Analysis workflows
These chapters walk through end-to-end μSR data analyses and demonstrate the Asymmetry GUI and Python API in lock-step. Almost all are reproducible walkthroughs on real instrument runs from the WiMDA muon-school corpus — several on the very datasets behind published papers — each with the model, seeds, and expected numbers; the Knight-shift chapter (and a few illustrative subsections) use synthetic versions of canonical experiments grounded in textbook archetypes (Blundell et al. 2022; Amato & Morenzoni 2024).
The narratives are the recommended onboarding path for users who have collected real data and want to see how to analyse it. They cross-reference the reference pages elsewhere in this user guide for full feature documentation.
New users should start with EMU detector grouping and α calibration.
- EMU detector grouping and α calibration
- The runs
- Step 1 — Load a run
- Step 2 — Open the Grouping window
- Step 3 — Calibrate α from the TF run
- Step 4 — The visual Detector Layout Editor
- Step 5 — Dead-time correction
- Step 6 — Timing: t0 and the good-data window
- Step 7 — A fit table with a manual column
- Reusing the calibration
- Where to go next
- Muon diffusion in copper: Kubo–Toyabe, Abragam, and QLCR
- The experiment and the corpus data
- The static Kubo–Toyabe signature
- Low-temperature quantum diffusion
- The dynamic Kubo–Toyabe fit and the hop rate
- The hop-rate curve and the mobility minimum
- Cross-check: the transverse-field Abragam line shape
- Quadrupolar level-crossing resonance (QLCR)
- Assumptions and limitations
- References
- Cross-references
- Photo-μSR in silicon: carrier recombination from period-mode runs
- ALC field scan in TCNQ
- Temperature scan through a magnetic transition
- Global fitting across fields: Li⁺ ionic motion in a garnet electrolyte
- Why a global fit is unavoidable here
- The runs
- Step 1 — Calibrate α from the TF run
- Step 2 — Read the raw field triplet
- Step 3 — The model and the parameter classification
- Step 4 — Run the joint fit
- Step 5 — Trend ν(T) and extract the activation energy
- Assumptions and limitations
- References
- Cross-references
- F–µ–F entangled states: measuring a bond length with muons
- Why PTFE hosts an entangled three-spin state
- The runs
- Step 1 — Calibrate α on the transverse-field run
- Step 2 — Read the raw zero-field signature
- Step 3 — Fit the F–µ–F polarisation and read off the bond length
- Step 4 — The frequency-domain view
- Assumptions and limitations
- References
- Cross-references
- Angle-dependent Knight shift
- Superconductor penetration depth from σ(T)
- Physical motivation
- The data
- Step 1 — Fit a TF run for σ
- Step 2 — Inspect the vortex line shape
- Step 3 — Trend σ(T) through T_c
- Step 4 — Compare the two fields
- Fitting a gap model
- Cross-reference — LiFeAs, the field width B_rms(T)
- Cross-reference — Re₆Zr, superfluid density and a TRSB step
- Interpretation
- Assumptions and limitations
- References
- Cross-references
- LF decoupling and static-vs-dynamic field distributions
- Physical motivation
- The data
- Step 1 — Load and overlay the decoupling series
- Step 2 — Fit each run with a single exponential
- Step 3 — Build the λ(B) trend
- Step 4 — The Redfield linearisation (headline)
- Contrast: the static counter-example
- The static LF-KT decoupling series
- Interpretation
- Common pitfalls
- Further reading
- Cross-references
Quick chooser
Workflow |
Typical experiment |
Key Asymmetry features |
|---|---|---|
Set up EMU detector grouping and calibrate α from a TF run (onboarding) |
Grouping window, Estimate α, visual Detector Layout Editor, dead-time |
|
Measure the muon hop rate ν in copper from a ZF dynamic-KT fit |
DynamicGaussianKT, fixed Δ / floated ν, motional narrowing |
|
Photo-μSR in silicon: carrier recombination from period-mode runs |
Compare light-ON vs light-OFF muonium dynamics in a photo-μSR run |
Red/green RG box, |
Locate an ALC resonance from a field-stepped scan |
ALC mode, Build Scan, baseline + peak fit, integral asymmetry |
|
Locate Tc and measure the order parameter of a ferromagnet or antiferromagnet (real EuO / Ni / molecular-magnet data) |
Logbook sort, Fit Wizard, parameter trending, power-law fit |
|
Global fitting across fields: Li⁺ ionic motion in a garnet electrolyte |
Extract an ion-hopping activation energy from LF triplets in a solid electrolyte (real Li₇La₃Zr₂O₁₂ data) |
Global (batch) fit with shared parameters, Keren model, axis transforms, Arrhenius trend |
Identify an F–µ–F entangled state and measure the muon–fluorine bond length (real PTFE data) |
FmuF models, ZF beating signature, sub-MHz FFT |
|
Find the muon site from the angle dependence of the Knight shift in a rotated single crystal |
Knight shift analysis window, Angle axis + Fold, Joint K(θ) fit, KnightAnisotropy, Suggest next angle |
|
Extract λ(T) from TF μSR in the vortex state of a superconductor (real BiSCCO / LiFeAs / Re₆Zr data) |
Multi-run TF fits, parameter trending, multi-series overlay, MaxEnt vortex lineshape, SC gap models |
|
Distinguish static from dynamic local fields with an LF scan (real Ca₃Co₂O₆ data) |
LF exponential fits, axis transforms (1/λ vs B² Redfield), static-KT decoupling diagnostic |
Further workflows
The internal porting workspace
(docs/porting/practical-workflows/workflow-catalogue.md)
catalogues additional workflows that Asymmetry partially or
fully supports — F–μ–F identification, spin-glass freezing,
muonium-radical hyperfine, and others.
ALC resonance scans have a worked example above
(ALC field scan in TCNQ) and a full feature reference in
Integral scan mode (avoided-level-crossing field scans); the angle-dependent Knight shift has a
worked example above (Angle-dependent Knight shift) and a feature
reference at Knight shift. Workflows that Asymmetry does not
yet support (e.g. multi-period arithmetic, LEM depth profiling) are
catalogued there too and surface as candidates in
docs/porting/ROADMAP.md.