Modular toolkit for electrochemical impedance spectroscopy (EIS) analysis with Distribution of Relaxation Times (DRT) support.
Key features:
- Reproducibility - Objective, data-driven parameter selection
- Modularity - Usable as CLI and Python library
- Advanced optimization - Multi-start, Differential Evolution
Example output:
Supported data formats:
- Gamry DTA - native format (automatic metadata parsing, ZCURVE block)
- CSV - three columns with a header row, e.g.
frequency,Z_real,Z_imag- Column names are matched case-insensitively against: frequency -
freq,frequency,f,hz; real part -zreal,z_real,z',re(z),real,z.real,re; imaginary part -zimag,z_imag,z'',im(z),imag,z.imag,im - If no name matches, the first three columns are used positionally (with a warning)
- Delimiter: comma, semicolon, or tab (auto-detection)
- Decimal format: US (dot) and European (comma for semicolon-delimited)
- Comments: lines starting with
#are ignored - Examples: example/example_eis_data.csv
- Column names are matched case-insensitively against: frequency -
Changelog: CHANGELOG.md
Requires Python 3.9 or newer.
git clone https://github.com/chmelat/eis_analysis
cd eis_analysis
pip install -e .After installation, the eis command is available system-wide.
Windows users: Python and Git are not preinstalled on Windows - see the step-by-step guide in Installation on Windows.
For alternative installation methods, see Installation options.
# Basic analysis (KK + Z-HIT validation + DRT)
eis data.DTA
# With circuit fitting
eis data.DTA --circuit "R(100) - (R(5000) | C(1e-6))"
# Save plots to files
eis data.DTA --save results --format pdfRun eis --help for all options.
# KK + Z-HIT validation + DRT analysis (default)
eis data.DTAOutput: Kramers-Kronig residuals, mu metric, Z-HIT reconstruction, DRT spectrum with detected peaks.
# Fit equivalent circuit
eis data.DTA --circuit "R(100) - (R(5000) | C(1e-6))"
# Use Differential Evolution for global optimization (default)
eis data.DTA --circuit "R(100) - (R(5000) | Q(1e-6, 0.9))"
# Use multi-start for local optimization
eis data.DTA --circuit "..." --optimizer multistart --multistart 20Repeat --circuit to fit several candidates on the same data and rank them
by information criteria:
eis data.DTA \
--circuit "R(100) - (R(5000) | C(1e-6))" \
--circuit "R(100) - (R(5000) | Q(1e-6, 0.9))" \
--circuit "R(100) - (R(5000) | Q(1e-6, 0.9)) - (R(100) | C(1e-5))"Circuit comparison (n = 160 residuals, weighting = modulus)
rank -c Circuit k err% dAIC dBIC cond
1 1 R(10)-(R(200)|C(2e-5)) 3 2.38 2.4 0.0 1.2e+00
2 3 R(10)-(R(150)|C(2e-5))-(R(50)|C(1e-6)) 5 2.33 0.0 3.7 1.3e+08
3 2 R(10)-(R(200)|Q(2e-5,0.9)) 4 2.38 4.4 5.1 6.0e+01
dAIC/dBIC < 2: indistinguishable, 4-7: noticeable, > 10: decisive
Selected by BIC: R(10)-(R(200)|C(2e-5)) (candidate 1)
Adding an element almost always lowers the residual, so the fit error alone
cannot tell a real improvement from fitting the noise. AIC and BIC charge for
each free parameter k and answer the question the error cannot: does the
data support the extra element?
Only differences are meaningful - below 2 the models are indistinguishable,
4-7 is a noticeable difference, above 10 is decisive. BIC charges ln(n) per
parameter against AIC's 2, so it penalizes complexity roughly 2.5x harder and
is what selects the reported winner. The example above is the case they
disagree on: the two-branch circuit has the lowest residual and wins on AIC,
but BIC rejects the extra branch - and its condition number, eight orders
higher, shows why. The ! flag marks cond > 1e10, where the covariance is
numerically unusable; below it, read the column anyway.
rank orders by BIC; -c is the position on the command line, which is also
the number the figures are saved under (<prefix>_fit_1, _fit_2, ...).
