Section 01
Data Acquisition
All spectra are retrieved from the ESO Science Archive, which provides public access to reduced data products after a 12-month proprietary period.
Primary Instrument: HARPS
| Parameter | Value | Notes |
|---|---|---|
| Telescope | ESO 3.6m, La Silla | Chile |
| Spectral Resolution | R ~ 115,000 | vs. R ~ 42,000 in Schmitt (2010) |
| Wavelength Coverage | 3780 – 6910 Å | Two arms: blue + red |
| Mode | HAM | High Accuracy Mode |
| Data Product | S1D | 1D merged, wavelength-calibrated, barycentric-corrected |
| Archive Epochs (55 Cnc A) | 88 spectra | All used after quality inspection |
Instrument Suite
| Instrument | Facility | Wavelength Range | Resolution | Usage |
|---|---|---|---|---|
| HARPS | ESO 3.6m, La Silla, Chile | 3780 – 6910 Å (optical) | R ~ 115,000 | Primary instrument for all FGK/M dwarf targets — optical stellar spectra |
| HST/STIS | Hubble Space Telescope — Space Telescope Imaging Spectrograph | ~1150 – 10,000 Å (UV + optical) | Varies by grating | UV oxygen lines inaccessible from ground. Gratings used: G140M, G750L, G430L (55 Cnc A); E140H, E140M, E230H, E230M (Alpha Cen A) |
| HST/COS | Hubble Space Telescope — Cosmic Origins Spectrograph | ~1150 – 3200 Å (far-UV) | High sensitivity far-UV | Far-UV spectra where available; high sensitivity for faint far-UV features |
Multi-Wavelength Strategy
Optical HARPS spectra cover the majority of target elements. HST UV coverage (STIS + COS) unlocks element lines that are blocked by Earth's atmosphere — critical for N, O, C UV transitions and for cross-validating ground-based oxygen measurements. HST data retrieved from MAST (Mikulski Archive for Space Telescopes, mast.stsci.edu).
Target Selection Criteria
- 1Confirmed exoplanet host (NASA Exoplanet Archive)
- 2FGK spectral type (Teff 4000–7000 K) — ATLAS9 grid; M dwarfs (Teff < 4000 K) use MARCS spherical grid
- 3Main sequence dwarf (log g > 3.8) — plane-parallel atmosphere valid
- 4V < 9 mag — sufficient HARPS S/N achievable
- 5Multiple HARPS epochs available for co-adding
- 6Not a spectroscopic binary
Spectrum Co-Adding (55 Cnc A — 88 Epochs)
This makes phosphorus (P I 6034 Å, EW ~ 12 mÅ) and lithium (Li I 6707 Å, EW ~ 3 mÅ) accessible — both invisible in a single exposure.
| Element | Line EW | Single epoch S/N 100 | Co-add S/N 940 |
|---|---|---|---|
| Fe I | ~80 mÅ | Yes (40σ) | Yes (400σ) |
| Ca I | ~40 mÅ | Yes (20σ) | Yes (200σ) |
| P I | ~12 mÅ | No (6σ — marginal) | Yes (60σ) |
| Li I | ~3 mÅ | No (1.5σ) | Yes (15σ) |
Radial Velocity Correction
Each spectrum is shifted to the stellar rest frame before co-adding: λ_rest = λ_obs / (1 + v_r / c). 55 Cnc A hosts 5 planets with total RV variation up to ±100 m/s — equivalent to ~0.002 Å at 6000 Å. Uncorrected co-adding blurs line profiles at the 0.2-pixel level.
Section 02
Stellar Model Atmosphere
We use the ATLAS9 one-dimensional, plane-parallel, LTE model atmosphere grid of Castelli & Kurucz (2003) — the current standard for FGK main-sequence dwarfs.
