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1 Markets I: The Ecosystem and Exchange-Traded Marketsবাজার অনলাইন 2 Markets II: Rates, FX and Creditবাজার অনলাইন 3 Markets III: Commodities, Energy and Cryptoবাজার অনলাইন 4 Quantitative Methodsপদ্ধতি অনলাইন 5 Derivatives and Volatilityডেরিভেটিভস অনলাইন 6 Rates, Credit, XVA and Riskসুদহার, ঋণ ও ঝুঁকি অনলাইন 7 Research Craft: Predictors, Backtests, Measurement, Portfoliosগবেষণা অনলাইন 8 Strategies I: Equities and Futuresকৌশল অনলাইন 9 Strategies II: Volatility, Relative Value, Macro and the Bank Desksকৌশল অনলাইন 10 Microstructure and Executionএক্সিকিউশন অনলাইন 11 Market Making and High-Frequency Tradingমার্কেট মেকিং অনলাইন 12 Machine Learning for Marketsমেশিন লার্নিং অনলাইন 13 Low-Latency Softwareপ্রযুক্তি অনলাইন 14 Networks, Hardware and Trading Infrastructureপ্রযুক্তি অনলাইন 15 Research, Data and Risk Platformsপ্রযুক্তি অনলাইন 16 The Desk and the Firmপ্রতিষ্ঠান অনলাইন 17 The Industry: Firms, Roles and Careersক্যারিয়ার অনলাইন 18 Interviews I: Maths, Probability and Speedক্যারিয়ার অনলাইন 19 Interviews II: Markets, Trading Games and the Final Roundক্যারিয়ার অনলাইন 20 Interviews III: Codeক্যারিয়ার অনলাইন
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Earth and Space Sciences · পরিভাষা

Limb darkening কী?

Definition 28.5 University Earth and Space Sciences — Year 3 · অধ্যায় 28 — Exoplanets

Limb darkening is the decrease of the surface brightness of a star from the centre of its disc to its edge, the limb. Near the limb the line of sight enters the star’s atmosphere obliquely and reaches unit optical depth in higher, cooler layers, which emit less. It is often written as a quadratic law in μ=cos⁡θ=1−r2\mu = \cos\theta = \sqrt{1 - r^2}, with rr the distance from the centre of the disc in stellar radii: I(μ)/I(1)=1−u1(1−μ)−u2(1−μ)2I(\mu)/I(1) = 1 - u_1(1 - \mu) - u_2(1 - \mu)^2.

Left: a planet with p = R_p/R_ = 0.1 crosses the disc of its star at the impact parameter b = 0.3, at the four contacts 1 to 4; the disc is darker towards the limb. Right: its light curve for a/R_ = 15 and a period of ten days, computed for a star with the quadratic limb-darkening coefficients u_1 = 0.40, u_2 = 0.25 (solid) and for a uniform star (dashed, depth exactly p2 = 1\,\%). Between contacts 2 and 3 the limb-darkened curve is rounded, and deeper than p2 near mid-transit. Left: a planet with p = R_p/R_ = 0.1 crosses the disc of its star at the impact parameter b = 0.3, at the four contacts 1 to 4; the disc is darker towards the limb. Right: its light curve for a/R_ = 15 and a period of ten days, computed for a star with the quadratic limb-darkening coefficients u_1 = 0.40, u_2 = 0.25 (solid) and for a uniform star (dashed, depth exactly p2 = 1\,\%). Between contacts 2 and 3 the limb-darkened curve is rounded, and deeper than p2 near mid-transit.
Left: a planet with p=Rp/R⋆=0.1p = R_p/R_\star = 0.1 crosses the disc of its star at the impact parameter b=0.3b = 0.3, at the four contacts 1 to 4; the disc is darker towards the limb. Right: its light curve for a/R⋆=15a/R_\star = 15 and a period of ten days, computed for a star with the quadratic limb-darkening coefficients u1=0.40u_1 = 0.40, u2=0.25u_2 = 0.25 (solid) and for a uniform star (dashed, depth exactly p2=1 %p^2 = 1\,\%). Between contacts 2 and 3 the limb-darkened curve is rounded, and deeper than p2p^2 near mid-transit.
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