2004
DOI: 10.1063/1.1628216
|View full text |Cite
|
Sign up to set email alerts
|

Exact effective Hamiltonian theory. II. Polynomial expansion of matrix functions and entangled unitary exponential operators

Abstract: Our recent exact effective Hamiltonian theory (EEHT) for exact analysis of nuclear magnetic resonance (NMR) experiments relied on a novel entanglement of unitary exponential operators via finite expansion of the logarithmic mapping function. In the present study, we introduce simple alternant quotient expressions for the coefficients of the polynomial matrix expansion of these entangled operators. These expressions facilitate an extension of our previous closed solution to the Baker-Campbell-Hausdorff problem … Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
12
0

Year Published

2008
2008
2016
2016

Publication Types

Select...
6
1
1

Relationship

1
7

Authors

Journals

citations
Cited by 18 publications
(12 citation statements)
references
References 23 publications
0
12
0
Order By: Relevance
“…These calculations were performed using exact effective Hamiltonian theory (EEHT) [19, 20] and expanded to fifth order with respect to resonance offset. For the XY-8 scheme,…”
Section: Resultsmentioning
confidence: 99%
“…These calculations were performed using exact effective Hamiltonian theory (EEHT) [19, 20] and expanded to fifth order with respect to resonance offset. For the XY-8 scheme,…”
Section: Resultsmentioning
confidence: 99%
“…The outcome of numerical optimizations with optimal control may not only provide optimum experiments for direct applications, but may also provide new insight into, e.g., the maximal possible transfer efficiencies, which then may be used (i) as an evaluation of whether there is room for improvements of state-of-the-art experiments and (ii) to provide new inspiration to alternative design strategies, for example based on average (or effective) Hamiltonian theory [40][41][42][43]. As an example of the latter, it became clear from optimal control design of heteronuclear coherence transfer schemes in solid-state NMR [14] that optimal control can increase the efficiency of so-called c-encoded dipolar recoupling experiments [44] by compensating more efficiently for spread in another crystallite orientation angle (b) leading to the concept of COMpensation for Beta (COMB) composite refocusing [45].…”
Section: Introductionmentioning
confidence: 99%
“…This approach is still of central importance in theory of multiple-pulse NMR, despite the emergence of alternative methods such as the Floquet theory, 8,9 the exact effective Hamiltonian theory, 10,11 and the Fer expansion, 12 which have advantages in some circumstances. I will only use the AHT in this article.…”
Section: Introductionmentioning
confidence: 99%