ATLAS9 Model Assumptions
| Assumption | Plain English | Valid For |
|---|---|---|
| 1D plane-parallel geometry | Atmosphere modeled as flat parallel layers | Main-sequence dwarfs (log g > 3.5) |
| LTE | Each layer in thermal equilibrium — Boltzmann/Saha distributions | Dense collision-dominated FGK photospheres |
| Opacity Distribution Functions | Millions of line opacities treated statistically for efficiency | All spectral types |
Cross-validation: key results also run through MARCS grid (Gustafsson et al. 2008). ATLAS9 vs. MARCS differences are typically < 0.03 dex for FGK dwarfs and are included in the systematic uncertainty budget.
55 Cancri A Model Parameters
| Parameter | Symbol | Value | Uncertainty | Source |
|---|---|---|---|---|
| Effective temperature | Teff | 5196 K | ± 24 K | CHARA interferometry — von Braun et al. 2011, ApJ 740, 49 |
| Surface gravity | log g | 4.41 | ± 0.02 | CHARA interferometry — von Braun et al. 2011 |
| Metallicity | [Fe/H] | +0.32 | ± 0.02 | Spectroscopic self-consistency (§4) |
| Microturbulence | ξ | ~0.9 km/s | ± 0.1 km/s | Fe I EW self-consistency (§4) |
Section 03
Atomic Data: Line List
All atomic line data are loaded from external, version-controlled CSV files. No wavelengths or log gf values are hardcoded in pipeline software — ensuring full traceability.
VALD3 Query Settings
| Setting | Value | Notes |
|---|---|---|
| Query type | Extract Stellar | Filters by predicted line depth for given stellar parameters |
| Wavelength range | 3780 – 6910 Å | Matches HARPS coverage |
| Depth threshold | ≥ 1% of continuum | Removes lines too weak to measure |
| Access method | FTP (required) | HTTP truncates large requests — use vald.astro.uu.se FTP |
| Format | Long format | Includes broadening parameters (γvdW) |
⚠ FTP Required for Full Line List
The VALD3 web interface truncates output for large requests. Queries covering the full HARPS range with 27 target elements require FTP access to retrieve the complete line list. Register at vald.astro.uu.se for a free academic FTP account.
NIST Quality Grades
| Grade | log gf Uncertainty | Usage Policy |
|---|---|---|
| A+ | < 1% | Full science use |
| A | < 3% | Full science use |
| B | < 10% | Science use, flagged in uncertainty budget |
| C | < 25% | Excluded from primary results |
| D | > 25% | Excluded entirely |
Target Element List — 27 Elements
| Priority | Element | Symbol | Group | Scientific Significance |
|---|---|---|---|---|
| 1 | Iron I | Fe I | Iron peak | [Fe/H] calibration, Teff constraint |
| 1 | Iron II | Fe II | Iron peak | log g constraint via ionization equilibrium |
| 1 | Carbon | C | CHNOPS | C/O ratio — carbon vs. oxygen-rich planet mineralogy |
| 1 | Oxygen | O | CHNOPS | C/O ratio; most abundant metal in rocky planets |
| 1 | Magnesium | Mg | Alpha | Mg/Si ratio — mantle mineralogy (olivine vs. pyroxene) |
| 1 | Silicon | Si | Alpha | Primary rocky planet building block |
| 1 | Calcium | Ca | Alpha | Alpha element tracer; strong optical lines |
| 1 | Titanium | Ti | Alpha | Galactic chemical evolution tracer; perovskite in mantles |
| 1 | Nickel | Ni | Iron peak | Rocky planet core composition; Fe/Ni ratio |
| 1 | Sodium | Na | Bio-significant | Biological tracer; Na D doublet |
| 1 | Phosphorus | P | CHNOPS | Limiting nutrient for life; varies 10× across FGK stars |
| 1 | Sulfur | S | CHNOPS/Alpha | Life-essential volatile; disk chemistry tracer |