Values are comparable only within one run: change the weighting or the frequency range between candidates and the comparison is meaningless.
The BIC winner is what --analyze-oxide receives, and which circuit that was
is written to the log. A candidate that fails to fit is reported in the table
and skipped rather than ending the run.
Detailed documentation: doc/MODEL_SELECTION_AIC_BIC.md
- what the criteria measure, a worked example of the arithmetic, and what they cannot tell you.
# Automatic Voigt chain fitting
eis data.DTA --voigt-chain
# With automatic element count optimization
eis data.DTA --voigt-chain --voigt-auto-M# Thickness calculation from capacitance
eis data.DTA --circuit "R(100) - (R(5000) | C(1e-6))" --analyze-oxide
# With custom parameters
eis data.DTA --circuit "..." --analyze-oxide --epsilon-r 22 --area 0.5
# Inverse: permittivity from a known thickness (SEM/TEM)
eis data.DTA --circuit "..." --analyze-oxide --thickness 25# Process multiple files without interactive display
for f in *.DTA; do
eis "$f" --save "${f%.DTA}" --no-show
doneData quality verification using Lin-KK test. Validates causality, linearity, and stability of measured data.
# Default (included in standard analysis)
eis data.DTA
# Skip KK validation
eis data.DTA --no-kk
# Custom mu threshold
eis data.DTA --mu-threshold 0.80Detailed documentation: doc/LinKK_analysis.md
Non-parametric K-K validation using Hilbert transform. Runs by default alongside Lin-KK. Faster and provides complementary assessment.
# Both Lin-KK and Z-HIT run by default
eis data.DTA
# Disable Z-HIT (use only Lin-KK)
eis data.DTA --no-zhit
# Disable Lin-KK (use only Z-HIT)
eis data.DTA --no-kkDetailed documentation: doc/ZHIT_IMPLEMENTATION_SPEC.md
Distribution of Relaxation Times - model-free method for impedance data analysis. The regularization parameter is selected automatically by a hybrid search: GCV (Generalized Cross-Validation) gives a first estimate, and an L-curve search over +-1.5 decades around it picks the final lambda - GCV assumes a linear solution, which the non-negativity constraint of the DRT violates.
New to DRT? Start with the intuitive introduction: doc/DRT_INTUITION.md.
# Default DRT with auto-lambda
eis data.DTA
# Manual lambda selection
eis data.DTA --lambda 1e-3
# GMM peak detection (more robust)
eis data.DTA --peak-method gmm
# R_inf from the highest frequency decade instead of the HF median
eis data.DTA --ri-fitBy default R_inf is the median of Re(Z) over the (up to 5) highest-frequency
points, which assumes the spectrum has already flattened onto the real axis at
f_max. Use --ri-fit when it has not.
Detailed documentation: doc/GCV_IMPLEMENTATION.md, doc/GMM_PEAK_DETECTION.md, doc/RINF_ESTIMATION.md
Elegant operator overloading syntax for circuit definition.
Supported elements:
| Element | Description | Example |
|---|---|---|
R(value) |
Resistor | R(100) |
C(value) |
Capacitor | C(1e-6) |
L(value) |
Inductor | L(1e-6) |
Q(Q, n) |
Constant Phase Element (CPE) | Q(1e-4, 0.8) |
W(sigma) |
Warburg (semi-infinite) | W(50) |
Wo(R_W, tau) |
Warburg (bounded) | Wo(100, 1.0) |
K(R, tau) |
Voigt with tau parametrization | K(1000, 1e-4) |
G(sigma, tau) |
Gerischer (reaction-diffusion) | G(100, 1e-3) |
CC(C_inf, dC, tau, alpha) |
Cole-Cole dielectric relaxation | CC(1e-8, 1e-7, 1e-3, 0.2) |
Values in parentheses serve as initial guesses for the nonlinear fitting algorithm.
