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	<id>https://spindynamics.org/wiki/index.php?action=history&amp;feed=atom&amp;title=Hsqcedetgp.m</id>
	<title>Hsqcedetgp.m - Revision history</title>
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	<updated>2026-10-04T09:12:30Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
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	<entry>
		<id>https://spindynamics.org/wiki/index.php?title=Hsqcedetgp.m&amp;diff=10239&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=Hsqcedetgp.m&amp;diff=10239&amp;oldid=prev"/>
		<updated>2026-08-30T09:12:00Z</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-l50&quot; &gt;Line 50:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 50:&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;[[hsqc.m]], [[ct_hsqc.m]], [[clip_hsqc.m]], [[hmqcetgp.m]], [[hmqcetgpsi.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;[[hsqc.m]], [[ct_hsqc.m]], [[clip_hsqc.m]], [[hmqcetgp.m]], [[hmqcetgpsi.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=Hsqcedetgp.m&amp;diff=10096&amp;oldid=prev</id>
		<title>Kuprov: new page for Spinach main f053e432: documents hsqcedetgp.m from the source header and implementation</title>
		<link rel="alternate" type="text/html" href="https://spindynamics.org/wiki/index.php?title=Hsqcedetgp.m&amp;diff=10096&amp;oldid=prev"/>
		<updated>2026-08-30T08:03:10Z</updated>

		<summary type="html">&lt;p&gt;new page for Spinach main f053e432: documents hsqcedetgp.m from the source header and implementation&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{DISPLAYTITLE:hsqcedetgp.m}} __NOTOC__&lt;br /&gt;
Echo/antiecho gradient-selected multiplicity-edited HSQC pulse sequence, based on the Bruker hsqcedetgp pulse program and the standard HSQC sequence from [https://doi.org/10.1016/0009-2614(80)80041-8 https://doi.org/10.1016/0009-2614(80)80041-8], [https://doi.org/10.1002/cmr.a.10095 https://doi.org/10.1002/cmr.a.10095], and [https://doi.org/10.1002/mrc.1260310315 https://doi.org/10.1002/mrc.1260310315]. The gradient selection is represented analytically by coherence order selection statements.&lt;br /&gt;
&lt;br /&gt;
The Liouvillian is assembled as L=H+i*R+i*K, the two evolution time steps are the reciprocals of the sweep widths, and the J-coupling evolution time is delta=1/(2*|J|). The initial condition is Lz on the F2 nucleus and the detection state is L+ on the same nucleus. The INEPT block is a 90-degree F2 pulse, an evolution over delta/2, simultaneous 180-degree pulses on both channels, and a second evolution over delta/2. A trim pulse of parameters.trim_angle is then applied on the F2 channel, followed by a 90-degree F2 pulse about Ly and the transfer pulse on the F1 channel, which is taken as the difference between the +90-degree and the -90-degree rotations; this retains twice the part of the density matrix that changes sign with the phase of the F1 pulse and cancels the rest.&lt;br /&gt;
&lt;br /&gt;
The first half of the F1 evolution is run as a trajectory with npoints(1)-1 steps, midpoint 180-degree pulses are applied on every channel listed in parameters.decouple_f1, and the second half is run in refocusing mode. The echo and the antiecho branches are separated by retaining zero coherence order on the F2 nucleus together with, respectively, the +1 and the -1 coherence order on the F1 nucleus. Multiplicity editing follows: an evolution over parameters.edit_time, simultaneous 180-degree pulses on both channels, and a second evolution over parameters.edit_time. Back transfer is a simultaneous 90-degree pulse on both channels, an evolution over delta/2, simultaneous 180-degree pulses, and a further evolution over delta/2. The second analytical selection, onto zero coherence order on the F1 nucleus and +1 on the F2 nucleus, is followed by decoupling of the channels listed in parameters.decouple_f2 by [[decouple.m]] function and by separate detection of the two branches with npoints(2)-1 steps. The function requires the sphten-liouv formalism.&lt;br /&gt;
&lt;br /&gt;
==Syntax==&lt;br /&gt;
&lt;br /&gt;
     fid=hsqcedetgp(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.edit_time          multiplicity editing 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;
Note: natural abundance simulations should make use of the isotope dilution functionality. See [[dilute.m]] function.&lt;br /&gt;
&lt;br /&gt;
The multiplicity editing block is a pair of parameters.edit_time delays around simultaneous 180-degree pulses on both channels, and so the total editing period is twice parameters.edit_time.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
[[hsqc.m]], [[ct_hsqc.m]], [[clip_hsqc.m]], [[hmqcetgp.m]], [[hmqcetgpsi.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>
		
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