| 2 | Nitrogen | N | CHNOPS | Life-essential; difficult optical lines |
| 2 | Cobalt | Co | Iron peak | Fe peak nucleosynthesis tracer |
| 2 | Chromium | Cr | Iron peak | Type Ia vs. Type II SNe tracer via Cr/Fe |
| 2 | Aluminum | Al | Rocky planet | Refractory element; crustal composition |
| 2 | Potassium | K | Bio-significant | Life-essential; difficult lines |
| 2 | Barium | Ba | s-process | AGB star enrichment history |
| 2 | Yttrium | Y | s-process | Stellar age chemical clock (Y/Mg ratio) |
| 2 | Vanadium | V | Iron peak | Enzyme cofactor; nucleosynthesis tracer |
| 2 | Copper | Cu | Iron peak | Odd-Z iron-peak tracer; bio-essential; Cu I 5105/5218 Å |
| 3 | Manganese | Mn | Iron peak | Odd-Z nucleosynthesis; metallicity-dependent |
| 3 | Scandium | Sc | Light iron peak | Odd-even nucleosynthesis effect |
| 3 | Lithium | Li | Age indicator | Stellar age constraint; depletes with time |
| 3 | Europium | Eu | r-process | Neutron star merger enrichment history |
| 3 | Zirconium | Zr | s-process | Refractory s-process tracer |
| 3 | Strontium | Sr | s-process | Light s-process anchor; completes Sr/Y/Ba/Zr picture |
Special Line Handling
| Line | Issue | Treatment |
|---|---|---|
| [O I] 6300.304 Å | Blended with Fe I + Ni I 6300.336 Å | Ni blend subtracted using measured Ni abundance; no NLTE correction (forbidden line) |
| O I 7771–7775 Å triplet | Large NLTE corrections (−0.2 to −0.4 dex) | Amarsi et al. (2021) grid; cross-checked against [O I] 6300 Å |
| Na I D 5890/5896 Å | Strong — damping wings + NLTE | Voigt profile fit; Lind et al. (2011) correction (~−0.07 dex) |
| P I 6034/6043 Å | Very weak — requires S/N > 300 | Only accessible in co-added spectrum; upper limit if < 3σ |
| C I 5380 Å | High χ (7.7 eV) — Teff sensitive | Cross-validated against C I 5052 Å; Amarsi et al. (2019) NLTE correction |
Section 04
Spectral Analysis
Before measuring elemental abundances, the spectrum is continuum-normalized and stellar parameters (Teff, log g, ξ) are verified through self-consistency checks on Fe I and Fe II lines.
Continuum Normalization
- 1Identify continuum anchor windows — regions free of significant absorption for the target's stellar parameters (Barklem & Aspelund-Johansson 2005).
- 2For metal-rich stars ([Fe/H] > +0.2), use the ATLAS9 model continuum as additional reference in crowded regions (5000–5400 Å).
- 3Fit a Chebyshev polynomial (degree 3) through anchor points with iterative 3σ sigma-clipping.
- 4Divide observed spectrum by the fitted continuum.
- 5Verify: σ < 0.005 (0.5% of continuum) in clean windows before proceeding.
Challenge for 55 Cancri A
At [Fe/H] = +0.32, the spectrum is significantly more crowded than solar. The 5000–5400 Å region has very high Fe I line density. The ATLAS9 model continuum is weighted more heavily here to avoid over-fitting through shallow absorption features.
Stellar Parameter Self-Consistency
| Parameter | Diagnostic | Convergence Criterion |
|---|---|---|
| Teff | Fe I abundance vs. excitation potential χ | |∂[Fe/H]/∂χ| < 0.01 dex/eV — requires ≥ 20 Fe I lines spanning χ = 0.5–5.0 eV |
| ξ (microturbulence) | Fe I abundance vs. reduced EW log(EW/λ) | |∂[Fe/H]/∂log(EW/λ)| < 0.01 dex per unit |
| log g | Ionization equilibrium: A(Fe I) vs. A(Fe II) | |A(Fe I) − A(Fe II)| < 0.05 dex |
All three constraints must be simultaneously satisfied. Convergence typically takes 3–5 iterations starting from interferometric values.
