Spinach (software)
 | This article reads like a press release or a news article and may be largely based on routine coverage. (December 2023) |
 | |
| Developer(s) | Ilya Kuprov (lead developer) |
|---|---|
| Initial release | 17 November 2011 |
| Stable release | 2.8
/ 6 August 2023 |
| Written in | Matlab |
| Operating system | Windows, Linux, macOS |
| Available in | English |
| Type | Magnetic resonance |
| License | MIT License |
| Website | spindynamics |
Spinach is an open-source magnetic resonance simulation package initially released in 2011[1] and continuously updated since.[2] The package is written in Matlab and makes use of the built-in parallel computing and GPU interfaces of Matlab.[3]
The name of the package whimsically refers to the physical concept of spin and to Popeye the Sailor who, in the eponymous comic books, becomes stronger after consuming spinach.[4]
Overview
[edit]Spinach implements magnetic resonance spectroscopy and imaging simulations by solving the equation of motion for the density matrix in the time domain:[1]
![{\displaystyle {\begin{matrix}{\frac {\partial }{\partial t}}\mathbf {\rho } \left(t\right)=-i\mathbf {L} \left(t\right)\mathbf {\rho } \left(t\right)\\\Downarrow \\\mathbf {\rho } \left(t+dt\right)=\exp \left[-i\mathbf {L} \left(t\right)dt\right]\mathbf {\rho } \left(t\right)\\\end{matrix}}}](https://wikimedia.riteme.site/api/rest_v1/media/math/render/svg/8a7930f055ca5ae3651655ae2ae8c71a6de763e9)
where the Liouvillian superoperator is a sum of the Hamiltonian commutation superoperator , relaxation superoperator , kinetics superoperator , and potentially other terms that govern spatial dynamics and coupling to other degrees of freedom:[2]
Computational efficiency is achieved through the use of reduced state spaces, sparse matrix arithmetic, on-the-fly trajectory analysis, and dynamic parallelization.[5]
Standard functionality
[edit]As of 2023, Spinach is cited in over 300 academic publications.[1] According to the documentation[2] and academic papers citing its features, the most recent version 2.8 of the package performs:
- Time-domain nuclear magnetic resonance (NMR) simulations of:
- Standard NMR experiments (DEPT, COSY, NOESY, HSQC, TOCSY, etc.).[6]
- Protein and nucleic acid NMR experiments (HNCA, HNCOCA, HNCO, etc.).[7]
- Magic angle spinning NMR experiments (CP-MAS, MQMAS, WISE, etc.).[8]
- Experiments involving residual dipolar coupling and other residual order effects.[9]
- Zero- and ultra-low field experiments, including Earth's field NMR.[10]
- Nuclear quadrupole resonance, including overtone NMR.[11]
- Time-domain magnetic resonance imaging (MRI) simulations, including:
- Standard and user-specified imaging sequences.[2]
- Diffusion coefficient and diffusion tensor imaging.[12]
- Three-dimensional point-resolved NMR spectroscopy.[13]
- Ultrafast spatially encoded NMR spectroscopy.[14]
- Time-domain electron spin resonance (ESR) simulations of:
- Standard pulsed ESR experiments (HYSCORE, ENDOR, ESEEM, etc.).
- Pulsed dipolar spectroscopy (DEER, RIDME, etc.).
- Dynamic nuclear polarization for static and spinning samples.[15]
Common models of spin relaxation (Redfield theory, stochastic Liouville equation, Lindblad theory) and chemical kinetics are supported, and a library of powder averaging grids is included with the package.[2]
Optimal control module
[edit]Spinach contains an implementation the gradient ascent pulse engineering (GRAPE) algorithm[16] for quantum optimal control. The documentation[2] and the book describing the optimal control module of the package[17] list the following features:
- L-BFGS quasi-Newton and Newton-Raphson GRAPE optimizers.
- Spin system trajectory analysis by coherence and correlation order.
- Spectrogram analysis of the pulse waveform.
- Prefixes, suffixes, keyholes, and freeze masks.
- Optimization of cooperative pulses and phase cycles.
- Waveform penalty functionals and instrument response.
Dissipative background evolution generators and control operators are supported, as well as ensemble control over distributions in common instrument calibration parameters, such as control channel power and offset.[2]
References
[edit]- ^ a b c Hogben, H.J.; Krzystyniak, M.; Charnock, G.T.P.; Hore, P.J.; Kuprov, I. (2011). "Spinach – a software library for simulation of spin dynamics in large spin systems". Journal of Magnetic Resonance. 208 (2): 179–194. doi:10.1016/j.jmr.2010.11.008. ISSN 1090-7807.
