogeneity.

    restricted amount of attention restricted amount of space

    Restricted amount of sources forces social and physical systems to present emergence of order.

    hypothesis

    Twitter users want to spread their messages and beads under driving want to be mobile. As a result, the twitter users collectively advertise and the beads form groups to move together. Both systems self-organize and create dynamic heterogeneity.

    The origin of the fluctuations in dynamics would be the same origins:

    Therefore, the interpretation of the dynamic heterogeneity of the beads in a critical limit would help to characterize viral memes (#hashtags) in twitter.

    Refs: 1 C. Sanl et al. (arXiv - 2013). 2 L. Berthier (2011).

    Refs: 1 H. Simon (1971). 2 L. Weng et al. (2012). 3 J. P. Gleeson et al. (2014).

    0 12 24 36 48 60 72 840

    10

    20

    30

    40

    time (hours)

    num

    ber o

    f tw

    eets

    /uni

    t tim

    e daily tweet cycles

    propogations of #hashtags 0 10 20 30 40 50 60 70 80 90

    0

    5

    10

    15

    20

    25

    4(l=

    2R,

    )

    (s)

    =0.652=0.725=0.741=0.749=0.753=0.755=0.760=0.761=0.762=0.766=0.770=0.771

    (a)

    4(l, )

    h

    4(l, )

    mobility of beads

    spatiotemporal granular flow

    time

    0.2

    0.6

    1

    1.4

    1.8

    *

    P(r

    =2

    R,t

    )M

    M

    Twitter #hashtag analysis

    single beads: groups:

    perim

    eter

    quantifying dynamic heterogeneity:

    time (s) 0 0.5 1 1.5 2

    [Ref:2]

    [Ref:2]

    #nice: #pepsi:

    observation: artificial representation:

    0 10 20 30 40 50 60

    time (hours) 0 1 2 3 4 5 6 7 8

    time (hours)

    analysis:

    time (hours)

    cum

    ulat

    ive

    time (hours)

    cum

    ulat

    ive

    5 mm

    Inset: The displacement field demonstrates local heterogeneities in the flow.

    A typical snapshot of an experiment: The white spots indicate the positions of the beads floating on surface waves.

    [email protected]

    http://fcxn.wordpress.com ! Month 6 General Meeting

    http://xn.unamur.be

    Fluctuations drive viral memes in online social media: Integrating criticality into network science

    Ceyda Sanl, Vsevolod Salnikov, Lionel Tabourier, and Renaud Lambiotte

    CompleXity Networks, naXys, University of Namur, Belgium.

    To spread our posts throughout online social network such as Twitter: When do we need to post? How often should a #hashtag be posted? These questions emphasize the time features of our twitting activity. They would be controlled much more easily compared to the followings: What we post and how many number of followers we have.

    To be mobile in dense granular media such as highly packed beads on surface waves: Do single beads move independently or form a group? Is the trajectory of each bead regular in time? The quantification of the bead dynamics shows that the beads perform heterogenous motion with a distinct time scale to characterize this heterogeneity.

    restricted amount of attention restricted amount of space

    Restricted amount of sources forces social and physical systems to present emergence of order.

    hypothesis

    Twitter users want to spread their messages and beads under driving want to be mobile. As a result, the twitter users collectively advertise and the beads form groups to move together. Both systems self-organize and create dynamic heterogeneity.

    The origin of the fluctuations in dynamics would be the same origins:

    Therefore, the interpretation of the dynamic heterogeneity of the beads in a critical limit would help to characterize viral memes (#hashtags) in twitter.

    Refs: 1 C. Sanl et al. (arXiv - 2013). 2 L. Berthier (2011).

    Refs: 1 H. Simon (1971). 2 L. Weng et al. (2012). 3 J. P. Gleeson et al. (2014).

    0 12 24 36 48 60 72 840

    10

    20

    30

    40

    time (hours)

    num

    ber o

    f tw

    eets

    /uni

    t tim

    e daily tweet cycles

    propogations of #hashtags 0 10 20 30 40 50 60 70 80 90

    0

    5

    10

    15

    20

    25

    4(l=

    2R,

    )

    (s)

    =0.652=0.725=0.741=0.749=0.753=0.755=0.760=0.761=0.762=0.766=0.770=0.771

    (a)

    4(l, )

    h

    4(l, )

    mobility of beads

    spatiotemporal granular flow

    time

    0.2

    0.6

    1

    1.4

    1.8

    *

    P(r

    =2

    R,t

    )M

    M

    Twitter #hashtag analysis

    single beads: groups:

    perim

    eter

    quantifying dynamic heterogeneity:

    time (s) 0 0.5 1 1.5 2

    [Ref:2]

    [Ref:2]

    #nice: #pepsi:

    observation: artificial representation:

    0 10 20 30 40 50 60

    time (hours) 0 1 2 3 4 5 6 7 8

    time (hours)

    analysis:

    time (hours)

    cum

    ulat

    ive

    time (hours)

    cum

    ulat

    ive

    Social Dynamic Behavior Patterns

    @CeydaSanli

    CompleXity Networks

    5 mm

    Inset: The displacement field demonstrates local heterogeneities in the flow.