EW Measurement Quality Thresholds
| Criterion | Requirement | Action if Failed |
|---|---|---|
| EW minimum | > 5 mÅ | Below detection — report upper limit |
| EW maximum | < 300 mÅ | Saturated — exclude from LTE analysis |
| Fit quality (χ²red) | < 2.0 | Refit or exclude |
| Line S/N | > 5 | Exclude |
| Center shift | < 0.05 Å from VALD/NIST | Flag — possible misidentification |
Section 05
Line Profiles
The correct line profile model depends on line strength. Gaussian fits work well for weak lines; strong lines with pressure-broadened wings require Voigt profiles.
Gaussian vs. Lorentzian vs. Voigt
| Profile | Appropriate For | Physics | EW Rule |
|---|---|---|---|
| Gaussian | Weak lines EW < 80 mÅ | Thermal + instrumental broadening | ≈ Voigt (< 1% difference) in this regime |
| Lorentzian | Theoretical damping wings only | Pressure broadening (van der Waals) | Overestimates core depth — not used alone |
| Voigt | All line strengths | Gaussian core convolved with Lorentzian wings | Required for EW > 150 mÅ |
Always fitted with Voigt profiles: Na D doublet, Mg b triplet (5167–5184 Å), Ba II 5853 Å, Ca H&K (3934/3968 Å).
Worked Example: Na I D1 (5895.92 Å)
The Na I D doublet was first observed in the Sun by Fraunhofer (1814) and identified as sodium by Kirchhoff & Bunsen (1859). For 55 Cnc A ([Fe/H] = +0.32), the lines are especially deep due to enhanced sodium abundance.
- 1Locate: Extract ±5 Å around 5895.92 Å after RV correction. D1 and D2 are separated by ~6 Å, well-resolved at R~115,000.
- 2Choose profile: Na D EW ~ 450–550 mÅ → damping regime → Voigt required. Gaussian would underestimate EW by ~25%, causing ~0.2 dex error in [Na/H] — larger than the entire uncertainty budget.
- 3Measure EW: Numerical integration over fitted Voigt profile. EW = ∫(1 − F(λ)/Fc) dλ, expressed in mÅ.
- 4Uncertainty: Primary limit is continuum placement, not photon noise. σEW ≈ σcont × window × 1000 ≈ 0.005 × 6.0 × 1000 ≈ 30 mÅ (~6% relative).
- 5Atomic data: λ = 5895.924 Å (NIST A+), χ = 0.000 eV (ground state), log gf = −0.184 (NIST A), γvdW = −7.530 (Barklem 2000). Input to iSpec/Turbospectrum.
- 6NLTE correction: −0.07 ± 0.02 dex (Lind et al. 2011) for these parameters. Expected result: [Na/H] ≈ +0.34 to +0.44, [Na/Fe] ≈ +0.02 to +0.12 (near-solar ratio).
Section 06
Abundance Derivation
From equivalent width to photospheric abundance — via the curve of growth, iSpec/Turbospectrum radiative transfer, and solar normalization to Asplund et al. (2021).
