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| About the Authors | p. viii |
| Preface | p. x |
| Acknowledgments | p. xv |
| Basic tasks of signal processing in spectroscopy | p. 1 |
| Challenges with quantification of time signals | p. 11 |
| The quantum-mechanical concept of resonances in scattering and spectroscopy | p. 20 |
| Resonance profiles | p. 24 |
| Why is this topic relevant for biomedical researchers and clinical practitioners? | ... MOREp. 26 |
| The role of quantum mechanics in signal processing | p. 29 |
| Direct link of quantum-mechanical spectral analysis with rational response functions | p. 31 |
| Expansion methods for signal processing | p. 40 |
| Non-classical polynomials | p. 40 |
| Classical polynomials | p. 53 |
| Recurrent time signals and their generating fractions as spectra with no recourse to Fourier integrals | p. 56 |
| The fast Padé transform for quantum-mechanical spectral analysis and signal processing | p. 63 |
| Padé acceleration and analytical continuation of time series | p. 65 |
| Description of the background contribution by the off-diagonal fast Padé transform | p. 67 |
| Diagonal and para-diagonal fast Padé transform | p. 69 |
| Determination of the exact number K of resonances | p. 74 |
| Exact Shank's filter for finding K, including the fundamental frequencies and amplitudes: the use of Wynn's recursion | p. 74 |
| Exact number K and the existence of the solution of ordinary difference equations | p. 77 |
| The role of linear dependence as spuriousness in determining K within the state space-based perspective of signal processing | p. 78 |
| Froissart doublet spuriousness in the frequency domain for finding K | p. 81 |
| Froissart doublets in exact analytical computations | p. 82 |
| Exact quantum-mechanical, Padé-based recovery of spectral parameters | p. 85 |
| Input data (tabular & graphic) and reconstructed tabular data | p. 91 |
| Input tabular data for the spectral parameters of 25 resonances | p. 91 |
| Numerical values of the reconstructed spectral parameters at six signal lengths, N/M (N = 1024, M = 1-32) | p. 95 |
| Numerical values of the reconstructed spectral parameters near full convergence for 3 partial signal lengths NP = 180, 220, 260 | p. 97 |
| Graphic presentation of the input data | p. 99 |
| Absorption total shape spectra | p. 104 |
| Absorption total shape spectra or envelopes | p. 104 |
| Padé and Fourier convergence rates of absorption total shape spectra | p. 107 |
| Residual spectra and consecutive difference spectra | p. 110 |
| Residual or error absorption total shape spectra | p. 110 |
| Residual or error absorption total shape spectra near full convergence | p. 113 |
| Consecutive difference spectra for absorption envelope spectra | p. 113 |
| Consecutive differences for absorption envelope spectra near full convergence | p. 116 |
| Absorption component shape spectra of individual resonances | p. 116 |
| Absorption component spectra and metabolite maps | p. 116 |
| Absorption component spectra and envelope spectra near full convergence | p. 118 |
| Distributions of reconstructed spectral parameters in the complex plane | p. 121 |
| Distributions of spectral parameters in FPT(+) | p. 121 |
| Distributions of spectral parameters in FPT(-) | p. 124 |
| Convergence of fundamental frequencies in FPT(-) | p. 126 |
| Distributions of fundamental frequencies in FPT(±) near full convergence | p. 126 |
| Convergence of fundamental amplitudes in FPT(-) | p. 129 |
| Distribution of fundamental amplitudes in FPT(±) near full convergence | p. 131 |
| Preview of illustrations for the concept of Froissart doublets | p. 133 |
| The importance of exact quantification for MRS | p. 138 |
| Harmonic transients in time signals | p. 149 |
| Rational response function to generic external perturbations | p. 149 |
| The exact solution for the general harmonic inversion problem | p. 151 |
| General time series | p. 152 |
| The response or the Green function | p. 154 |
| The key prior knowledge: Internal structure of time signals | p. 155 |
