Refine
Year of publication
- 2012 (1)
Document Type
- Doctoral Thesis (1)
Language
- English (1)
Has Fulltext
- yes (1) (remove)
Is part of the Bibliography
- no (1)
Institute
- Biochemie und Chemie (1) (remove)
Nuclear Magnetic Resonance ("NMR") is a powerful and versatile technique relying on nuclei that posses a spin. Since its discovery more than 6 decades ago, NMR and related techniques has become a tool with innumerable applications throughout the fields of Physics, Chemistry, Biology and Medicine. Numerous Nobel Prizes have been awarded for work in the field and a multi billion dollar industry has developed on its basis.
One of NMR's major shortcomings is its inherent lack of sensitivity. Because it relies on the Boltzmann populations of spin states with a minuscule Zeeman splitting, this is particularly true for room temperature experiments.
As a result, in an enormous technological effort to enlarge the Zeeman splitting NMR magnets have been moving to higher and higher magnetic fields. However, even for proton spins possessing the largest magnetic moment of all nuclei, the degree of polarization that can be achieved in the strongest spectroscopic magnets available today (~24 T) at room temperature is merely ~ 8*(10 exp (-5)). In other words, this low polarization theoretically allows a sensitivity enhancement of 104 towards full polarization.
Since Magnetic Resonance Imaging ("MRI") is based on the same principle, it shares this problem with NMR. Furthermore, for technical and physiological reasons full body MRI tomographs do not reach the magnetic field strengths of spectroscopic NMR magnets, making this even more of an issue for MRI.
In consequence, MRI is chiefly restricted to detecting protons, while both MRI and NMR detection of 13C (or other low nuclei) under physiological conditions, i.e. low natural abundance of 13C and a low concentration of the respective substance, suffer from long acquisitions times that are necessary to obtain adequate signal to noise ratios ("SNR").
However, this drawb of NMR can be overcome. The enormous potential sensitivity increase of four orders of magnitude can - at least partially - be exploited by several hyperpolarization techniques, creating entirely new applications and fields of research.
These hyperpolarization techniques comprise chemical approaches like Parahydrogen Induced Polarization ("PHIP") or Photochemically Induced Dynamic Nuclear Polarization ("Photo-CIDNP"), as well as physical techniques like optically pumped (noble) gases13, 14 or Dynamic Nuclear Polarization ("DNP"), which will be the focus of this work. A hyperpolarized substance will render a larger signal without being physically or chemically altered in any other way. It is therefore "marked" without any marker, making it an agent free contrast agent for MRI.
DNP is a technique, in which hyperpolarization of nuclear spins is achieved by microwave (\MW") irradiation of unpaired electron spins in radicals, which are coupled to these nuclei, e.g. 1H, 13C or 15N. The electron spin population is perturbed if the microwave irradiation is resonant with the electron spin transition, which affects the polarization of hyperfine-coupled close nuclei. For large microwave power (i.e. saturating the electron spin transition) the orders of magnitude larger thermal electron spin polarization is effectively transferred to these nuclear spins in the sample. For proton spins the maximum polarization gain amounts to 660, whereas for 13C the sensitivity gain can be as large as 2600. In contrast to e.g. PHIP, which is restricted to specific reaction precursors, DNP is not limited to specific nuclei or hyperpolarization target molecules, making it a very versatile technique. DNP has been first proposed by Overhauser in 1953,15 and experimentally observed shortly thereafter in metals16 and liquids,17 both being systems with mobile electrons. In the 1960s and 70s, DNP was used as a spectroscopic tool in liquids, thoroughly mapping the effect in the low field regime. As well, several other transfer mechanisms were discovered, which are active in the solid state with localized electrons, namely the solid effect the cross effect and thermal mixing. The theory for all three of these mechanisms predicts reduced transfer efficiencies at higher magnetic fields. This fact and the lack of high frequency microwave sources to excite electron spins at magnetic field strengths above 1 T, effectively relegated DNP to a position of an interesting scientifi curiosity.
In the early 1990s, DNP came to a renaissance, when DNP was performed at high field in solid state magic angle spinning ("MAS") experiments using high power gyrotron microwave sources. This pioneering work sparked a surge of new developments and applications.
As well, this success triggered attempts to investigate also the potential of DNP in the liquid state at high magnetic fields, e.g. at 3.4 T35{38 and 9.2 T. To date, DNP can be considered one of the "hot topics" in the field of magnetic resonance, bringing about special issue in magnetic resonance journals and DNP sections on magnetic resonance conferences.
This thesis deals with the development of an in-bore liquid state DNP polarizer for MRI applications operating in ow through mode at a magnetic field strength of 1.5 T. Following this introductory chapter, the theoretical background necessary to understand and interpret the experimental results is explained in chapter 2. Subsequently, chapter 3 deals with the issue of performing liquid state DNP at high magnetic fields and its challenges. The chapter comprises a quick overview of the necessary hardware, the experimental findings for various samples and the interpretation of these findings. along with the ramifications for the aim of this work. Chapter 4 deals with the issue of increasing sensitivity and contrast in MRI, in particular by means of DNP. The chapter illustrates the development of our polarizer by presenting the hardware that was developed and demonstrating its performance under various conditions. As well, several alternative approaches are introduced and compared to our approach. Finally, chapter 5 summarizes the findings and gives an outlook on further developments.