The Curve of Growth
| Regime | EW Range | Behavior | Notes |
|---|---|---|---|
| Linear | < ~50 mÅ | EW ∝ N (number of absorbing atoms) | Direct proportionality — preferred |
| Flat (saturation) | ~50–150 mÅ | EW grows slowly with abundance | Sensitive to microturbulence ξ |
| Damping | > ~150 mÅ | EW ∝ √N (pressure-broadened wings) | Requires accurate γvdW; Voigt fit only |
Solar Normalization
Schmitt (2010) — Predecessor Study
Solar reference: Lodders (2003)
A(Fe)☉ = 7.50
Instrument: ELODIE (R ~ 42,000)
The Exoplanet Codex (2026)
Solar reference: Asplund et al. (2021)
A(Fe)☉ = 7.46 (−0.04 dex revision)
Instrument: HARPS (R ~ 115,000)
Key Science Ratios
| Ratio | Threshold | Interpretation | Solar Value |
|---|---|---|---|
| C/O | 0.8 | Below: silicate/oxide minerals (Earth-like). Above: SiC, graphite — possible diamond interior | 0.55 |
| Mg/Si | 1.0 | Above: olivine-dominated mantle (Mg₂SiO₄). Below: pyroxene-dominated (MgSiO₃) | 1.05 |
| Fe/Si | — | Iron core mass fraction predictor for rocky planets | 0.86 (mass) |
| [α/Fe] | — | High at low [Fe/H] = old star formed before Type Ia SNe Fe enrichment | ~0.0 |
| CHNOPS Index | vs. Redfield ratio | C:N:O:P:S ratios vs. marine organism composition — habitability indicator | 1.0 (reference) |
Section 07
Uncertainty Analysis
The uncertainty budget follows the Type A / Type B framework of the JCGM Guide to the Expression of Uncertainty in Measurement (GUM) — consistent with precision metrology practice.
Type A — Statistical (Random)
| Source | Estimation Method | Typical Magnitude |
|---|---|---|
| Photon noise on EW | Covariance matrix of Gaussian/Voigt fit | σEW ≈ 1.5 × FWHM / S/N |
| Line-to-line scatter | σ / √N for N lines of same element | ~0.02 – 0.05 dex |
| Continuum placement | Repeat normalization, vary anchor points | ~0.01 – 0.03 dex |
Type B — Systematic (Non-Random)
| Source | Estimation Method | Typical Magnitude |
|---|---|---|
| ΔTeff = ±50 K | Re-run abundances at Teff ± 50 K | ±0.05 – 0.10 dex |
| Δlog g = ±0.1 | Re-run at log g ± 0.1 | ±0.02 – 0.05 dex |
| Δξ = ±0.1 km/s | Re-run at ξ ± 0.1 | ±0.03 – 0.06 dex |
| log gf uncertainty | NIST grade (A: 3%, B: 10%) | ~0.02 – 0.05 dex |
| NLTE corrections | Uncertainty on correction grids | ~0.02 – 0.08 dex |
| 1D vs. 3D models | Compare ATLAS9 vs. MARCS | ~0.03 – 0.10 dex (C, O) |
| Continuum (systematic) | Model-based vs. polynomial normalization | ~0.02 – 0.05 dex |
O I / Ni I Blend at 6300 Å
The dominant source of published C/O ratio discrepancies for 55 Cnc A (Teske et al. 2013). The Ni I 6300.336 Å contribution is calculated from our measured Ni abundance and subtracted. Its uncertainty propagates into σ(C/O) as a correlated term.
Section 08
Data Model
The pipeline processes each star from raw ESO archive FITS files to final abundance tables through six sequential stages, each with well-defined input and output schemas.
Multi-Target Dataset Summary
| Target | HARPS S1D | HST Observations | HST Gratings | Program / PI |
|---|---|---|---|---|
| Solar (calibrator) | 10 spectra | — | — | ESO 1102.D-0954(A) · PI: Dumusque (U. Geneva) · Direct solar feed, SNR 306–309 |
| 55 Cancri A | 88 spectra | STIS | G140M, G750L, G430L, E230M | Multiple programs · MAST archive |
| Alpha Centauri A | 75 spectra | 111 observations | E140H, E140M, E230H, E230M | Multiple programs · MAST archive |
Solar Dataset Note
The solar spectra are direct solar feed observations — the Sun itself, not asteroid-reflected sunlight. ESO Program 1102.D-0954(A), PI Xavier Dumusque (University of Geneva). The high SNR (306–309 per exposure) allows validation of weak lines including P I 6034 Å and Li I 6707 Å before touching science targets.
