Inversion recovery sequences

Changed by Yaïr Glick, 27 Mar 2017

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Inversion recovery pulse sequences are a type of MRI sequence used to produce images with heavy T1-weighting or to selectively null the signal for certain tissues (e.g. fat or fluid).

Physics

The basic part ofBasically, an inversion recovery (IR) pulse sequence is a spin echo pulse sequence preceded by a 180-degree° RF pulse. The preparatory pulse inverts longitudinal magnetisation (Mz), namely, it flips Mz to its negative value, -Mz. Tissues regain Mz at different longitudinal (T1) relaxation rates determined by their T1 relaxation times. The spin echo 90° readout pulse is applied at the beginningexact time when longitudinal magnetisation reaches the null point for the tissue we wish to suppress.The time elapsed between the preparatory 180° pulse and the 90° readout pulse is termed time to inversion (TI).

By choosing the appropriate TI, suppression of the pulse sequence, inverting the net magnetisation vector. After a pre-determined delay, known as the inversion time (TI), the rest of the pulse sequence (e.g. spin echo) occurs.

Spin echo inversion recovery

After the initial 180-degree inversion pulse, the usual spin echo or fast spin echo sequence can take place. Depending on the inversion time chosen specificdifferent tissues can be nulled, such that no signal is returnedpossible:

This techniqueInversion recovery can also be used to generate profoundly T1 weighted images.

Image reconstruction

Virtually all IR spin echo sequences use magnitude reconstruction for the final image. What this means is that pixel intensity reflects only the magnitude of longitudinal magnetisation, disregarding polarity; absolute values (i.e. absolute distances from the null point) are used.The little-used phase-sensitive inversion recovery (PSIR) reconstruction method, by contradistinction, takes polarity into account, rendering pixels with accentuatednegative Mz values darker and vice versa.

Advantages

These sequences offer several advantages:

  • twice the dynamic range of T1W spin echo sequences; due to the 180° inverting pulse, longitudinal relaxation goes from -Mz to Mz
  • using a short TI, longer T1 values will contribute to T2 contrast since inverted values are also rendered as positive when using magnitude reconstruction (see above) 
  • can be performed on a device with any magnetic field strength
  • relatively insensitive to magnetic field inhomogeneity (cf. SPIR/SPAIR)
  • relatively low susceptibility to metal, particularly useful for imaging patients with orthopedic hardware
  • can be used with fast (turbo) spin echo sequences, thereby reducing scan times