Values in quotes (e.g., R("100")) are treated as fixed constants and will not be fitted.
Operators:
| Operator | Meaning | Example |
|---|---|---|
- |
Series connection | R(100) - C(1e-6) |
| |
Parallel connection | R(1000) | C(1e-6) |
Operator precedence: - has HIGHER precedence than | (Python rules).
Always use parentheses around parallel combinations: (R|C).
# Voigt element
eis data.DTA --circuit "R(100) - (R(5000) | C(1e-6))"
# Randles circuit with CPE
eis data.DTA --circuit "R(10) - (R(100) | Q(1e-4, 0.8))"
# With fixed parameter
eis data.DTA --circuit 'R("0.86") - (R(2.4e9) | Q(1e-10, 0.823))'Detailed documentation: doc/CIRCUIT_PARSER.md, doc/K_ELEMENT_GUIDE.md, doc/WEIGHTING_AND_STATISTICS.md (weighting, fit error, standard errors and confidence intervals)
Automatic Voigt chain estimation using linear regression for initial guess, then nonlinear refinement.
# Basic Voigt chain
eis data.DTA --voigt-chain
# Automatic element count optimization
eis data.DTA --voigt-chain --voigt-auto-M
# Custom density (elements per decade)
eis data.DTA --voigt-chain --voigt-n-per-decade 5Detailed documentation: doc/VOIGT_CHAIN_MATH.md
Global optimization for finding global minimum.
# Default DE
eis data.DTA --circuit "R(100) - (R(5000) | C(1e-6))"
# Custom parameters
eis data.DTA --circuit "..." --de-strategy 2 --de-popsize 20 --de-maxiter 500DE strategies: 1=randtobest1bin (default), 2=best1bin, 3=rand1bin
Detailed documentation: doc/DIFFERENTIAL_EVOLUTION.md
Multiple starts from different initial points.
# Multi-start with 20 restarts
eis data.DTA --circuit "..." --optimizer multistart --multistart 20
# With larger perturbation
eis data.DTA --circuit "..." --optimizer multistart --multistart-scale 3.0Detailed documentation: doc/MULTISTART_OPTIMIZATION.md
Oxide layer thickness calculation from capacitance, or the inverse - relative permittivity from an independently known thickness.
# Automatic analysis
eis data.DTA --circuit "..." --analyze-oxide
# Custom permittivity and area
eis data.DTA --circuit "..." --analyze-oxide --epsilon-r 9 --area 0.5
# Inverse: thickness known from SEM/TEM, estimate permittivity
eis data.DTA --circuit "..." --analyze-oxide --thickness 25Common permittivities: ZrO2 ~ 22, Al2O3 ~ 9, TiO2 ~ 80, SiO2 ~ 3.9
The inverse direction is useful for cross-validation: if the estimated permittivity lands near the literature value for the expected oxide, the chosen equivalent circuit is physically consistent.
Detailed documentation: doc/OXIDE_ANALYSIS_GUIDE.md
-
input- Input file (.DTA or .csv). Without argument, synthetic data is used for testing. Built-in test circuit: Rs - (R0||Q0) - (R1||Q1) with 1% Gaussian noise:- Rs = 10 Ω (series resistance)
- R0 = 100 kΩ, Q0 = (1e-6 S·s^n, n=0.6)
- R1 = 800 kΩ, Q1 = (3e-5 S·s^n, n=0.43)
-
--f-min- Minimum frequency [Hz]. Data below this value will be cut off. Useful for removing noise at low frequencies. -
--f-max- Maximum frequency [Hz]. Data above this value will be cut off. Useful for removing artifacts at high frequencies.Both cuts apply to R_inf estimation, DRT and circuit fitting only. Kramers-Kronig and Z-HIT always run on the full measured spectrum: they are integral relations over all frequencies, so validating a truncated range produces spurious residuals.
