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	<id>https://spindynamics.org/wiki/index.php?action=history&amp;feed=atom&amp;title=Hsqcetgpsi.m</id>
	<title>Hsqcetgpsi.m - Revision history</title>
	<link rel="self" type="application/atom+xml" href="https://spindynamics.org/wiki/index.php?action=history&amp;feed=atom&amp;title=Hsqcetgpsi.m"/>
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	<updated>2026-10-02T11:27:26Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
	<generator>MediaWiki 1.31.15</generator>
	<entry>
		<id>https://spindynamics.org/wiki/index.php?title=Hsqcetgpsi.m&amp;diff=10244&amp;oldid=prev</id>
		<title>Kuprov: version fragment to 2.13 per IK 2026-08-30</title>
		<link rel="alternate" type="text/html" href="https://spindynamics.org/wiki/index.php?title=Hsqcetgpsi.m&amp;diff=10244&amp;oldid=prev"/>
		<updated>2026-08-30T09:12:06Z</updated>

		<summary type="html">&lt;p&gt;version fragment to 2.13 per IK 2026-08-30&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 09:12, 30 August 2026&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l56&quot; &gt;Line 56:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 56:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[hsqcetgp.m]], [[hsqc.m]], [[ct_hsqc.m]], [[clip_hsqc.m]], [[hmqc.m]], [[coherence.m]], [[decouple.m]], [[dilute.m]], [[Built-in experiments]]&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[hsqcetgp.m]], [[hsqc.m]], [[ct_hsqc.m]], [[clip_hsqc.m]], [[hmqc.m]], [[coherence.m]], [[decouple.m]], [[dilute.m]], [[Built-in experiments]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;&amp;#160;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;''Version 2.&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;11&lt;/del&gt;, authors: [[Ilya Kuprov]]''&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;''Version 2.&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;13&lt;/ins&gt;, authors: [[Ilya Kuprov]]''&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Kuprov</name></author>
		
	</entry>
	<entry>
		<id>https://spindynamics.org/wiki/index.php?title=Hsqcetgpsi.m&amp;diff=10102&amp;oldid=prev</id>
		<title>Kuprov: sync with Spinach main f053e432: new page for sensitivity-improved echo/antiecho gradient-selected HSQC pulse sequence</title>
		<link rel="alternate" type="text/html" href="https://spindynamics.org/wiki/index.php?title=Hsqcetgpsi.m&amp;diff=10102&amp;oldid=prev"/>
		<updated>2026-08-30T08:12:20Z</updated>