Disadvantages

  • 180° preparatory pulses lengthen scan times
  • higher specific absorption rate (SAR) due to additional 180° pulses
  • potential signal-to-noise ratio (SNR) decrease due to tissue suppression
  • increase in flow-related artifacts
  • inversion recovery technique is not specific to a certain tissue. For this reason, STIR should not be used with gadolinium injection, as tissues with T1 shortening owing to gadolinium uptake may be inadvertently suppressed along with fat
  • -<p><strong>Inversion recovery pulse sequences</strong> are a type of <a href="/articles/mri-sequences-overview">MRI sequence</a> used to produce images with heavy T1-weighting or selectively null the signal for certain tissues (e.g. fat or fluid). </p><p>The basic part of an inversion recovery sequence is 180-degree RF pulse at the beginning of the pulse sequence, inverting the net magnetisation vector. After a pre-determined delay, known as the inversion time (TI), the rest of the pulse sequence (e.g. spin echo) occurs.</p><h4>Spin echo inversion recovery</h4><p>After the initial 180-degree inversion pulse, the usual <a href="/articles/spin-echo-sequences">spin echo</a> or <a href="/articles/fast-spin-echo-sequence">fast spin echo sequence</a> can take place. Depending on the inversion time chosen specific tissues can be nulled, such that no signal is returned:</p><ul>
  • +<p><strong>Inversion recovery pulse sequences</strong> are a type of <a href="/articles/mri-sequences-overview">MRI sequence</a> used  to selectively null the signal for certain tissues (e.g. fat or fluid).</p><h4>Physics</h4><p>Basically, an inversion recovery (IR) pulse sequence is a <a href="/articles/spin-echo-sequences">spin echo pulse sequence</a> preceded by a 180° RF pulse. The preparatory pulse inverts longitudinal magnetisation (M<sub>z</sub>), namely, it flips M<sub>z</sub> to its negative value, -M<sub>z</sub>. Tissues regain M<sub>z</sub> at different longitudinal (T1) relaxation rates determined by their T1 relaxation times. The spin echo 90° readout pulse is applied at the exact time when longitudinal magnetisation reaches the null point for the tissue we wish to suppress.<br>The time elapsed between the preparatory 180° pulse and the 90° readout pulse is termed <strong>time to inversion</strong> (TI).</p><p>By choosing the appropriate TI, suppression of different tissues is possible:</p><ul>
  • -<a href="/articles/short-tau-inversion-recovery">STIR</a>: fat is nulled</li>
  • +<a href="/articles/short-tau-inversion-recovery">Short tau inversion recovery</a> (STIR): fat is nulled</li>
  • -<a href="/articles/fluid-attenuation-inversion-recovery">FLAIR</a> or <a href="/articles/double-inversion-recovery-sequence">DIR</a>: fluid is nulled</li>
  • -</ul><p>This technique can also be used to generate profoundly T1 weighted images with accentuated contrast. </p><p> </p>
  • +<a href="/articles/fluid-attenuation-inversion-recovery">Fluid attenuated inversion recovery</a> (FLAIR) or <a href="/articles/double-inversion-recovery-sequence">double inversion recovery</a> (DIR): fluid is nulled</li>
  • +</ul><p>Inversion recovery can also be used to generate profoundly T1 weighted images.</p><h4>Image reconstruction</h4><p>Virtually all IR spin echo sequences use magnitude reconstruction for the final image. What this means is that pixel intensity reflects only the magnitude of longitudinal magnetisation, disregarding polarity; absolute values (i.e. absolute distances from the null point) are used.<br>The little-used phase-sensitive inversion recovery (PSIR) reconstruction method, by contradistinction, takes polarity into account, rendering pixels with negative M<sub>z</sub> values darker and vice versa.</p><h4>Advantages</h4><p>These sequences offer several advantages:</p><ul>
  • +<li>twice the dynamic range of T1W spin echo sequences; due to the 180° inverting pulse, longitudinal relaxation goes from -M<sub>z</sub> to M<sub>z</sub>
  • +</li>
  • +<li>using a short TI, longer T1 values will contribute to T2 contrast since inverted values are also rendered as positive when using magnitude reconstruction (see above) </li>
  • +<li>can be performed on a device with any magnetic field strength</li>
  • +<li>relatively insensitive to magnetic field inhomogeneity (cf. SPIR/SPAIR)</li>
  • +<li>relatively low susceptibility to metal, particularly useful for imaging patients with orthopedic hardware</li>
  • +<li>can be used with fast (turbo) spin echo sequences, thereby reducing scan times</li>
  • +</ul><h4>Disadvantages</h4><ul>
  • +<li>180° preparatory pulses lengthen scan times</li>
  • +<li>higher specific absorption rate (SAR) due to additional 180° pulses</li>
  • +<li>potential signal-to-noise ratio (SNR) decrease due to tissue suppression</li>
  • +<li>increase in flow-related artifacts</li>
  • +<li>inversion recovery technique is not specific to a certain tissue. For this reason, <a href="/articles/short-tau-inversion-recovery">STIR</a> should not be used with <a href="/articles/gadolinium">gadolinium</a> injection, as tissues with T1 shortening owing to gadolinium uptake may be inadvertently suppressed along with fat</li>
  • +</ul>

References changed:

  • 2. Bushberg JT, Seibert JA, Leidholdt EM, Boone JM. The Essential Physics of Medical Imaging. Third edition (2012). Lippincott, Williams & Wilkins. <a href="https://books.google.co.uk/books?vid=ISBN9781451153941">ISBN: 9781451153941</a><span class="ref_v4"></span>
  • 2. Bushberg JT, Seibert JA, Jr. EML et-al. The Essential Physics of Medical Imaging. Lippincott Williams & Wilkins. (2002) ISBN:0683301187. <a href="http://books.google.com/books?vid=ISBN0683301187">Read it at Google Books</a> - <a href="http://www.amazon.com/gp/product/0683301187">Find it at Amazon</a><span class="auto"></span>

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