    A typical snapshot of an experiment: The white spots indicate the positions of the beads floating on surface waves.

    [email protected]

    http://fcxn.wordpress.com ! Month 6 General Meeting

    http://xn.unamur.be

    Fluctuations drive viral memes in online social media: Integrating criticality into network science

    Ceyda Sanl, Vsevolod Salnikov, Lionel Tabourier, and Renaud Lambiotte

    CompleXity Networks, naXys, University of Namur, Belgium.

    To spread our posts throughout online social network such as Twitter: When do we need to post? How often should a #hashtag be posted? These questions emphasize the time features of our twitting activity. They would be controlled much more easily compared to the followings: What we post and how many number of followers we have.

    To be mobile in dense granular media such as highly packed beads on surface waves: Do single beads move independently or form a group? Is the trajectory of each bead regular in time? The quantification of the bead dynamics shows that the beads perform heterogenous motion with a distinct time scale to characterize this heterogeneity.

    restricted amount of attention restricted amount of space

    Restricted amount of sources forces social and physical systems to present emergence of order.

    hypothesis

    Twitter users want to spread their messages and beads under driving want to be mobile. As a result, the twitter users collectively advertise and the beads form groups to move together. Both systems self-organize and create dynamic heterogeneity.

    The origin of the fluctuations in dynamics would be the same origins:

    Therefore, the interpretation of the dynamic heterogeneity of the beads in a critical limit would help to characterize viral memes (#hashtags) in twitter.

    Refs: 1 C. Sanl et al. (arXiv - 2013). 2 L. Berthier (2011).

    Refs: 1 H. Simon (1971). 2 L. Weng et al. (2012). 3 J. P. Gleeson et al. (2014).

    0 12 24 36 48 60 72 840

    10

    20

    30

    40

    time (hours)

    num

    ber o

    f tw

    eets

    /uni

    t tim

    e daily tweet cycles

    propogations of #hashtags 0 10 20 30 40 50 60 70 80 90

    0

    5

    10

    15

    20

    25

    4(l=

    2R,

    )

    (s)

    =0.652=0.725=0.741=0.749=0.753=0.755=0.760=0.761=0.762=0.766=0.770=0.771

    (a)

    4(l, )

    h

    4(l, )

    mobility of beads

    spatiotemporal granular flow

    time

    0.2

    0.6

    1

    1.4

    1.8

    *

    P(r

    =2R

    ,t)

    MM

    Twitter #hashtag analysis

    single beads: groups:

    perim

    eter

    quantifying dynamic heterogeneity:

    time (s) 0 0.5 1 1.5 2

    [Ref:2]

    [Ref:2]

    #nice: #pepsi:

    observation: artificial representation:

    0 10 20 30 40 50 60

    time (hours) 0 1 2 3 4 5 6 7 8

    time (hours)

    analysis:

    time (hours)

    cum

    ulat

    ive

    time (hours)

    cum

    ulat

    ive

    August 31, 2015, Meeting.

  • Research Questions

    Social Dynamic Behavior Patterns 1C. Sanli, CompleXity Networks, UNamur

    data science behavior

    science

    nonequilibrium physics

    ? online social media computational

    social science

    complex networks

    complex systems

    (bursts)

    (dynamic heterogeneity)

  • Research Interests

    C. Sanli, CompleXity Networks, UNamur

    hashtag diffusion in Twitter

    communication patterns of online users

    timeSocial Dynamic Behavior Patterns 2

    circadian human behavior (internal)

    elections, discoveries, etc. (external)

    complex decision-making

    RT + @ RE

    WHO WHOM

    aU : activity of users

    RT

    @

    RE

    RT + @ RE

    pU : popularity of users

    RT

    @

    RE

    KPI

  • Discrete Digital to Continuous Behavior

    C. Sanli, CompleXity Networks, UNamur

    Not everything is connected (structure), no homogeneity in time (temporal) = complexity

    What do we measure from the data? = challenge

    Social Dynamic Behavior Patterns 3

    {hash":["OptimizRBudapest"],"source":"stream","user_alias":"ateknea","corpus":["en"],"text":"See you all in August 26-27, 2015! #OptimizRBudapest @CeydaSanli,"_id":"010101010","date":1440499664,"at":[{"type":"","alias":"CeydaSanli"}], "user_id":"101010101"}

  • C. Sanli, CompleXity Networks, UNamur

    Two Examples from My Research: Local Variation of

    Hashtag Spike Trains and Popularity in Twitter

    Temporal Patterns of Online Communication in Spreading a Scientific Rumor: How Often, Who Interacts with Whom?