		<summary type="html">&lt;p&gt;sync with Spinach main f053e432: new page for sensitivity-improved echo/antiecho gradient-selected HSQC pulse sequence&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{DISPLAYTITLE:hsqcetgpsi.m}} __NOTOC__&lt;br /&gt;
Sensitivity-improved echo/antiecho gradient-selected HSQC pulse sequence, based on the Bruker hsqcetgpsi pulse program and the standard HSQC sequence from:&lt;br /&gt;
&lt;br /&gt;
           https://doi.org/10.1016/0009-2614(80)80041-8&lt;br /&gt;
           https://doi.org/10.1002/cmr.a.10095&lt;br /&gt;
           https://doi.org/10.1016/0022-2364(91)90036-S&lt;br /&gt;
           https://doi.org/10.1021/ja00052a088&lt;br /&gt;
           https://doi.org/10.1007/BF00175254&lt;br /&gt;
&lt;br /&gt;
The gradient selection is represented analytically by coherence order selection statements.&lt;br /&gt;
&lt;br /&gt;
The simulation runs in the spherical tensor Liouville space formalism, and starts from Lz on the F2 nucleus. The front end is that of [[hsqcetgp.m]]: a 90-degree F2 pulse, an INEPT block of total duration 1/(2J) split in half by simultaneous 180-degree pulses on both channels, an F2 trim pulse of the user-specified angle, and the transfer pulses, of which the F1 90-degree pulse enters as the difference between the results of the +90 and the -90 degree rotations. The indirect dimension is evolved in two halves, with 180-degree refocusing pulses on the isotopes listed in parameters.decouple_f1 applied at the midpoint, and the first gradient pair is replaced by two [[coherence.m]] calls that keep F2 coherence order zero together with F1 coherence order +1 in the echo branch and -1 in the antiecho branch. Both branches then receive an F1 inversion pulse. The sensitivity improvement block that follows consists of a 90-degree pulse pair on F2 and F1 about X, a delay of parameters.si_time, simultaneous 180-degree pulses on both channels, a second delay of parameters.si_time, and a 90-degree pulse pair on F2 and F1 about Y. The back-transfer evolution of total duration 1/(2J) is then refocused by simultaneous 180-degree pulses, and is followed by a 90-degree and a 180-degree F2 pulse before the second gradient, which is represented by selection of F1 coherence order zero and F2 coherence order +1 in both branches. Decoupling of the isotopes listed in parameters.decouple_f2 is applied by [[decouple.m]], and L+ on the F2 nucleus is detected in the direct dimension.&lt;br /&gt;
&lt;br /&gt;
==Syntax==&lt;br /&gt;
&lt;br /&gt;
     fid=hsqcetgpsi(spin_system,parameters,H,R,K)&lt;br /&gt;
&lt;br /&gt;
==Parameters==&lt;br /&gt;
&lt;br /&gt;
     parameters.sweep              [F1 F2] sweep widths, Hz&lt;br /&gt;
 &lt;br /&gt;
     parameters.npoints            [F1 F2] numbers of points&lt;br /&gt;
 &lt;br /&gt;
     parameters.spins              {F1 F2} nuclei (e.g. '13C','1H')&lt;br /&gt;
 &lt;br /&gt;
     parameters.decouple_f2        nuclei to decouple in F2, e.g.&lt;br /&gt;
                                   {'15N','13C'}&lt;br /&gt;
 &lt;br /&gt;
     parameters.decouple_f1        nuclei that receive midpoint&lt;br /&gt;
                                   180-degree refocusing pulses in&lt;br /&gt;
                                   F1, e.g. {'1H','13C'}&lt;br /&gt;
 &lt;br /&gt;
     parameters.J                  working scalar coupling, Hz&lt;br /&gt;
 &lt;br /&gt;
     parameters.trim_angle         proton trim pulse angle, rad&lt;br /&gt;
 &lt;br /&gt;
     parameters.si_time            sensitivity improvement delay, s&lt;br /&gt;
 &lt;br /&gt;
     H  - Hamiltonian matrix, received from context function&lt;br /&gt;
 &lt;br /&gt;
     R  - relaxation superoperator, received from context function&lt;br /&gt;
 &lt;br /&gt;
     K  - kinetics superoperator, received from context function&lt;br /&gt;
&lt;br /&gt;
==Outputs==&lt;br /&gt;
&lt;br /&gt;
     fid.pos,fid.neg -  echo and antiecho components of the&lt;br /&gt;
                        signal.&lt;br /&gt;
&lt;br /&gt;
==Notes==&lt;br /&gt;
Natural abundance simulations should make use of the isotope dilution functionality. See [[dilute.m]] function.&lt;br /&gt;
&lt;br /&gt;
The function is only available for the sphten-liouv formalism, and parameters.decouple_f1 must not contain the F1 isotope itself.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
[[hsqcetgp.m]], [[hsqc.m]], [[ct_hsqc.m]], [[clip_hsqc.m]], [[hmqc.m]], [[coherence.m]], [[decouple.m]], [[dilute.m]], [[Built-in experiments]]&lt;br /&gt;
&lt;br /&gt;
''Version 2.11, authors: [[Ilya Kuprov]]''&lt;/div&gt;</summary>
		<author><name>Kuprov</name></author>
		
	</entry>
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