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SCIENCE · INVESTIGATE AND EXPLAIN

Correct an instrument offset with separate evidence

Use independent standards to restore a wavelength comparison without changing raw observations.

Learning outcome: Calculate a shared additive correction and reject a one-offset calibration when standards disagree.

Starting recap

Corrected center equals raw center minus the independently measured offset. Provisional zero offset is not verified calibration.

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Try

D’s standards both read 2 nm high, so raw 390.90 and 488.13 nm correct to 388.90 and 486.13 nm.

Open the experiment

Predict

Can a mismatch be repaired by assuming the sample identity and shifting it until it fits?

Experiment

Follow D through all stages; compute both standard offsets, corrected feature centers and corrected coverage while retaining raw values.

Compare spectral features and independent calibration

Fictional spectrum records · selected atomic reference comparisons · Seven fictional supplied records compared with eight selected NIST air-wavelength values for neutral H, He and Na. Inclusive +/-0.10 nm is a teaching compatibility tolerance, not a source uncertainty or line width. Every revealed feature must map to a distinct selected transition of one species. Unreported lines never imply absence. Before calibration, zero offset is provisional. No measured stellar spectrum, abundance analysis, temperature inference, Doppler fitting or complete catalogue is supplied.

Reset keeps your prediction, captures and practice history.

A: emission pattern: emission. These are fictional supplied feature positions. Reference markers are selected neutral-atom transitions, not a complete list of lines. Roman numeral I means neutral.

Provisional comparison: calibration not yet supplied. Applied subtraction: 0.00 nm. Raw observations stay unchanged as evidence is revealed.

Air wavelength (nm) · feature positions, not intensity380400450500550600650690Raw recordCorrected recordH I referencesHe I referencesNa I referencesTinted record spans: coverage. Outside each span: unavailable, not zero light.
Detail: 388.4–389.4 nm · same fixed scale for every caseCorrected featuresH I referenceHe I reference388.4388.6388.8389.0389.2389.4Features outside this window are not moved into the inset.

The ±0.10 nm matching tolerance is stipulated for this exercise. It is not a confidence interval, NIST uncertainty, line width or instrument resolution. No line strengths are measured here.

Supplied features and independent correction (nm in air)
FeatureRaw centerCorrected centerAvailability
1388.90000388.90000Supplied
2Not yet revealedNot yet revealedRecorded, unrevealed

1 revealed feature(s). Raw coverage: 380.00–680.00 nm. Corrected coverage: 380.00–680.00 nm. An unreported reference line is not negative evidence, even inside the covered interval. A narrow record cannot supply a second feature merely because a later evidence stage is selected.

Can ONE listed species explain every revealed feature using distinct selected transitions?
SpeciesResultFirst compatible assignment: feature → reference; signed residual
H ICompatible within this library

1 → h-388 (388.90490 nm); -0.00490 nm

He ICompatible within this library

1 → he-388 (388.86489 nm); 0.03511 nm

Na INo complete assignmentNo assignment claimed.

Several listed patterns remain compatible. More discriminating observed features are needed.

A match is conditional support within this selected-line, single-species comparison. It does not establish abundance, stellar temperature or complete composition. Failure may reflect a mixture, omitted transitions, motion or calibration; it does not prove an element absent.

Inspect the independent calibration record

Not yet supplied. Select the calibration evidence stage. Zero subtraction at earlier stages is provisional, not evidence of a calibrated instrument.

Compare schematic spectrum types

These drawings show patterns, not measured heights or a model of a stellar atmosphere. All three use the same schematic horizontal wavelength direction.

Schematic only · wavelength increases to the rightContinuousEmissionAbsorption

A hot dense source can supply a continuum; excited low-density gas can supply emission lines; cooler gas along the view of a continuum source can produce absorption features. The corresponding transition positions may coincide while strengths depend on physical conditions. A dark line is reduced light at selected wavelengths, not no light everywhere.

Inspect selected reference wavelengths and sources
Selected NIST air wavelengths; source angstroms divided by ten
ID / speciesSource Ånm in airSource row
h-388 / H I3889.049388.90490RCWM80
h-434 / H I4340.462434.04620MK00a
h-486 / H I4861.2786486.12786MK00a
he-388 / He I3888.6489388.86489M02
he-447 / He I4471.479447.14790M60a
he-587 / He I5875.6148587.56148M02
na-588 / Na I5889.950588.99500R56
na-589 / Na I5895.924589.59240R56

Selected factual values from J. E. Sansonetti and W. C. Martin, NIST Handbook of Basic Atomic Spectroscopic Data, SRD 108, accessed 26 October 2026. These are selected multiplet components, not intensity-weighted centroids. Source intensities and database tables are not reproduced. NIST distinguishes Standard Reference Data licensing from ordinary federal works; no public-domain or CC license is asserted for the compilation. NIST accuracy disclaimer. Synthetic records and diagrams are authored teaching material.

