Solving non-linear frequency problem, NMR

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Discussion Overview

The discussion revolves around a complex problem in solid-state NMR data analysis, specifically focusing on the challenge of solving for parameters A, B, and C from non-linear frequency equations involving signal phases. The scope includes theoretical aspects of NMR, mathematical reasoning, and potential experimental approaches.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant introduces a set of equations representing signal phases in 3D NMR data, suggesting that A, B, and C can theoretically be determined despite the non-linear term complicating the process.
  • Another participant notes that A, B, and C cannot be separated due to their identical appearance in the equations.
  • A clarification is made regarding the presence of coefficients in front of the unknowns, indicating that these coefficients form a singular matrix, which complicates the solution.
  • One participant expresses a desire for a transformation or method that could aid in solving the problem, offering acknowledgment in a future paper as an incentive.
  • Further details are provided about the equations, including the dependence of coefficients on spin angular momentum quantum numbers and Clebsch-Gordon coefficients.
  • A historical reference is made to Frydman's shearing transformation, which is suggested as a method to eliminate certain terms in the equations to isolate isotropic frequencies.
  • Concerns are raised about the singularity of the coefficient matrix, with a suggestion to vary the experiment to obtain a non-singular matrix or to seek additional information through double-quantum coherence.
  • A participant reflects on the difficulties of the problem, acknowledging the linear dependence of the coefficients and considering the implications of including third-order effects.

Areas of Agreement / Disagreement

Participants express a range of views on the problem, with no consensus reached regarding the feasibility of solving for A, B, and C given the singular matrix issue and the non-linear nature of the equations. Multiple competing approaches and hypotheses are presented without resolution.

Contextual Notes

The discussion highlights limitations related to the linear dependence of coefficients and the singularity of the matrix, which are acknowledged but not resolved. The complexity of the equations and the experimental conditions are also noted as factors influencing the problem.

zeta
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Hi All;
Long time reader, first time poster.
Here's a tricky one. I have a solid state NMR set of data in 3D. Let's say the signal phases
in the three dimensions are:
exp(i*(A+B*C+C)t_1)
exp(i*(A+B*C+C)t_2)
exp(i*(A+B*C+C)t_3)

given the information, one should be able to (in theory) determine A,B,C... however given the fact that there is a patently non-linear term this is non-trivial. Any ideas?
 
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Since A, B and C enter the same way in every equation, they cannot be separated.
 
sorry, I should have included the fact that there are coefficients in front of the unknowns ie.,
one can write the coefficients as a 3*3 matrix which is singular.
The frequencies in the phase are derived from Average Hamiltonian theory
thanks for the interest!

ED: error
 
ps if someone can think of a transform or method for solution, then you will at the very least get an acknowledgment on a paper
 
Still don't get it. Do the coefficients differ in the 3 eqns? Are they known?

It would help if you can make a more detailed and exact statement of the problem.
 
Here's what the phases amount to in terms of equations:

a*A+b*B*C+c*C
d*A+e*B*C+f*C
g*A+h*B*C+i*C

I would like to solve for A,B,C given the coefficients, which depend on the spin angular momentum quantum numbers of the transitions (r <-> c), as well as Clebsch-Gordon coefficients.
In the mid nineties frydman introduced the shearing transformation whereby in 2d NMR one may remove the quadrupolar anisotropy ( term C) by essentially eliminating this from line 2 (indirect detected dimension, delta m \neq +/- 1) by multiplying line two by a multiple of line one (direct detected dimension, delta m = +/- 1).
In the indirect dimension the frequency is thus a linear sum of the isotropic contributions, terms A, B.

ED: errors

hence the MO for doing 3d is to completely isolate the isotropic frequencies
 
Last edited:
I'm not worried about the non-linearity, but if your coefficient matrix is truly singular then i think you are hosed. Can you vary your experiment to get a matrix that's non-singular? (Well-conditioned is better yet!)

Can you get additional info some other way? My NMR knowledge is poor so I'll probably embarrass myself with this question, but how about double-quantum coherence?
 
yes, 'hosed' is the right word for it. The underlying problem is the linear dependence of the C-G coefficients unfortunately. However I think you hit the nail viz more information and this is the tack I was taking. The second line is in fact double quantum (the third triple) and my thought was to lift the linear dependence by including third order effects on this non-symmetric transition (3/2<->-1/2), but then my elegant paper/experiment goes to hell. such is life I guess...

thanks for the advice!
 
That's usually the way it goes. If it were easy someone would already have done it...
 
  • #10
yeah, ain't physics grand :)
 

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