--circuit,-c- Equivalent circuit for fitting. Syntax:-= series,|= parallel. Example:"R(100) - (R(5000) | C(1e-6))". Supported elements: R, C, L, Q, W, Wo, K, G, CC. Repeat the option to fit several candidates on the same data and rank them by AIC/BIC - see Comparing candidate circuits.--weighting(default: modulus) - Weighting type for fitting:uniform(w=1, all points equal),sqrt(w=1/sqrt|Z|, compromise),modulus(w=1/|Z|, balances relative errors),proportional(w=1/|Z|^2, emphasizes high-frequency). See doc/WEIGHTING_AND_STATISTICS.md for detailed guide.--no-fit- Skip circuit fitting.
--optimizer(default: de) - Optimizer type:de(Differential Evolution - global),multistart(multiple local fits), orsingle(one local fit).
Parameters whose bounds span many decades (R, C, Q, L) are searched as
log10(value), so the population spreads over the decades instead of being
drawn almost entirely from the top one; the exponents (n of the CPE and
alpha of the Cole-Cole element) stay linear.
If DE still ends far from the data and only the local refinement gets there,
the fit reports Global search contributed nothing - see
doc/DIFFERENTIAL_EVOLUTION.md section 7.3.
--de-strategy(default: 1) - DE strategy: 1=randtobest1bin (balanced, default), 2=best1bin (fast convergence), 3=rand1bin (more exploration).--de-popsize(default: 15) - Population size as multiple of parameter count. Higher = better exploration but slower.--de-maxiter(default: 1000) - Maximum number of generations. Increase if optimization doesn't converge.--de-tol(default: 0.01) - Convergence tolerance (relative fitness change).--de-workers(default: 1) - Number of parallel workers. -1 = all CPU cores.
--multistart N- Number of restarts for multi-start optimization (default: 16). Each restart starts from perturbed initial values. Implies--optimizer multistart; combining with another--optimizeris an error.--multistart-scale(default: 2.0) - Perturbation size in sigma units (standard deviation from covariance matrix). Higher = larger parameter space exploration.
--lambda,-l(default: auto GCV) - Regularization parameter for DRT. Without this parameter, automatic selection using GCV (Generalized Cross-Validation) and L-curve method is used. Higher values = smoother DRT, lower = more detail but also noise. Note: on low-noise data auto-lambda may drive lambda toward 0, giving a sparse/spiky DRT that is unreliable for peak-shape analysis; the tool reports the effective bin count (N_eff) and warns when the DRT is too sparse or lambda lands at the search-range edge — set--lambdamanually (e.g. 0.1) in that case.--n-tau,-n(default: 100) - Number of points on the tau time constant axis. Higher values give finer DRT resolution but increase computational cost.--normalize-rpol- Normalize gamma(tau) by polarization resistance so that integral = 1. Useful for comparing samples with different R_pol.--peak-method(default: scipy) - Peak detection method in DRT:scipy(fast, scipy.signal.find_peaks) orgmm(robust, weighted Gaussian Mixture Model fitted directly to gamma(tau)).--gmm-bic-threshold(default: 10.0) - BIC threshold for GMM peak detection. Lower values detect more peaks (2-5: sensitive, 10-20: conservative). Only used with--peak-method gmm.--lambda-probe- Peak stability diagnostics: re-solves the DRT at lambda10^(+-0.5) and lambda10^(+-1) around the selected lambda and tracks each detected peak across the solutions. Reports per-peak persistence, position drift (decades of tau), R variation, and a verdict (STABLE / MARGINAL / ARTIFACT). A peak that appears only in a narrow lambda window is likely a regularization artifact rather than a real relaxation process. The probe solutions are also drawn as thin overlay curves in the DRT plot. Example:eis data.DTA --lambda-probe.--ri-fit- Estimate R_inf from the highest frequency decade (f >= f_max/10) instead of the default median of the (up to 5) highest-frequency points. Handles both inductive and capacitive high-frequency ends: if Im(Z) changes sign inside the decade the real-axis intercept is interpolated at the crossing, purely capacitive data are extrapolated to Im=0 by a 2nd-degree polynomial in the Nyquist plane, and otherwise an R-L-K modelR_s + jwL + R_k/(1+jw*tau)is fitted by linear least squares. Use it when the spectrum has not yet flattened onto the real axis at f_max — an inductive tail from the cabling, or an arc that is not closed. The CLI prints the default median next to the result for comparison. See doc/RINF_ESTIMATION.md.--no-drt- Skip DRT analysis. Useful if you only want circuit fitting.
