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|a 9783540780236
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|a 10.1007/978-3-540-78023-6
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|a Chrysikopoulos, Haris S.
|e author.
|4 aut
|4 http://id.loc.gov/vocabulary/relators/aut
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|a Clinical MR Imaging and Physics
|h [electronic resource] :
|b A Tutorial /
|c by Haris S. Chrysikopoulos.
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|a 1st ed. 2009.
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|a Berlin, Heidelberg :
|b Springer Berlin Heidelberg :
|b Imprint: Springer,
|c 2009.
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|a IX, 176 p.
|b online resource.
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|a text
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|a Resonance -- Electromagnetic Fields -- Macroscopic Magnetization -- Macroscopic Magnetization Revisited -- Excitation Phenomena -- T1 Relaxation (Longitudinal or Spin-Lattice Relaxation) -- T2 Relaxation (Transverse or Spin-Spin Relaxation) -- Magnetic Substrates of T1 Relaxation -- Magnetic Substrates of T2 Relaxation -- Proton (Spin) Density Contrast -- Partial Saturation -- Free Induction Decay -- Spin Echo -- Integration of T1, T2, and Proton Density Phenomena -- Inversion Recovery -- Image Formation - Fourier Transform - Gradients -- Gradient Echo Imaging -- Pulse Sequences -- Fast or Turbo Spin Echo Imaging -- Selective Fat Suppression -- Chemical Shift Imaging -- Magnetization Transfer Contrast -- Diffusion -- Artifacts -- Noise -- Imaging Time -- Resolution -- Contrast Agents -- Blood Flow -- MR Angiography -- Basics of MR Examinations and Interpretation.
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|a Keywords Spin › Electromagnetic radiation › Resonance › Nucleus › Hydrogen › Proton › Certain atomic nuclei possess inherent magnetic Let us summarize the MRI procedure. Te patient properties called spin, and can interact with electro- is placed in a magnetic feld and becomes temporarily 1 magnetic (EM) radiation through a process called magnetized. Resonance is achieved through the - resonance. When such nuclei absorb EM energy they plication of specifc pulses of EM radiation, which is proceed to an excited, unstable confguration. Upon absorbed by the patient. Subsequently, the excess - return to equilibrium, the excess energy is released, ergy is liberated and measured. Te captured signal producing the MR signal. Tese processes are not is processed by a computer and converted to a gray random, but obey predefned rules. scale (MR) image. Te simplest nucleus is that of hydrogen (H), con- Why do we need to place the patient in a m- sisting of only one particle, a proton. Because of its net? Because the earth's magnetic feld is too weak to abundance in humans and its strong MR signal, H be clinically useful; it varies from 0. 3-0. 7 Gauss (G). is the most useful nucleus for clinical MRI. Tus, foC r urrent clinical MR systems operate at low, mid or our purposes, MRI refers to MRI of hydrogen, and for h igh feld strength ranging from 0. 1 to 3.
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|a Radiology.
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|a Radiology.
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|a SpringerLink (Online service)
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|t Springer Nature eBook
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|i Printed edition:
|z 9783540870661
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|i Printed edition:
|z 9783540779995
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|u https://doi.uam.elogim.com/10.1007/978-3-540-78023-6
|z Texto Completo
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|a ZDB-2-SME
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|a ZDB-2-SXM
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|a Medicine (SpringerNature-11650)
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|a Medicine (R0) (SpringerNature-43714)
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