| The Rutishauser quotient-difference recursive algorithm | p. 159 |
| The Gordon product-difference recursive algorithm | p. 161 |
| The Lanczos algorithm for continued fractions | p. 167 |
| The Padé-Lanczos approximant | p. 169 |
| The fast Padé transform FPT(-) outside the unit circle | p. 170 |
| The fast Padé transform FPT(+) inside the unit circle | p. 173 |
| Signal-noise separation via Froissart doublets | p. 177 |
| Critical importance of poles and zeros in generic spectra | p. 178 |
| Spectral representations via Padé poles and zeros as pFPT(±) and zFPT(±) | p. 178 |
| Padé canonical spectra | p. 180 |
| Signal-noise separation with exclusive reliance upon resonant frequencies | p. 181 |
| Model reduction problem via Padé canonical spectra | p. 183 |
| Denoising Froissart filter | p. 184 |
| Signal-noise separation with exclusive reliance upon resonant amplitudes | p. 185 |
| Padé partial fraction spectra | p. 189 |
| Model reduction problem via Heaviside or Padé partial fraction spectra | p. 190 |
| Disentangling genuine from spurious resonances | p. 192 |
| Machine accurate quantification and illustrated signal-noise separation | p. 193 |
| Formulation of the most stringent test for quantification in MRS | p. 193 |
| The key factors for high resolution in quantification | p. 195 |
| The goals and plan for presentation of results | p. 196 |
| Numerical presentation of the spectral parameters | p. 200 |
| Input spectral parameters with 12-digit accuracy | p. 200 |
| Exponential convergence rates of Padé reconstructions of spectral parameters with 12-digit accuracy | p. 202 |
| Signal-noise separation via Froissart doublets with pole-zero coincidences | p. 205 |
| Converged Padé genuine resonances and lack of convergence of Froissart doublets in FPT(±) with a quarter of full signal length | p. 205 |
| Zooming near convergence for Padé genuine resonances and instability of non-converged configurations of Froissart doublets in FPT(±) | p. 216 |
| Practical significance of the Froissart filter for exact signal-noise separation | p. 224 |
| Padé processing for MR spectra from in vivo time signals | p. 227 |
| Relative performance of the FPT and FFT for total shape spectra for encoded FIDs | p. 227 |
| The FIDs, convergence regions and absorption spectra at full signal length encoded at high magnetic field strengths | p. 228 |
| Convergence patterns of FPT(-) and FFT for absorption total shape spectra | p. 231 |
| Error Analysis for encoded in vivo time signals | p. 241 |
| Residual spectra as the difference between the fully converged Fourier and Padé spectra at various partial signal lengths | p. 242 |
| Self-contained Padé error analysis: Consecutive difference spectra | p. 245 |
| Prospects for comprehensive applications of the fast Padé transform to in vivo MR time signals encoded from the human brain | p. 250 |
| Magnetic resonance in neuro-oncology: Achievements and challenges | p. 251 |
| MRS and MRSI as a key non-invasive diagnostic modality for neuro-oncology | p. 251 |
| MRI for brain tumor diagnostics | p. 251 |
| Primary diagnosis of brain tumors by MRS & MRSI | p. 253 |
| Grading of primary brain tumors by MRS & MRSI | p. 256 |
| Characterization of brain tumors by MRS & MRSI | p. 258 |
| MRSI for target planning for brain tumors | p. 260 |
| Assessing response of brain tumors to therapy and prognosis via MRSI | p. 260 |
| Major limitations and dilemmas in MRS & MRSI for neuro-oncology due to FFT envelopes and fittings | p. 262 |
| Poor resolution and SNR | p. 263 |
| Unreliable quantifications by fitting FFT spectra | p. 267 |
| Fitting estimates for concentrations of a small number of metabolites | p. 269 |
| Lack of component spectra of clinically important over-lapping resonances for brain tumor diagnostics | p. 269 |
| The number of metabolites & non-uniqueness of fitting | p. 270 |
| Accurate extraction of clinically-relevant metabolite concentrations for neuro-diagnostics via MRS | p. 272 |
| Methodological strategy: The need for standards in quantification | p. 272 |