--no-kk- Skip Kramers-Kronig validation. KK test verifies causality, linearity, and stability of data.--mu-threshold(default: 0.85) - Stopping threshold of the Lin-KK M-iteration: elements are added until mu drops below this value. Lower values allow more Voigt elements (higher overfit tolerance). It controls the fit, not data quality - quality is judged by the residuals.--auto-extend/--no-auto-extend(default: on) - Automatically optimize extend_decades for KK validation (minimizes pseudo chi-squared). On by default to avoid tau-truncation bias that produces spurious imaginary-part residuals on data with strong capacitive/inductive tails. Use--no-auto-extendto disable.--extend-decades-max(default: 1.0) - Maximum extend_decades for--auto-extendsearch range.--kk-series-c- Include a series capacitance1/(jwC)in the Lin-KK model (Schonleberadd_cap). Use for blocking/capacitive low-frequency behavior (e.g. two-electrode cells, blocking oxides): a series C is KK-compliant but has zero real part, so the standard Voigt chain cannot represent it and imaginary residuals grow toward low frequencies while the real fit stays good. Off by default so results stay comparable with earlier analyses; the fitted C is printed in the KK summary.
--no-zhit- Disable Z-HIT validation (runs by default alongside Lin-KK).--zhit-optimize-offset- Use weighted least-squares offset optimization instead of fixed reference point.
Reads the per-point residuals of both validations above, so it belongs to neither.
-
--max-residual(default: 5.0) - Residual threshold for flagging an individual point as suspicious [%]. Applies to both KK and Z-HIT: once the validations have run (either one alone is enough), points whose relative deviation|Z - Z_fit| / |Z|exceeds this value in either method are listed with the frequency, both residuals, and which method flagged them. Each residual plot is then marked with the points its own method flagged - a band on the KK panel at a frequency KK considers fine would contradict theflagged bycolumn. The two methods are complementary - Lin-KK fits both impedance components and is sensitive to phase errors, Z-HIT reconstructs the magnitude from the phase and is sensitive to magnitude errors and drift. Nothing is removed or down-weighted; the list is diagnostic. Higher values = less sensitive.Two guards keep the list meaningful. A point must also exceed four times the median residual of that method, because a residual is the sum of the data error and the method's own reconstruction error, and Z-HIT's is the larger of the two (on measured spectra this changes nothing - the absolute threshold stays binding). And a method whose median residual already exceeds the threshold is skipped entirely - over half its points would be flagged, so the spectrum fails as a whole, which the
Data quality:line already reports. The median rather than the mean: a handful of genuine outliers pulls a mean over the threshold and would switch the report off exactly when it has something to say.Interpretation: an isolated point with good neighbours is usually a genuine defect (interference, contact, bubble). A systematic trend toward the lowest frequencies is usually sample drift - a real property of a non-stationary measurement, not a bad point, and deleting it hides the problem instead of fixing it.
--voigt-chain- Use automatic Voigt chain fitting. Linear regression for R_i and tau_i estimation, then nonlinear refinement.--voigt-n-per-decade(default: 3) - Number of time constants per decade for Voigt chain. Higher = finer coverage but more parameters.--voigt-extend-decades(default: 0.0) - Extend tau range by N decades beyond data limits. Useful if you expect processes outside measured range.--voigt-prune-threshold(default: 0.01) - Threshold for removing small R_i (as fraction of R_pol). Elements with R_i < threshold * R_pol are removed.--voigt-allow-negative- Allow negative R_i values (Lin-KK style). Otherwise negative elements are removed.--voigt-no-inductance- Do not include series inductance L in model.--voigt-fit-type(default: complex) - Fit type:complex(default, real+imag),real(real part only),imag(imaginary part only).--voigt-auto-M- Automatically optimize number of M elements using mu metric.--voigt-mu-threshold(default: 0.85) - Mu threshold value for--voigt-auto-M.--voigt-max-M(default: 50) - Maximum number of M elements for--voigt-auto-M.--no-voigt-info- Do not display detailed Voigt chain fitting info.
