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Confidently Wrong: Why Ignoring Binaries Biases IMF Inference at Large Sample Sizes

Anna L. Rosen

Abstract

The stellar initial mass function (IMF) high-mass slope $α$ is routinely measured by fitting single-star models to photometric samples that contain 20-90% unresolved binaries. This practice introduces a systematic negative bias on $α$ that is constant with sample size $N$. Because posterior credible intervals shrink as $1/\sqrt{N}$, at sufficiently large $N$ the bias exceeds the reported uncertainty and the true value falls outside the credible interval - a regime we call "confidently wrong." We bracket this bias between two limiting observation operators: mass-addition $(m_\text{obs} = m_1 + m_2)$, a formal upper bound on unresolved-system mass overestimation, and luminosity-addition $(m_\text{obs} = L^{-1}(L_1 + L_2))$, an idealized lower-bias photometric case based on the ZAMS mass-luminosity relation. Across four astrophysical environments spanning $α= 1.60-2.30$, we find: (1) mass-addition bias of $0.054-0.086$ with crossover to confidently wrong at $N_\text{cross} \sim 5{,}000-10{,}000$; (2) luminosity-addition bias of $0.011-0.021$ with $N_\text{cross} \sim 75{,}000-150{,}000$; and (3) a binary-aware mixture likelihood that marginalizes over the Moe & Di Stefano (2017) binary population model recovers the true slope in the synthetic tests presented here. Published single-star IMF slopes can therefore plausibly carry systematic errors of order $0.01-0.09$ if unresolved binaries are not modeled, comparable to or exceeding reported uncertainties in some regimes. Since current and upcoming surveys (Gaia, JWST, Roman, LSST) will deliver $N = 10^4-10^6$ resolved stars per rich cluster, binary-aware inference is likely necessary to avoid binary-driven systematic bias in the large-$N$ single-star-fitting regime.

Confidently Wrong: Why Ignoring Binaries Biases IMF Inference at Large Sample Sizes

Abstract

The stellar initial mass function (IMF) high-mass slope is routinely measured by fitting single-star models to photometric samples that contain 20-90% unresolved binaries. This practice introduces a systematic negative bias on that is constant with sample size . Because posterior credible intervals shrink as , at sufficiently large the bias exceeds the reported uncertainty and the true value falls outside the credible interval - a regime we call "confidently wrong." We bracket this bias between two limiting observation operators: mass-addition , a formal upper bound on unresolved-system mass overestimation, and luminosity-addition , an idealized lower-bias photometric case based on the ZAMS mass-luminosity relation. Across four astrophysical environments spanning , we find: (1) mass-addition bias of with crossover to confidently wrong at ; (2) luminosity-addition bias of with ; and (3) a binary-aware mixture likelihood that marginalizes over the Moe & Di Stefano (2017) binary population model recovers the true slope in the synthetic tests presented here. Published single-star IMF slopes can therefore plausibly carry systematic errors of order if unresolved binaries are not modeled, comparable to or exceeding reported uncertainties in some regimes. Since current and upcoming surveys (Gaia, JWST, Roman, LSST) will deliver resolved stars per rich cluster, binary-aware inference is likely necessary to avoid binary-driven systematic bias in the large- single-star-fitting regime.
Paper Structure (8 sections, 14 equations, 5 figures, 1 table)

This paper contains 8 sections, 14 equations, 5 figures, 1 table.

Figures (5)

  • Figure 1: Literature context for the benchmark IMF slopes used in this paper. Published high-mass IMF slopes from the compilation of hennebelle2024 are plotted against the IMF-depth proxy $1/f(m_\mathrm{lo})$, defined here as the number of total IMF stars expected per star above a study's lower-mass fitting limit $m_\mathrm{lo}$. Larger values therefore correspond to shallower surveys that constrain $\alpha$ using only the rare high-mass tail. Points are color-coded by broad environment class, and diamond markers denote measurements that include explicit binary corrections. Horizontal dotted lines mark the four benchmark $\alpha$ values used in this paper.
  • Figure 2: Binary population model from moe2017. (a) Mass-dependent binary fraction $f_\mathrm{b}(m_1)$, showing the step-function dependence from 22% for late M dwarfs to 90% for O stars. Colored bands mark spectral type regions (M, K, G/F, A, B, O). (b) Mass-ratio distribution $p(q \mid m_1)$ for four representative primary masses spanning the full range of power-law index $\gamma$. The narrow peak at $q \approx 1$ is the "twin excess." (c) Distortion of the observed system mass function under mass-addition (dashed) relative to the true single-star IMF (solid) for all four environments. The shaded region highlights the mass overestimate from unresolved binaries.
  • Figure 3: Parameter recovery across four astrophysical environments at $N = 10{,}000$ using the mass-addition operator. (a) True vs. recovered $\alpha$: naive estimates (diamonds, with 95% CIs) are systematically biased low, while binary-aware estimates (circles) are consistent with the truth (dashed line). (b) Residual posterior distributions: naive posteriors (dashed) are shifted negative, confirming systematic bias; binary-aware posteriors (solid) are centered on zero.
  • Figure 4: The "confidently wrong" regime across four astrophysical environments. Each panel shows the 95% credible interval width (solid lines) and absolute bias $|\hat{\alpha}_\mathrm{naive} - \alpha_\mathrm{true}|$ (dotted lines) as functions of sample size $N$ on log-log axes. Four inference configurations are compared: mass-addition naive (orange diamonds), luminosity-addition naive (amber squares), binary-aware mass-addition (blue circles, solid), and binary-aware luminosity-addition (blue triangles, dashed). The gray dashed line shows the $1/\sqrt{N}$ Bernstein--von Mises scaling. The shaded region marks where the mass-addition bias exceeds the CI width --- the "confidently wrong" regime. Both binary-aware models track the $1/\sqrt{N}$ scaling with bias consistent with zero.
  • Figure 5: The "confidently wrong" posteriors under mass-addition for all four environments. Naive posteriors (solid lines) at $N = 1{,}000$, $5{,}000$, $30{,}000$, and $100{,}000$ are shown with progressively darker shading; binary-aware posteriors (dashed) at $N = 100{,}000$ recover the truth (dotted vertical line) in every environment. As $N$ increases, naive posteriors narrow onto the biased value rather than the truth. Bias magnitudes decrease from Solar (0.086) to Low-$Z$ starburst (0.054), but all environments enter the confidently wrong regime. Posteriors are Gaussian approximations from HMC summary statistics.