    C. Sanl and R. Lambiotte, PLoS ONE 10(7): e0131704 (2015).

    C. Sanl and R. Lambiotte, Frontiers in Physics: Computational Social Science 3(79), (2015).

    Social Dynamic Behavior Patterns 4

  • The UpshotPOWER OF FICTION

    Why Rumors Outrace the Truth OnlineSEPT. 29, 2014

    Photo

    CreditTomi Um

    Brendan Nyhan@BrendanNyhan

    Continue reading the main storyShare This Page

    EmailShareTweetSave

    Information Diffusion in Twitter

    C. Sanli, CompleXity Networks, UNamur

    tweets retweets (RT) mentions (@) replies (RE)

    Tomi Um

    Social Dynamic Behavior Patterns 5

    Hashtag Diffusion in Twitter

    C. Sanli, CompleXity Networks, UNamur

    hashtag

    hashtag spike train

    time

    coun

    t

    Social dynamic behaviour patterns 1

    I. Part:

    II. Part: RT + @ RE

    WHO WHOM

    aU : activity of users

    RT

    @

    RE

    RT + @ RE

    pU : popularity of users

    RT

    @

    RE

  • Spike Trains

    C. Sanli, CompleXity Networks, UNamur

    time

    coun

    t

    t t0 f

    I. LOCAL VARIABLE OF A TIME SERIES

    Time series in social system include interaction among agents. Considering online social

    network such as Twitter, we address self-organized optimizing of popularity of information.

    To this end, we create time series of #hashtag propogation, user activity, and user #hashtag

    activity.

    In a time series, if a time delay between successive events, inter-event interval , is a

    resultant of independent events, the distrubution of inter-event interval is Poissonian. If not,

    many bursty events are observed and therefore forward propogation of a signal is a function

    of its temporal history. Thus, quantifying is crucial.

    Local variable Lv is an alternative way to characterize whether a time series is Poissonian

    or non-Poissonian. For a stationarly process, Lv is a ratio of the dierence between the

    inter-event interval of forward event and the inter-event interval of backward event to the

    sum of these inter-event intervals. Suppose that a signal propogates in distinct time such as

    1 . . . , i1, i, i+1, . . . N . Then, at i, the inter-event interval of forward event is i+1 =

    i+1 i and the inter-event interval of backward event is i = i i1. Consequently, Lvis

    Lv =3

    N 2

    N1X

    i=2

    (i+1 i) (i i1)(i+1 i) + (i i1)

    2=

    i+1 ii+1 + i

    2. (1)

    Here, N is the total appearance of a time series in distinct times. Multiple activity in same

    i is ignored.

    If Lv = 1 the distribution of the inter-event interval of a time series is Poissonian. If a

    time series considers significant amount of bursty activity, the distribution is non-Poissonian.

    When N < 3 the distribution is automatically assumed to be Poissonian.

    II. LIMITS OF Lv

    Rank of a time series can be defined as how many activity proceeded in distinct times i.

    If events occur in multiple dierent i, N 3, the signal has high rank. If a time serie is

    too short, N 3, the signal has low rank.

    2

    100

    102

    104

    106

    0

    50

    100

    150

    200

    250

    300

    rh

    Fv

    < rh>=11

    < rh>= 2

    Real activity(a)

    FV = 1

    100

    102

    104

    106

    0

    50

    100

    150

    200

    250

    300

    rh

    Fv

    < rh>=11

    < rh>= 2

    (b) Random activity

    FV = 1

    FIG. 7. Local variation Lv of single #hashtag time series versus low rank rh of the corresponsing

    #hashtag. (a) Real #hashtag propogation. (b) Randomly selected #hashtag activity from real

    data set.

    0 50 100 150 200 250 300 350

    0

    0.5

    1

    1.5

    2

    2.5

    3

    3.5

    h (hour)

    Lv

    < r

    h>=91127

    < rh>=18553

    < rh>= 1678

    < rh>= 318

    < rh>= 174

    < rh>= 117

    < rh>= 86

    < rh>= 68

    < rh>= 56

    < rh>= 47

    < rh>= 41

    < rh>= 35

    Real activity(a)

    0 50 100 150 200 250 300 350

    0

    0.5

    1

    1.5

    2

    2.5

    3

    3.5

    h (hour)

    Lv

    < rh>=91127

    < rh>=18553

    < rh>= 1678

    < rh>= 318

    < rh>= 174

    < rh>= 117

    < rh>= 86

    < rh>= 68

    < rh>= 56

    < rh>= 47

    < rh>= 41

    < rh>= 35

    FIG. 8. Local variation Lv of single #hashtag time series versus life time (h) of the corresponsing

    #hashtag. (a) Real #hashtag propogation. (b) Randomly selected #hashtag activity from real

    data set..