--analyze-oxide- Perform oxide layer analysis - thickness calculation from capacitance.--epsilon-r(default: 22.0) - Relative permittivity of oxide. Default 22 for ZrO2. Other oxides: Al2O3 ~ 9, TiO2 ~ 80, SiO2 ~ 3.9. Ignored (with a warning) when--thicknessis given.--thickness- Known oxide thickness [nm], e.g. from SEM/TEM. Reverses the analysis: the thickness becomes the input and the relative permittivity the estimated quantity.--area(default: from DTA metadata, else 1.0) - Electrode area [cm^2]. Required for correct thickness calculation. An explicit value always takes precedence over the DTA metadata.
--numeric-jacobian- Use numeric Jacobian instead of analytic. Analytic Jacobian is faster and more accurate but not available for all elements. Use this option for custom/non-standard elements.
--ocv- Display OCV (Open Circuit Voltage) curve if available in data.--save,-s- Save plots with this prefix.--save resultswritesresults_nyquist_bode,results_kk,results_zhit,results_drt,results_fitand, when the matching switch is given,results_ri_fit(--ri-fit) andresults_ocv(--ocv), each with the extension given by--format. Only the plots actually produced by the run are written.--format,-f(default: png) - Format of saved plots:png(raster),pdf/svg/eps(vector for publications).--no-show- Do not display plots interactively. Useful for batch processing with--save.-v,--verbose- Show debug messages on stderr (prefix[DEBUG]).-q,--quiet- Quiet mode - hide INFO messages, show only warnings and errors.--version- Print the version and exit.
Logging levels:
- INFO (default): stdout, no prefix
- WARNING: stdout, prefix
! - ERROR: stderr, prefix
!! - DEBUG (
-v): stderr, prefix[DEBUG]
For an isolated environment, we recommend using a virtual environment (venv). This prevents dependency conflicts with other projects and does not affect your system Python installation. If you prefer not to use venv, skip to the direct installation below.
With virtual environment (recommended):
Linux/macOS:
# Create virtual environment
python3 -m venv eis_env
# Activate environment
source eis_env/bin/activate
# Install (now in isolated environment)
git clone https://github.com/chmelat/eis_analysis
cd eis_analysis
pip install -e . # Editable install (for development)
# or
pip install . # Standard installWindows: see the dedicated step-by-step guide in Installation on Windows.
Without virtual environment (direct installation):
git clone https://github.com/chmelat/eis_analysis
cd eis_analysis
pip install -e . # Editable install (for development)
# or
pip install . # Standard installAfter installation, the eis command is available (in activated environment if using venv):
eis --help
eis data.DTAStep-by-step guide, no prior Python experience needed.
1. Install prerequisites (one-time setup):
- Python - download from python.org/downloads and run the installer. Important: check "Add python.exe to PATH" on the first installer screen.
- Git (optional) - download from git-scm.com. If you don't want to install Git, download the project as a ZIP instead: on the GitHub page click Code -> Download ZIP and extract it.
2. Open PowerShell (Start menu -> type "PowerShell") and get the project:
git clone https://github.com/chmelat/eis_analysis
cd eis_analysis(If you downloaded the ZIP, use cd to enter the extracted folder instead.)
3. Create and activate a virtual environment (recommended - keeps the installation isolated):
python -m venv eis_env
eis_env\Scripts\Activate.ps1If activation fails with an error about scripts being disabled, allow local scripts first (one-time setting), then retry:
Set-ExecutionPolicy -ExecutionPolicy RemoteSigned -Scope CurrentUserIf you use the classic Command Prompt (cmd.exe) instead of PowerShell, activate with eis_env\Scripts\activate.bat.
