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Of course it can. Use the imaging() context (see imaging examples for how to use it); it returns gradients as operators. At that point, gradient operators may be used in exactly the same way as pulse operators, including in shaped pulse functions, such as shaped_pulse_xy(), including simultaneously ...

Okay, I'll cook up something - it will be slow af, but it will work.

How's this looking? In Hilbert space, computationally efficient coherence selection is non-trivial because (unlike in spherical tensor notation) the basis is not already sorted by single-spin coherence order.

Alright - I think I can do the syntax matching. Working on it...

It would actually be very useful to know what syntax fees more natural - I can make alterations of course. How would you wish that parametrisation to work?

Okay, in the order of the original post: 1. The sys.magnet parameter does set the centre of the sweep - this is the field that goes into the background Hamiltonian in Line 70 of dnp_field_sweep.m function. The microwave offset is then added in Line 78, and the field offset inside the loop. The code ...

Dear Rajat, of course it would slow down as you add more spins - without approximations, the complexity of Liouville space simulations of spin-1/2 systems grows very rapidly. Matrix dimensions go as 4^n, and then matrix-vector multiplication complexity scales quadratically with the dimension, so we ...

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Use this direct link for now:

https://spindynamics.org/documents/spinach_2_7_6009.zip - that's the latest Spinach, it includes DEERNet and the descrambling functionality. The documentation Wiki (http://spindynamics.org/wiki/index.php?title=Main_Page) appears to be up.

Thanks for the heads-up, I am on the phone with the hosting provider.