    5

    I. DAILY CYCLE OF #HASHTAGS

    00:00 03:00 06:00 09:00 12:00 15:00 18:00 21:00 24:000

    0.05

    0.1

    0.15

    0.2

    0.25

    0.3

    0.35

    0.4

    0.45

    0.5

    1 day (hour)

    PD

    F (

    no

    rma

    lize

    d p

    rob

    ab

    ility

    de

    nsi

    ty)

    of

    #h

    ash

    tag

    s

    total

    rush hour

    dead hour

    FIG. 1. Daily activity of #hashtags: Normalized probability density (PDF) of the activity versus

    day time.

    II. HETEROGENEITY IN POPULARITY AND LIFE TIME OF #HASHTAGS

    104

    102

    100

    102

    104

    100

    101

    102

    103

    104

    105

    106

    h (hour)

    r h

    r =2h

    FIG. 2. Rank of #hashtag rh versus life time of #hashtag h.

    2

    . . .

    I. DAILY CYCLE OF #HASHTAGS

    00:00 03:00 06:00 09:00 12:00 15:00 18:00 21:00 24:000

    0.05

    0.1

    0.15

    0.2

    0.25

    0.3

    0.35

    0.4

    0.45

    0.5

    1 day (hour)

    PD

    F (

    no

    rma

    lize

    d p

    rob

    ab

    ility

    de

    nsi

    ty)

    of

    #h

    ash

    tag

    s

    total

    rush hour

    dead hour

    FIG. 1. Daily activity of #hashtags: Normalized probability density (PDF) of the activity versus

    day time.

    II. HETEROGENEITY IN POPULARITY AND LIFE TIME OF #HASHTAGS

    104

    102

    100

    102

    104

    100

    101

    102

    103

    104

    105

    106

    h (hour)

    r h

    r =2h

    FIG. 2. Rank of #hashtag rh versus life time of #hashtag h.

    2

    I. DAILY CYCLE OF #HASHTAGS

    00:0012:0000:0012:0000:0012:0000:0012:0000:0012:0000:0012:0000:000

    10

    20

    30

    40

    50

    60

    70

    80

    hour

    count/m

    in.

    #ledebat

    #hollande

    #sarkozy

    #votehollande

    #fh2012

    #france2012

    FIG. 1. ...

    hpi =

    p

    2

    Social Dynamic Behavior Patterns 6

    = popularity

  • C. Sanli, CompleXity Networks, UNamur

    Local Analysis on Hashtag Spike Trains

    Social Dynamic Behavior Patterns 7

    hash

    tag

    coun

    t

    time

  • Populars are Regular

    C. Sanli, CompleXity Networks, UNamur

    8

    0

    5

    10

    15

    20

    25

    30

    0 1 2 3 4 50

    5

    10

    15

    20

    25

    30

    =91127 =18553 = 1678 = 318 = 174 = 117 = 86 = 68 = 56 = 47 = 41 = 35

    =91127 =18553 = 1678 = 318 = 174 = 117 = 86 = 68 = 56 = 47 = 41 = 35

    LV

    P(

    )L V

    P(

    )L V

    Real activity(a)

    Random activity(b)

    FIG. 7. Probability density function (PDF) of the local vari-ation LV of real hashtag propagation (a) and random hash-tag time sequence (b). Two distinct shapes are visible: (a)From high p to low p, the peak position of P (LV ) shifts fromlow values of LV to higher values of LV . (b) P (LV ) alwayspeaks around 1 for the random sequences generated by arti-ficial hashtag spike trains. The same color coding is appliedas used in Fig. 6.

    14 (ACM, New York, NY, USA, 2014) pp. 913924.[9] U. Frana, H. Sayama, C. McSwiggen, R. Daneshvar, and

    Y. Bar-Yam, ArXiv e-prints (2014), arXiv:1411.0722[physics.soc-ph].

    [10] A. Mollgaard and J. Mathiesen, ArXiv e-prints (2015),arXiv:1502.03224 [physics.soc-ph].

    [11] J. Ratkiewicz, S. Fortunato, A. Flammini, F. Menczer,and A. Vespignani, Phys. Rev. Lett. 105, 158701 (2010).