4. Install and run:
pip install .
eis --help
eis data.DTAThe (eis_env) prefix in the prompt shows the environment is active. When you open a new PowerShell window later, activate it again with eis_env\Scripts\Activate.ps1 before running eis.
Note: If you install without a virtual environment and Windows reports eis is not recognized, the Python Scripts folder is not in your PATH (pip prints a warning about this during installation). Either use the virtual environment as shown above, or run the tool as python eis.py from the project folder.
If you prefer not to install the package, you can run the script directly:
pip install numpy scipy matplotlib # Install dependencies
python3 eis.py --help # Run script directly
python3 eis.py data.DTAOn Windows, use python instead of python3 (the python3 command does not exist there by default):
python eis.py --helpsudo apt install python3-numpy python3-scipy python3-matplotlib
pip install -e . # Then install the package# Development tools (ruff, mypy, pytest)
pip install -e ".[dev]"Run the test suite with pytest:
python3 -m pytest tests/ # All tests
python3 -m pytest tests/ -v # Verbose output
python3 -m pytest tests/ -q # Quiet mode
python3 -m pytest tests/test_drt_recovery.py # Single file
python3 -m pytest tests/ -k "voigt" # Tests matching patternOn Windows, use python -m pytest instead of python3 -m pytest.
Complete Python API: doc/PYTHON_API.md
| Document | Description |
|---|---|
| doc/PYTHON_API.md | Complete Python API reference |
| doc/WEIGHTING_AND_STATISTICS.md | Weighting types and statistical metrics |
| doc/ROBUST_LOSS_SOFT_L1.md | Robust loss (soft-L1): proposal, rationale and measured benefit - not implemented yet |
| doc/CIRCUIT_PARSER.md | Circuit parser syntax |
| doc/K_ELEMENT_GUIDE.md | K element guide |
| doc/MODEL_SELECTION_AIC_BIC.md | Choosing between circuits (AIC/BIC) |
| doc/LinKK_analysis.md | Kramers-Kronig validation |
| doc/ZHIT_IMPLEMENTATION_SPEC.md | Z-HIT validation |
| doc/DRT_INTUITION.md | DRT - intuitive introduction |
| doc/GCV_IMPLEMENTATION.md | Lambda selection (GCV + L-curve) documentation |
| doc/GMM_PEAK_DETECTION.md | GMM peak detection |
| doc/DRT_METHOD_ANALYSIS.md | DRT method analysis |
| doc/RINF_ESTIMATION.md | R_inf (ohmic resistance) estimation |
| doc/VOIGT_CHAIN_MATH.md | Voigt chain mathematics |
| doc/DIFFERENTIAL_EVOLUTION.md | Differential Evolution |
| doc/MULTISTART_OPTIMIZATION.md | Multi-start optimization |
| doc/NONLINEAR_FIT_ANALYSIS.md | Nonlinear optimization overview |
| doc/OXIDE_ANALYSIS_GUIDE.md | Oxide layer analysis |
- Orazem, M.E., Tribollet, B.: Electrochemical Impedance Spectroscopy (2008)
- Boukamp, B.A.: "A Linear Kronig-Kramers Transform Test for Immittance Data Validation", J. Electrochem. Soc. 142 (1995)
- Schonleber, M. et al.: "A Method for Improving the Robustness of linear Kramers-Kronig Validity Tests", Electrochimica Acta 131 (2014)
- Yrjana, V., Bobacka, J.: "Implementing Kramers-Kronig validity testing using pyimpspec", Electrochim. Acta 504 (2024)
- Wahba, G.: "A comparison of GCV and GML", Annals of Statistics 13 (1985)
- Saccoccio, M. et al.: "Optimal regularization in DRT", Electrochimica Acta 147 (2014)
This code was developed with the assistance of Claude Code.
License: MIT License