- ^ a b c d e f g "Spinach Documentation Wiki". SpinDynamics.org – Spin Dynamics Group. 28 July 2023. Retrieved 4 November 2023.
- ^ Kuprov, I. (2023). "Notes on software engineering". Spin: from basic symmetries to quantum optimal control. Springer. pp. 351–373. doi:10.1007/978-3-031-05607-9_9. ISBN 978-3-031-05606-2.
- ^ "Spinach - a fast and general spin dynamics simulation library" (PDF). Retrieved 2023-11-27.
- ^ Kuprov, I. (2023). "Incomplete basis sets". Spin: from basic symmetries to quantum optimal control. Springer. pp. 291–312. doi:10.1007/978-3-031-05607-9_7. ISBN 978-3-031-05606-2.
- ^ Concilio, M.G. (2020). "Large‐scale magnetic resonance simulations: a tutorial". Magnetic Resonance in Chemistry. 58 (8): 691–717. doi:10.1002/mrc.5018. ISSN 0749-1581.
- ^ Krushelnitsky, A.; Hempel, G.; Jurack, H.; Ferreira, T.M. (2023). "Rocking motion in solid proteins studied by the 15N proton-decoupled R1ρ relaxometry". Physical Chemistry Chemical Physics. 25 (23): 15885–15896. doi:10.1039/d3cp00444a. ISSN 1463-9076.
- ^ Gutmann, T.; Groszewicz, P.B.; Buntkowsky, G. (2019). "Solid-state NMR of nanocrystals". Annual Reports on NMR Spectroscopy. pp. 1–82. doi:10.1016/bs.arnmr.2018.12.001. ISSN 0066-4103.
- ^ Williams, R.V.; Yang, J.-Y.; Moremen, K.W.; Amster, I.J.; Prestegard, J.H. (2019). "Measurement of residual dipolar couplings in methyl groups via carbon detection". Journal of Biomolecular NMR. 73 (3–4): 191–198. doi:10.1007/s10858-019-00245-5. ISSN 0925-2738. PMC 7020099.
- ^ Kaseman, D.C.; Malone, M.W.; Tondreau, A.; Espy, M.A.; Williams, R.F. (2021). "Quantitation of nuclear magnetic resonance spectra at Earth's magnetic field". Analytical Chemistry. 93 (46): 15349–15357. doi:10.1021/acs.analchem.1c02910. ISSN 0003-2700.
- ^ Haies, I.M.; Jarvis, J.A.; Bentley, H.; Heinmaa, I.; Kuprov, I.; Williamson, P.T.F.; Carravetta, M. (2015). "14N overtone NMR under MAS: signal enhancement using symmetry-based sequences and novel simulation strategies". Physical Chemistry Chemical Physics. 17 (9): 6577–6587. doi:10.1039/c4cp03994g. ISSN 1463-9076. PMC 4673505.
- ^ Guduff, L.; Kuprov, I.; van Heijenoort, C.; Dumez, J.-N. (2017). "Spatially encoded 2D and 3D diffusion-ordered NMR spectroscopy". Chemical Communications. 53 (4): 701–704. doi:10.1039/c6cc09028a. ISSN 1359-7345.
- ^ Allami, A.J.; Concilio, M.G.; Lally, P.; Kuprov, I. (2019-07-05). "Quantum mechanical MRI simulations: solving the matrix dimension problem". Science Advances. 5 (7). doi:10.1126/sciadv.aaw8962. ISSN 2375-2548. PMC 6641938.
- ^ Dumez, J.-N. (2021). "Frequency-swept pulses for ultrafast spatially encoded NMR". Journal of Magnetic Resonance. 323: 106817. doi:10.1016/j.jmr.2020.106817. ISSN 1090-7807.
- ^ Redrouthu, V.S.; Mathies, G. (2022). "Efficient pulsed dynamic nuclear polarization with the X-inverse-X sequence". Journal of the American Chemical Society. 144 (4): 1513–1516. doi:10.1021/jacs.1c09900. ISSN 0002-7863.
- ^ Khaneja, N.; Reiss, T.; Kehlet, C.; Schulte-Herbrüggen, T.; Glaser, S.J. (2005). "Optimal control of coupled spin dynamics: design of NMR pulse sequences by gradient ascent algorithms". Journal of Magnetic Resonance. 172 (2): 296–305. doi:10.1016/j.jmr.2004.11.004. ISSN 1090-7807.
- ^ Kuprov, I. (2023). "Optimal control of spin systems". Spin: from basic symmetries to quantum optimal control. Springer. pp. 313–349. doi:10.1007/978-3-031-05607-9_8. ISBN 978-3-031-05606-2.