    [12] J. Borge-Holthoefer, A. Rivero, I. Garca, E. Cauh,A. Ferrer, D. Ferrer, D. Francos, D. Iiguez, M. P. Prez,G. Ruiz, F. Sanz, F. Serrano, C. Vias, A. Tarancn, andY. Moreno, PLoS ONE 6, e23883 (2011).

    [13] S. Gonzlez-Bailn, J. Borge-Holthoefer, A. Rivero, andY. Moreno, Sci. Rep. 1, 197 (2011).

    [14] K. Sasahara, Y. Hirata, M. Toyoda, M. Kitsuregawa, andK. Aihara, PLoS ONE 8, e61823 (2013).

    [15] D. Y. Kenett, F. Morstatter, H. E. Stanley, and H. Liu,PLoS ONE 9, e102001 (2014).

    [16] F. Deschtres and D. Sornette, Phys. Rev. E 72, 016112(2005).

    0 0.5 1 1.5 2 2.5 30

    0.5

    1

    1.5

    2

    2.5

    3

    LV (t1)

    L V(t 2

    )

    101 102 103 104 1050

    0.2

    0.4

    0.6

    0.8

    1

    r (L V

    (t 1),

    L V(t 2

    ))

    (a)

    (b)

    =91127 =18553 = 1678 = 318 = 174 = 117 = 86 = 68 = 56 = 47

    bursty regular

    FIG. 8. Linear correlation of LV through real hashtag spiketrains. (a) The linear relation of the first and the secondhalves of the empirical spike trains, LV (t1) and LV (t1), re-spectively, are investigated. The legend ranks hpi in dierentcolors and symbols. (b) The Pearson correlation coecientr(LV (t1), LV (t2)) between these quantities show that whilethe temporal correlation through moderately popular hashtagis maximum, r reaches the minimum values for both bursty(high LV and low p) and regular (low LV and high p) spiketrains.

    [17] L. Weng, F. Menczer, and Y.-Y. Ahn, Sci. Rep. 3, 2522(2013).

    [18] J. Cheng, L. Adamic, P. A. Dow, J. M. Kleinberg, andJ. Leskovec, in Proceedings of the 23rd International Con-ference on World Wide Web, WWW 14 (ACM, NewYork, NY, USA, 2014) pp. 925936.

    [19] L. Weng, A. Flammini, A. Vespignani, and F. Menczer,Sci. Rep. 2, 335 (2012).

    [20] J. P. Gleeson, J. A. Ward, K. P. OSullivan, and W. T.Lee, Phys. Rev. Lett. 112, 048701 (2014).

    [21] U. Cetin and H. O. Bingol, Phys. Rev. E 90, 032801(2014).

    [22] J. P. Gleeson, K. P. OSullivan, R. A. Baos, andY. Moreno, ArXiv e-prints (2015), arXiv:1501.05956[physics.soc-ph].

    [23] S. Shinomoto, K. Shima, and J. Tanji, Neural Comput.15, 2823 (2003).

    [24] S. Koyama and S. Shinomoto, Journal of Physics A:Mathematical and General 38, L531 (2005).

    [25] K. Miura, M. Okada, and S. ichi Amari, Neural Comput.18, 2359 (2006).

    8

    0

    5

    10

    15

    20

    25

    30

    0 1 2 3 4 50

    5

    10

    15

    20

    25

    30

    =91127 =18553 = 1678 = 318 = 174 = 117 = 86 = 68 = 56 = 47 = 41 = 35

    =91127 =18553 = 1678 = 318 = 174 = 117 = 86 = 68 = 56 = 47 = 41 = 35

    LVP(

    )

    L VP(

    )

    L V

    Real activity(a)

    Random activity(b)

    FIG. 7. Probability density function (PDF) of the local vari-ation LV of real hashtag propagation (a) and random hash-tag time sequence (b). Two distinct shapes are visible: (a)From high p to low p, the peak position of P (LV ) shifts fromlow values of LV to higher values of LV . (b) P (LV ) alwayspeaks around 1 for the random sequences generated by arti-ficial hashtag spike trains. The same color coding is appliedas used in Fig. 6.

    14 (ACM, New York, NY, USA, 2014) pp. 913924.[9] U. Frana, H. Sayama, C. McSwiggen, R. Daneshvar, and

    Y. Bar-Yam, ArXiv e-prints (2014), arXiv:1411.0722[physics.soc-ph].

    [10] A. Mollgaard and J. Mathiesen, ArXiv e-prints (2015),arXiv:1502.03224 [physics.soc-ph].