Pipeline Data Flow
Key File Schemas
Future Integrations
| Integration | Purpose | Status |
|---|---|---|
| JWST atmospheric spectra | Cross-correlate host star abundances with exoplanet atmospheric composition | Planned — Milestone C |
| Hypatia Catalog | Automated ingestion for literature comparison per star | Planned — Milestone C |
| NASA Exoplanet Archive API | Live planet parameter cross-matching | In design |
Section 09
Solar Validation
Before analyzing any exoplanet host star, the pipeline is validated against the Sun using 10 direct solar HARPS S1D spectra (ESO 1102.D-0954(A), PI: Dumusque) — processed identically to the science targets.
Solar Calibration Criteria
| Quantity | Required Result | If Failed |
|---|---|---|
| A(Fe)☉ recovery | 7.46 ± 0.05 (Asplund et al. 2021) | Systematic pipeline error — must identify and correct before any science results |
| C/O☉ recovery | 0.55 ± 0.05 | Systematic oxygen measurement error |
| Dataset | 10 HARPS S1D, direct solar feed · SNR 306–309 per exposure | — |
Literature Comparison for 55 Cancri A
| Reference | Method | Key Result |
|---|---|---|
| Fischer & Valenti (2005) | HIRES/Keck spectral synthesis | [Fe/H] = +0.33 ± 0.04 |
| Valenti & Fischer (2005) | Spectral synthesis (SME) | Full atmospheric parameters |
| Teske et al. (2013) | EW method — dedicated C/O study | C/O = 0.78 ± 0.08 (ApJ 778, 132) |
| Hypatia Catalog (HIP 43587) | Weighted mean of all literature values | Reference for systematic offsets |
Section 10
References
| Amarsi et al. (2019) | A&A 630, A104 — Carbon NLTE corrections |
| Amarsi et al. (2021) | A&A 656, A113 — Oxygen NLTE corrections |
| Amarsi et al. (2022) | A&A 668, A68 — Iron NLTE corrections |
| Asplund et al. (2021) | A&A 653, A141 — Solar photospheric abundances (current standard) |
| Barklem & Aspelund-Johansson (2005) | A&A 435, 373 — Van der Waals damping constants |
| Blackwell et al. (1979) | MNRAS 186, 657 — Microturbulence / equivalent width method |
| Blanco-Cuaresma et al. (2014) | A&A 569, A111 — iSpec spectral analysis framework |
| Castelli & Kurucz (2003) | Proc. IAU Symp. 210 — ATLAS9 model atmosphere grid |
| Fischer & Valenti (2005) | ApJ 622, 1102 — 55 Cnc A parameters, [Fe/H] = +0.33 |
| Gustafsson et al. (2008) | A&A 486, 951 — MARCS model atmosphere grid |
| Kramida et al. (2023) | NIST Atomic Spectra Database — physics.nist.gov/asd |
| Lind et al. (2011) | A&A 528, A103 — Sodium NLTE corrections |
| Lodders (2003) | ApJ 591, 1220 — Solar abundances (used in Schmitt 2010) |
| Osorio et al. (2015) | A&A 579, A53 — Magnesium NLTE corrections |
| Ryabchikova et al. (2015) | PhyS 90, 054005 — VALD3 atomic line database |
| Schmitt (2010) | Senior Thesis, University of Montana — predecessor 55 Cnc abundance study |
| Plez (2012) | Turbospectrum: Code for spectral synthesis — radiative transfer, native molecular lines |
| Gerber et al. (2023) | A&A 669, A43 — Turbospectrum NLTE radiative transfer |
| Teske et al. (2013) | ApJ 778, 132 — 55 Cnc C/O ratio (dedicated study) |
| Valenti & Fischer (2005) | ApJS 159, 141 — Spectral synthesis method (SME) |
| von Braun et al. (2011) | ApJ 740, 49 — 55 Cnc A interferometric parameters (CHARA) |
Version 1.2 · May 2026 · github.com/damienabraxas/exoplanetcodex