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Research Article

Quantitative and empirical demonstration of the Matthew effect in a study of career longevity

Alexander M. Petersen, Woo-Sung Jung, Jae-Suk Yang, and H. Eugene Stanley
  1. aCenter for Polymer Studies and Department of Physics, Boston University, Boston, MA 02215;
  2. bGraduate Program for Technology and Innovation Management and Department of Physics, Pohang University of Science and Technology, Pohang 790-784, Republic of Korea; and
  3. cSanford C. Benstein and Co. Center for Leadership and Ethics, Columbia Business School, Columbia University, New York, NY 10027

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PNAS January 4, 2011 108 (1) 18-23; https://doi.org/10.1073/pnas.1016733108
Alexander M. Petersen
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  • For correspondence: amp17@physics.bu.edu hes@bu.edu
Woo-Sung Jung
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Jae-Suk Yang
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H. Eugene Stanley
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  • For correspondence: amp17@physics.bu.edu hes@bu.edu
  1. Contributed by H. Eugene Stanley, November 10, 2010 (sent for review November 8, 2009)

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    Fig. 1.

    Graphical illustration of the stochastic Poisson process quantifying career progress with position-dependent progress rate g(x) and stagnancy rate 1 - g(x). A new opportunity, corresponding to the advancement to career position x + 1 from career position x, can refer to a day at work or, even more generally, to any assignment given by an employing body. In this framework, career progress is made at a rate g(x) that is slower than the passing of work time, representing the possibility of career stagnancy. The traditional Poisson process corresponds to a constant progress rate g(x) ≡ λ. Here, we use a functional form for g(x) ≡ 1 - exp[-(x/xc)α] that is increasing with career position x, which captures the salient feature of the Matthew effect, that it becomes easier to make progress the further along the career. In SI Appendix, we further develop an alternative model where the progress rate g(t) depends on time.

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    Fig. 2.

    Demonstration of the fundamental relationship between the progress rate g(x) and the career longevity pdf P(x). The progress rate g(x) represents the probability of moving forward in the career to position x + 1 from position x. The small value of g(x) for small x captures the difficulty in making progress at the beginning of a career. The progress rate increases with career position x, capturing the role of the Matthew effect. We plot five g(x) curves with fixed xc = 103 and different values of the parameter α. The parameter α emerges from the small-x behavior in g(x) as the power-law exponent characterizing P(x). (Inset) Probability density functions P(x) resulting from inserting g(x) with varying α into Eq. 5. The value αc ≡ 1 separates two distinct types of longevity distributions. The distributions resulting from concave career development α < 1 exhibit monotonic statistical regularity over the entire range, with an analytic form approximated by the Gamma distribution Gamma(x; α,xc). The distributions resulting from convex career development α > 1 exhibit bimodal behavior. In the bimodal case, one class of careers is stunted by the difficulty in making progress at the beginning of the career, analogous to a “potential” barrier. The second class of careers forges beyond the barrier and is approximately centered around the crossover xc on a log–log scale.

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    Fig. 3.

    Extremely right-skewed pdfs P(x) of career longevity in several high-impact scientific journals and several major sports leagues. We analyze data from American baseball (Major League Baseball) over the 84-year period 1920–2004, Korean Baseball (Korean Professional Baseball League) over the 25-year period 1982–2007, American basketball (National Basketball Association and American Basketball Association) over the 56-year period 1946–2004, and English soccer (Premier League) over the 15-year period 1992–2007, and several scientific journals over the 42-year period 1958–2000. Solid curves represent least-squares best-fit functions corresponding to the functional form in Eq. 5. (A) Baseball fielder longevity measured in at-bats (pitchers excluded): we find α ≈ 0.77, xc ≈ 2,500 (Korea) and xc ≈ 5,000 (United States). (B) Basketball longevity measured in minutes played: we find α ≈ 0.63, xc ≈ 21,000 minutes. (C) Baseball pitcher longevity measured in IPO: we find α ≈ 0.71, xc ≈ 2,800 (Korea), and xc ≈ 3,400 (United States). (D) Soccer longevity measured in games played: we find α ≈ 0.55, xc ≈ 140 games. (E and F) High-impact journals exhibit similar longevity distributions for the “journal career length,” which we define as the duration between an author’s first and last paper in a particular journal. Deviations occur for long careers due to dataset limitations (for comparison, least-square fits are plotted in E with parameters α ≈ 0.40, xc = 9 years and in F with parameters α ≈ 0.10, xc = 11 years). These statistics are summarized in SI Appendix (Table S2).

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    Fig. 4.

    Probability density function P(z) of common metrics for career success, z. Solid curves represent best-fit functions corresponding to Eq. 5. (A) Career batting statistics in American baseball: Embedded Image, Embedded Image, (RBI = runs batted in). (B) Career statistics in American basketball: Embedded Image, Embedded Image. For clarity, the top set of data in each plot has been multiplied by a constant factor of four in order to separate overlapping data.

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Quantitative and empirical demonstration of the Matthew effect in a study of career longevity
Alexander M. Petersen, Woo-Sung Jung, Jae-Suk Yang, H. Eugene Stanley
Proceedings of the National Academy of Sciences Jan 2011, 108 (1) 18-23; DOI: 10.1073/pnas.1016733108

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Quantitative and empirical demonstration of the Matthew effect in a study of career longevity
Alexander M. Petersen, Woo-Sung Jung, Jae-Suk Yang, H. Eugene Stanley
Proceedings of the National Academy of Sciences Jan 2011, 108 (1) 18-23; DOI: 10.1073/pnas.1016733108
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Proceedings of the National Academy of Sciences: 108 (1)
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