    [11] J. Ratkiewicz, S. Fortunato, A. Flammini, F. Menczer,and A. Vespignani, Phys. Rev. Lett. 105, 158701 (2010).

    [12] J. Borge-Holthoefer, A. Rivero, I. Garca, E. Cauh,A. Ferrer, D. Ferrer, D. Francos, D. Iiguez, M. P. Prez,G. Ruiz, F. Sanz, F. Serrano, C. Vias, A. Tarancn, andY. Moreno, PLoS ONE 6, e23883 (2011).

    [13] S. Gonzlez-Bailn, J. Borge-Holthoefer, A. Rivero, andY. Moreno, Sci. Rep. 1, 197 (2011).

    [14] K. Sasahara, Y. Hirata, M. Toyoda, M. Kitsuregawa, andK. Aihara, PLoS ONE 8, e61823 (2013).

    [15] D. Y. Kenett, F. Morstatter, H. E. Stanley, and H. Liu,PLoS ONE 9, e102001 (2014).

    [16] F. Deschtres and D. Sornette, Phys. Rev. E 72, 016112(2005).

    0 0.5 1 1.5 2 2.5 30

    0.5

    1

    1.5

    2

    2.5

    3

    LV (t1)

    L V(t 2

    )

    101 102 103 104 1050

    0.2

    0.4

    0.6

    0.8

    1

    r (L V

    (t 1),

    L V(t 2

    ))

    (a)

    (b)

    =91127 =18553 = 1678 = 318 = 174 = 117 = 86 = 68 = 56 = 47

    bursty regular

    FIG. 8. Linear correlation of LV through real hashtag spiketrains. (a) The linear relation of the first and the secondhalves of the empirical spike trains, LV (t1) and LV (t1), re-spectively, are investigated. The legend ranks hpi in dierentcolors and symbols. (b) The Pearson correlation coecientr(LV (t1), LV (t2)) between these quantities show that whilethe temporal correlation through moderately popular hashtagis maximum, r reaches the minimum values for both bursty(high LV and low p) and regular (low LV and high p) spiketrains.

    [17] L. Weng, F. Menczer, and Y.-Y. Ahn, Sci. Rep. 3, 2522(2013).

    [18] J. Cheng, L. Adamic, P. A. Dow, J. M. Kleinberg, andJ. Leskovec, in Proceedings of the 23rd International Con-ference on World Wide Web, WWW 14 (ACM, NewYork, NY, USA, 2014) pp. 925936.

    [19] L. Weng, A. Flammini, A. Vespignani, and F. Menczer,Sci. Rep. 2, 335 (2012).

    [20] J. P. Gleeson, J. A. Ward, K. P. OSullivan, and W. T.Lee, Phys. Rev. Lett. 112, 048701 (2014).

    [21] U. Cetin and H. O. Bingol, Phys. Rev. E 90, 032801(2014).

    [22] J. P. Gleeson, K. P. OSullivan, R. A. Baos, andY. Moreno, ArXiv e-prints (2015), arXiv:1501.05956[physics.soc-ph].

    [23] S. Shinomoto, K. Shima, and J. Tanji, Neural Comput.15, 2823 (2003).

    [24] S. Koyama and S. Shinomoto, Journal of Physics A:Mathematical and General 38, L531 (2005).

    [25] K. Miura, M. Okada, and S. ichi Amari, Neural Comput.18, 2359 (2006).

    8

    0

    5

    10

    15

    20

    25

    30

    0 1 2 3 4 50

    5

    10

    15

    20

    25

    30

    =91127 =18553 = 1678 = 318 = 174 = 117 = 86 = 68 = 56 = 47 = 41 = 35

    =91127 =18553 = 1678 = 318 = 174 = 117 = 86 = 68 = 56 = 47 = 41 = 35

    LV

    P(

    )L V

    P(

    )L V

    Real activity(a)

    Random activity(b)

    FIG. 7. Probability density function (PDF) of the local vari-ation LV of real hashtag propagation (a) and random hash-tag time sequence (b). Two distinct shapes are visible: (a)From high p to low p, the peak position of P (LV ) shifts fromlow values of LV to higher values of LV . (b) P (LV ) alwayspeaks around 1 for the random sequences generated by arti-ficial hashtag spike trains. The same color coding is appliedas used in Fig. 6.

    14 (ACM, New York, NY, USA, 2014) pp. 913924.[9] U. Frana, H. Sayama, C. McSwiggen, R. Daneshvar, and

    Y. Bar-Yam, ArXiv e-prints (2014), arXiv:1411.0722[physics.soc-ph].

    [10] A. Mollgaard and J. Mathiesen, ArXiv e-prints (2015),arXiv:1502.03224 [physics.soc-ph].

