http://localhost/mediawiki/index.php?action=history&feed=atom&title=ISISISIS - Revision history2026-04-08T11:30:29ZRevision history for this page on the wikiMediaWiki 1.35.6http://localhost/mediawiki/index.php?title=ISIS&diff=787&oldid=prevJess at 17:28, 8 September 20222022-09-08T17:28:22Z<p></p>
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<td class="diff-context diff-side-deleted"><div>The '''[https://www.isis.stfc.ac.uk/Pages/home.aspx ISIS]''' neutron and muon source at the [https://www.ukri.org/about-us/stfc/locations/rutherford-appleton-laboratory/ Rutherford Appleton Laboratory] on the STFC [https://www.harwellcampus.com/ Harwell campus] near Oxford in Oxfordshire, UK produces ''pulsed'' muons from a synchrotron-driven proton beam on a target just upstream of the spallation neutron source. The advantages of ''pulsed'' muons are (1) that there is in principle no limit on how many muons can be stopped simultaneously in a sample; and (2) that irradiation with (''e.g.'') RF power for muon spin ''resonance'' experiments is vastly more efficient when applied to many muons at once. The primary disadvantages are (1) poor time resolution due to finite pulse width defining "<math>t=0</math>"; (2) the need to break up detectors into many small segments to avoid "pile-up" distortions. </div></td>
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<td class="diff-context diff-side-added"><div>The '''[https://www.isis.stfc.ac.uk/Pages/home.aspx ISIS]''' neutron and muon source at the [https://www.ukri.org/about-us/stfc/locations/rutherford-appleton-laboratory/ Rutherford Appleton Laboratory] on the STFC [https://www.harwellcampus.com/ Harwell campus] near Oxford in Oxfordshire, UK produces ''pulsed'' muons from a synchrotron-driven proton beam on a target just upstream of the spallation neutron source. The advantages of ''pulsed'' muons are (1) that there is in principle no limit on how many muons can be stopped simultaneously in a sample; and (2) that irradiation with (''e.g.'') RF power for muon spin ''resonance'' experiments is vastly more efficient when applied to many muons at once. The primary disadvantages are (1) poor time resolution due to finite pulse width defining "<math>t=0</math>"; (2) the need to break up detectors into many small segments to avoid "pile-up" distortions. </div></td>
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</table>Jesshttp://localhost/mediawiki/index.php?title=ISIS&diff=784&oldid=prevJess: Created page with "The '''[https://www.isis.stfc.ac.uk/Pages/home.aspx ISIS]''' neutron and muon source at the [https://www.ukri.org/about-us/stfc/locations/rutherford-appleton-laboratory/ Ruthe..."2022-09-08T17:23:57Z<p>Created page with "The '''[https://www.isis.stfc.ac.uk/Pages/home.aspx ISIS]''' neutron and muon source at the [https://www.ukri.org/about-us/stfc/locations/rutherford-appleton-laboratory/ Ruthe..."</p>
<p><b>New page</b></p><div>The '''[https://www.isis.stfc.ac.uk/Pages/home.aspx ISIS]''' neutron and muon source at the [https://www.ukri.org/about-us/stfc/locations/rutherford-appleton-laboratory/ Rutherford Appleton Laboratory] on the STFC [https://www.harwellcampus.com/ Harwell campus] near Oxford in Oxfordshire, UK produces ''pulsed'' muons from a synchrotron-driven proton beam on a target just upstream of the spallation neutron source. The advantages of ''pulsed'' muons are (1) that there is in principle no limit on how many muons can be stopped simultaneously in a sample; and (2) that irradiation with (''e.g.'') RF power for muon spin ''resonance'' experiments is vastly more efficient when applied to many muons at once. The primary disadvantages are (1) poor time resolution due to finite pulse width defining "<math>t=0</math>"; (2) the need to break up detectors into many small segments to avoid "pile-up" distortions. <br />
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Recent research highlights are featured at [https://www.isis.stfc.ac.uk/Pages/Science-Highlights.aspx Science Highlights].</div>Jess