| High-resolution quantification of brain MR signals in a clinician-friendly format | p. 272 |
| Padé-reconstructed lipids in the MR brain spectrum | p. 275 |
| Padé reconstruction of the components of total choline at 3.2 ppm to 3.3 ppm on the MR brain spectrum | p. 276 |
| Padé reconstruction in the region between 3.6 ppm and 4.0 ppm on the MR brain spectrum | p. 276 |
| Padé quantification of malignant and benign ovarian MRS data | p. 277 |
| Studies to date using in vivo proton MRS to evaluate benign and malignant ovarian lesions | p. 278 |
| Insights for ovarian cancer diagnostics from in vitro MRS | p. 280 |
| Padé versus Fourier for in vitro MRS data derived from benign and malignant ovarian cyst fluid | p. 282 |
| Padé versus Fourier for MRS data derived from benign ovarian cyst fluid | p. 284 |
| Padé versus Fourier for MRS data derived from malignant ovarian cyst fluid | p. 289 |
| Summary comparisons of the performance of FPT and FFT for MRS data derived from benign and malignant ovarian cyst fluid | p. 293 |
| Prospects for Padé-optimized MRS for ovarian cancer diagnostics | p. 302 |
| Breast cancer and non-malignant breast data: Quantification by FPT | p. 303 |
| Current challenges in breast cancer diagnostics | p. 303 |
| In vivo MR-based modalities for breast cancer diagnostics and clinical assessment | p. 304 |
| Magnetic resonance imaging applied to detection of breast cancer | p. 304 |
| Studies to date using in vivo MRS for distinguishing between benign and malignant breast lesions | p. 305 |
| In vivo MRS to assess response of breast cancer to therapy | p. 307 |
| Special challenges of in vivo MRS for breast cancer diagnostics | p. 308 |
| Insights for breast cancer diagnostics from in vitro MRS | p. 309 |
| Performance of the FPT for MRS data from breast tissue | p. 311 |
| Padé-reconstruction of MRS data for normal breast tissue | p. 312 |
| Padé-reconstruction of MRS data from fibroadenoma | p. 318 |
| Padé-reconstruction of MRS data from breast cancer | p. 322 |
| Comparison of the Padé findings for normal breast, fibroadenoma and breast cancer | p. 326 |
| Prospects for Padé-optimized MRS for breast cancer diagnostics | p. 330 |
| Multiplet resonances in MRS data from normal and cancerous prostate | p. 331 |
| Dilemmas and difficulties in prostate cancer diagnostics and screening | p. 331 |
| Initial detection of prostate cancer with in vivo MRS and MRSI | p. 332 |
| Distinguishing high from low risk prostate cancer | p. 334 |
| Surveillance for residual disease or local recurrence after therapy | p. 334 |
| Treatment planning and other aspects of clinical management | p. 335 |
| Limitations of current applications of in vivo MRSI directly relevant to prostate cancer | p. 335 |
| Insights for prostate cancer diagnostics by means of 2D in vivo MRS and in vitro MRS | p. 336 |
| Performance of the fast Padé transform for MRS data from prostate tissue | p. 339 |
| Normal glandular prostate tissue: MR spectral data reconstructed by FPT | p. 344 |
| Normal stromal prostate tissue: MR spectral data reconstructed by FPT | p. 350 |
| Malignant prostate tissue: MR spectral information reconstructed by FPT | p. 356 |
| Comparison of MRS retrievals from prostate tissue: Normal glandular, normal stromal and cancerous | p. 362 |
| Prospects for Padé-optimized MRSI within prostate cancer diagnostics | p. 370 |
| Recapitulation of Padé-optimized processing of biomedical time signals | p. 371 |
| The central role of rational functions in the theory of approximations | p. 371 |
| The dominant role of Padé approximant among all rational functions | p. 372 |
| Relevance of Padé-optimized MRS for diagnostics in clinical oncology | p. 382 |
| Conclusion and outlooks | p. 389 |
| Leading role of Padé approximants in the theory of rational functions and in MRS | p. 390 |
| Outlooks for Padé-optimized MRS and MRSI from a clinical perspective | p. 395 |
| List of acronyms | p. 399 |
| References | p. 401 |
| Index | p. 441 |
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