    [11] J. Ratkiewicz, S. Fortunato, A. Flammini, F. Menczer,and A. Vespignani, Phys. Rev. Lett. 105, 158701 (2010).

    [12] J. Borge-Holthoefer, A. Rivero, I. Garca, E. Cauh,A. Ferrer, D. Ferrer, D. Francos, D. Iiguez, M. P. Prez,G. Ruiz, F. Sanz, F. Serrano, C. Vias, A. Tarancn, andY. Moreno, PLoS ONE 6, e23883 (2011).

    [13] S. Gonzlez-Bailn, J. Borge-Holthoefer, A. Rivero, andY. Moreno, Sci. Rep. 1, 197 (2011).

    [14] K. Sasahara, Y. Hirata, M. Toyoda, M. Kitsuregawa, andK. Aihara, PLoS ONE 8, e61823 (2013).

    [15] D. Y. Kenett, F. Morstatter, H. E. Stanley, and H. Liu,PLoS ONE 9, e102001 (2014).

    [16] F. Deschtres and D. Sornette, Phys. Rev. E 72, 016112(2005).

    0 0.5 1 1.5 2 2.5 30

    0.5

    1

    1.5

    2

    2.5

    3

    LV (t1)

    L V(t 2

    )

    101 102 103 104 1050

    0.2

    0.4

    0.6

    0.8

    1

    r (L V

    (t 1),

    L V(t 2

    ))

    (a)

    (b)

    =91127 =18553 = 1678 = 318 = 174 = 117 = 86 = 68 = 56 = 47

    bursty regular

    FIG. 8. Linear correlation of LV through real hashtag spiketrains. (a) The linear relation of the first and the secondhalves of the empirical spike trains, LV (t1) and LV (t1), re-spectively, are investigated. The legend ranks hpi in dierentcolors and symbols. (b) The Pearson correlation coecientr(LV (t1), LV (t2)) between these quantities show that whilethe temporal correlation through moderately popular hashtagis maximum, r reaches the minimum values for both bursty(high LV and low p) and regular (low LV and high p) spiketrains.

    [17] L. Weng, F. Menczer, and Y.-Y. Ahn, Sci. Rep. 3, 2522(2013).

    [18] J. Cheng, L. Adamic, P. A. Dow, J. M. Kleinberg, andJ. Leskovec, in Proceedings of the 23rd International Con-ference on World Wide Web, WWW 14 (ACM, NewYork, NY, USA, 2014) pp. 925936.

    [19] L. Weng, A. Flammini, A. Vespignani, and F. Menczer,Sci. Rep. 2, 335 (2012).

    [20] J. P. Gleeson, J. A. Ward, K. P. OSullivan, and W. T.Lee, Phys. Rev. Lett. 112, 048701 (2014).

    [21] U. Cetin and H. O. Bingol, Phys. Rev. E 90, 032801(2014).

    [22] J. P. Gleeson, K. P. OSullivan, R. A. Baos, andY. Moreno, ArXiv e-prints (2015), arXiv:1501.05956[physics.soc-ph].

    [23] S. Shinomoto, K. Shima, and J. Tanji, Neural Comput.15, 2823 (2003).

    [24] S. Koyama and S. Shinomoto, Journal of Physics A:Mathematical and General 38, L531 (2005).

    [25] K. Miura, M. Okada, and S. ichi Amari, Neural Comput.18, 2359 (2006).

    hashtag dynamics artificial dynamics

    ranking popularity

    C. Sanl and R. Lambiotte, PLoS ONE 10(7): e0131704 (2015).

    Social Dynamic Behavior Patterns 8

  • Bursty versus Regular

    C. Sanli, CompleXity Networks, UNamur

    1 2 3 4 5 6

    00.20.40.60.8

    11.21.41.61.8

    log ()

    realrandom

    (

    ) L V

    10

    real hashtags:decay in with increasing p

    2010

    01020304050

    zva

    lues (LV) = 1

    realrandom

    0 0 =

    (a)

    (b)

    1 2 3 4 5 6

    00.20.40.60.8

    11.21.41.61.8

    log ()

    realrandom

    (

    ) L V

    10

    real hashtags:decay in with increasing p

    2010

    01020304050

    zva

    lues (LV) = 1

    realrandom

    0 0 =

    (a)

    (b)

    bursty

    regular

    Social Dynamic Behavior Patterns 9

    C. Sanl and R. Lambiotte, PLoS ONE 10(7): e0131704 (2015).

    KPI

  • C. Sanli, CompleXity Networks, UNamur

    Local Analysis on Communication Spike Trains

    Social Dynamic Behavior Patterns 10

    user

    co

    unt

    time

  • Populars are Random

    C. Sanli, CompleXity Networks, UNamur Social Dynamic Behavior Patterns 11

    0

    5

    10

    15

    20

    25

    WH

    O:

    < aU>=190< aU>=112< aU>= 84< aU>= 44< aU>= 25< aU>= 17< aU>= 12

    0 1 2 3 40

    10

    20

    30

    40

    50

    60

    < pU>=4418< pU>=1037< pU>= 570< pU>= 193< pU>= 48< pU>= 18< pU>= 11

    P(

    )L V

    WH

    OM

    : P(

    ) L V

    LV

    (a)

    (b) popularityof the user increases, the patterns become regular

    activityof the user plays no role

    0

    5

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    25

    WH

    O:

    < aU>=190< aU>=112< aU>= 84< aU>= 44< aU>= 25< aU>= 17< aU>= 12

    0 1 2 3 40

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    < pU>=4418< pU>=1037< pU>= 570< pU>= 193< pU>= 48< pU>= 18< pU>= 11

    P(

    )L V

    WH

    OM

    : P(

    ) L V

    LV

    (a)

    (b) popularityof the user increases, the patterns become regular

    activityof the user plays no role

    0

    5

    10

    15

    20

    25

    WH

    O:

    < aU>=190< aU>=112< aU>= 84< aU>= 44< aU>= 25< aU>= 17< aU>= 12

    0 1 2 3 40

    10

    20

    30

    40

    50

    60

    < pU>=4418< pU>=1037< pU>= 570< pU>= 193< pU>= 48< pU>= 18< pU>= 11

    P(

    )L V

    WH

    OM

    : P(

    ) L V

    LV

    (a)

    (b) popularityof the user increases, the patterns become regular

    activityof the user plays no role

    always bursty

    RT + @ RE

    WHO WHOM

    aU : activity of users

    RT

    @

    RE

    RT + @ RE

    pU : popularity of users

    RT

    @

    RE

    KPI

  • Sanli et al. Temporal Pattern of Online Communication Spike Trains

    1 1.5 2 2.5 3 3.5 4

    log ()10 U

    (d)

    1 1.5 2 2.5 3 3.5 4

    log ()10 U

    WH

    OM

    : rik

    k, (c)

    0

    0.2

    0.4

    0.6

    0.8

    1

    1 1.5 2 2.5 3 3.5 4

    log ()10 U

    (b)

    1 1.5 2 2.5 3 3.5 4

    log ()10 U

    WH

    O: r

    ikk,

    (a)

    0

    0.2

    0.4

    0.6

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    1

    r

    r

    full,RT

    full,@

    -RT

    -@

    U

    U

    r

    r

    full,RT

    full,@

    -RT

    -@

    U

    U

    Figure 7. Linear correlations of LV of the same users: The procedure and representation of the coef-ficients follow the same procedure as introduced in Fig. 6. However, we now impose the same users inthe same frequency classes. Even though (a, c) present the agreement in the temporal patterns of full andRT spike trains of the same users, with high correlation coefficients in almost all frequency ranges, (b)indicates lower consistency between RT and @ spike trains during entire activity aU and (d) providesa significant result. While less temporal coherence is observed between RT and @ spike trains in lowpopularity pU , the correlation drastically increases with pU .

    Frontiers 17

    C. Sanli, CompleXity Networks, UNamur Social Dynamic Behavior Patterns 12

    Communication Habits of Users Linear (Pearson) correlations of :

    0

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    25

    WH

    O:

    < aU>=190< aU>=112< aU>= 84< aU>= 44< aU>= 25< aU>= 17< aU>= 12

    0 1 2 3 40

    10

    20

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    40

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    60

    < pU>=4418< pU>=1037< pU>= 570< pU>= 193< pU>= 48< pU>= 18< pU>= 11

    P(

    )L V

    WH

    OM

    : P(

    ) L V

    LV

    (a)

    (b) popularityof the user increases, the patterns become regular

    activityof the user plays no role

    C. Sanl and R. Lambiotte, Frontiers in Physics: Computational Social Science 3(79), (2015).

    temporal patterns of @ and RT should be consisted

    for popular users

  • C. Sanli, CompleXity Networks, UNamur Social Dynamic Behavior Patterns 13

    Take Home Messages

    Activity and Popularity of Users in Online Network: Our activity in Twitter is highly driven by the complex-decison making (large KPI set). On the other hand, our popularity is independent of that!

    Structural versus Temporal in Network: Popularity of topics, e.g. hashtags, and users might be strongly influenced by temporal characteristics of the underlying network.

    Ranking Hashtags by Temporal Parameters: Observing bursts in less popular hashtags, popular hashtags give regular signals.