Scientific context: NASA introduction to spectra and NASA on stellar composition and temperature. This comparison is not a stellar-atmosphere simulation.

2 compatible listed patterns: H I, He I.

Calibration is not yet revealed; this is a provisional zero-offset comparison. Several listed patterns remain compatible. More discriminating observed features are needed.

Captures preserve the supplied spectrum record and evidence stage. Replaying compares fictional feature positions with selected reference transitions; it is not a new measurement, complete stellar classification or abundance analysis.

Understand

Distinguish a sample mismatch from an instrument offset

Select record D and inspect its first raw center, 390.90 nm. Under the provisional zero-offset comparison it does not match a selected reference within ±0.10 nm. Reveal all features: the second raw center, 488.13 nm, also leaves no compatible single-species explanation in the selected reference set.

Do not fix the mismatch by assuming the sample must be hydrogen and shifting the observations until that identity fits. That would use the desired conclusion as the calibration evidence. Instead, reveal the independent instrument check in the final evidence stage.

The supplied calibration standards have stipulated true positions 500.00 and 600.00 nm. The instrument records them at 502.00 and 602.00 nm for D. These fictional standards are instrument checks, not additional atomic transitions claimed from a source database.

Calculate the correction from both standards

For each standard, compute recorded minus stipulated position. The first gives 502.00 − 500.00 = +2.00 nm; the second gives 602.00 − 600.00 = +2.00 nm. Both support the same additive instrument offset in this teaching model.

Corrected wavelength equals raw wavelength minus the offset. Thus D’s centers become 390.90 − 2.00 = 388.90 nm and 488.13 − 2.00 = 486.13 nm. The raw values remain in the ledger. A correction adds an interpretation layer; it does not rewrite the instrument record as though it originally read the corrected value.

Compare the corrected pair with the selected H I references 388.9049 and 486.12786 nm. Their residuals are −0.00490 and +0.00214 nm. The independently supported correction restores hydrogen compatibility under the selected-line hypothesis. NIST hydrogen air-wavelength table.

Correct the coverage along with the features

D’s raw covered interval is 382–682 nm. Subtracting the same +2 nm offset gives a corrected interval of 380–680 nm. Correcting the markers but leaving the axis coverage in the raw coordinate system would mix two wavelength scales.

Draw two aligned paper axes: raw above and corrected below. Mark both features, both interval endpoints and the calibration standards. Label the displacement as an instrument correction. The first raw feature is outside the narrow 388.4–389.4 nm detail inset; it should not be squeezed into that inset merely to make the comparison look closer.

Before the calibration stage, the display’s zero-offset calculation is provisional. “Unknown calibration” does not mean “calibration verified to be zero.” After the calibration stage, the stipulated offset is known within this exercise. That change in evidence can restore candidates, so candidate elimination need not be monotonic across all stages.

Keep instrumental and astrophysical explanations separate

An instrument offset and a physical shift of source wavelengths are different hypotheses. This exercise establishes an additive correction from standards independently of the unknown sample. It does not calculate a radial velocity or establish that the source is stationary in every physical sense.

A common additive displacement is not automatically an astrophysical Doppler shift. Motion-related interpretations require an appropriate wavelength relation and independently controlled instrumental effects. The browser contains no such velocity analysis. Its reference values also use air wavelengths consistently; changing conventions would be another source of mismatch to investigate, not evidence of motion by itself.

Real calibration has uncertainty and may require a correction that varies with wavelength. Here both standards must imply the same offset, treated as exact for the authored example. The ±0.10 nm feature tolerance is separate from that calibration assumption and from NIST’s reference uncertainties. The NIST handbook supplies selected reference facts, not a guarantee about this fictional instrument.

Transfer to inconsistent standards

A new instrument records the 500.00 nm standard at 502.00 nm and the 600.00 nm standard at 603.00 nm. A learner proposes subtracting their average offset, 2.50 nm, and calling the record calibrated under this model. Is that justified?

Check the spectrum-calibration transfer

No. The implied offsets are +2.00 and +3.00 nm, so one additive offset cannot explain both standards under the stipulated exact-check assumptions. Investigate the calibration model, standards or instrument behavior. Averaging does not make the current one-offset model adequate.

Apply

What supports applying the +2 nm instrument correction in D?

Public practice checks a specific claim. It does not establish independent mastery.

Distinguish independent calibration from identity-driven adjustment and from an unsupported Doppler interpretation.

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

Skipping retains experiments and awards no mastery.

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