Author: bugman
Date: Thu Nov 28 22:43:31 2013
New Revision: 21698
URL: http://svn.gna.org/viewcvs/relax?rev=21698&view=rev
Log:
Completed the relaxation dispersion model list at
http://www.nmr-relax.com/analyses/relaxation_dispersion.html.
Modified:
website/analyses/relaxation_dispersion.html
Modified: website/analyses/relaxation_dispersion.html
URL:
http://svn.gna.org/viewcvs/relax/website/analyses/relaxation_dispersion.html?rev=21698&r1=21697&r2=21698&view=diff
==============================================================================
--- website/analyses/relaxation_dispersion.html (original)
+++ website/analyses/relaxation_dispersion.html Thu Nov 28 22:43:31 2013
@@ -53,7 +53,7 @@
<h2>Models</h2>
<p>Numerous analytic and numeric relaxation dispersion models are
supported by relax. It the model you are interested is not yet supported,
please see the <a
href="http://wiki.nmr-relax.com/Tutorial_for_adding_relaxation_dispersion_models_to_relax";>tutorial
for adding dispersion models to relax</a>.</p>
- <h3>Experiment type independent models</h3>
+ <h3>Experiment independent models</h3>
<p>The following models are independent of the experiment type:</p>
<ul>
@@ -69,7 +69,7 @@
<li><b>'LM63 3-site'</b>: The original Luz and Meiboom 1963 3-site
fast exchange equation with parameters <em>{R<sub>2</sub><sup>0</sup>, ...,
Φ<sub>exB</sub>, k<sub>B</sub>, Φ<sub>exC</sub>,
k<sub>C</sub>}</em>.</li>
<li><b>'<a href="http://wiki.nmr-relax.com/CR72";>CR72</a>'</b>: The
reduced Carver and Richards 1972 2-site equation for most time scales whereby
the simplification <em>R<sub>2A</sub><sup>0</sup> =
R<sub>2B</sub><sup>0</sup></em> is assumed. It has the parameters
<em>{R<sub>2</sub><sup>0</sup>, ..., p<sub>A</sub>, Δω,
k<sub>ex</sub>}</em>.</li>
<li><b>'<a href="http://wiki.nmr-relax.com/CR72_full";>CR72
full</a>'</b>: The full Carver and Richards 1972 2-site equation for most
time scales with the parameters <em>{R<sub>2A</sub><sup>0</sup>,
R<sub>2B</sub><sup>0</sup>, ..., p<sub>A</sub>, Δω,
k<sub>ex</sub>}</em>.</li>
- <li><b>'<a href="http://wiki.nmr-relax.com/IT99";>IT99</a>'</b>: The
Ishima and Torchia 1999 2-site model for all time scales with
<em>p<sub>A</sub> » p<sub>A</sub></em> and with parameters
<em>{R<sub>2</sub><sup>0</sup>, ..., Φ<sub>ex</sub>,
p<sub>A</sub>.Δω<sup>2</sup>, k<sub>ex</sub>}</em>.</li>
+ <li><b>'<a href="http://wiki.nmr-relax.com/IT99";>IT99</a>'</b>: The
Ishima and Torchia 1999 2-site model for all time scales with
<em>p<sub>A</sub> » p<sub>B</sub></em> and with parameters
<em>{R<sub>2</sub><sup>0</sup>, ..., Φ<sub>ex</sub>,
p<sub>A</sub>.Δω<sup>2</sup>, k<sub>ex</sub>}</em>.</li>
<li><b>'<a href="http://wiki.nmr-relax.com/TSMFK01";>TSMFK01</a>'</b>:
The Tollinger et al., 2001 2-site very-slow exchange model for time scales
within range of microsecond to second time scale. Applicable in the limit of
slow exchange, when <em>R<sub>2A</sub><sup>0</sup> -
R<sub>2B</sub><sup>0</sup> « k<sub>AB</sub>, k<sub>BA</sub> «
1/τ<sub>CPMG</sub></em>. <em>2*τ<sub>CPMG</sub></em> is the time
between successive 180 degree pulses. The parameters are
<em>{R<sub>2A</sub><sup>0</sup>, ..., Δω, k<sub>AB</sub>}</em>.</li>
</ul>
@@ -78,6 +78,43 @@
<ul>
<li><b>'NS CPMG 2-site expanded'</b>: A model for 2-site exchange
expanded using Maple by Nikolai Skrynnikov (Tollinger et al., 2001). It has
the parameters <em>{R<sub>2</sub><sup>0</sup>, ..., p<sub>A</sub>,
Δω, k<sub>ex</sub>}</em>.</li>
+ <li><b>'NS CPMG 2-site 3D'</b>: The reduced model for 2-site exchange
using 3D magnetisation vectors whereby the simplification
<em>R<sub>2A</sub><sup>0</sup> = R<sub>2B</sub><sup>0</sup></em> is assumed.
It has the parameters <em>{R<sub>2</sub><sup>0</sup>, ..., p<sub>A</sub>,
Δω, k<sub>ex</sub>}</em>.</li>
+ <li><b>'NS CPMG 2-site 3D full'</b>: The reduced model for 2-site
exchange using 3D magnetisation vectors with the parameters
<em>{R<sub>2A</sub><sup>0</sup>, R<sub>2B</sub><sup>0</sup>, ...,
p<sub>A</sub>, Δω, k<sub>ex</sub>}</em>.</li>
+ <li><b>'NS CPMG 2-site star'</b>: The reduced model for 2-site
exchange using complex conjugate matrices whereby the simplification
<em>R<sub>2A</sub><sup>0</sup> = R<sub>2B</sub><sup>0</sup></em> is assumed.
It has the parameters <em>{R<sub>2</sub><sup>0</sup>, ..., p<sub>A</sub>,
Δω, k<sub>ex</sub>}</em>.</li>
+ <li><b>'NS CPMG 2-site star full'</b>: The full model for 2-site
exchange using complex conjugate matrices with the parameters
<em>{R<sub>2A</sub><sup>0</sup>, R<sub>2B</sub><sup>0</sup>, ...,
p<sub>A</sub>, Δω, k<sub>ex</sub>}</em>.</li>
+ </ul>
+
+ <h3>Analytic models for R1rho experiments</h3>
+ <p>The following analytic models are designed for
R<sub>1ρ</sub>-type experiments:</p>
+
+ <ul>
+ <li><b>'<a href="http://wiki.nmr-relax.com/M61";>M61</a>'</b>: The
Meiboom 1961 2-site fast exchange equation for on-resonance data with
parameters <em>{R<sub>1ρ</sub>', ..., Φ<sub>ex</sub>,
k<sub>ex</sub>}</em>.</li>
+ <li><b>'<a href="http://wiki.nmr-relax.com/M61_skew";>M61
skew</a>'</b>: The Meiboom 1961 2-site equation for all time scales with
<em>p<sub>A</sub> » p<sub>B</sub></em> and with parameters
<em>{R<sub>1ρ</sub>', ..., p<sub>A</sub>, Δω,
k<sub>ex</sub>}</em>.</li>
+ <li><b>'<a href="http://wiki.nmr-relax.com/DPL94";>DPL94</a>'</b>: The
Davis et al., 1994 extension of the M61 model for off-resonance data with
parameters <em>{R<sub>1ρ</sub>', ..., Φ<sub>ex</sub>,
k<sub>ex</sub>}</em>.</li>
+ <li><b>'<a href="http://wiki.nmr-relax.com/TP02";>TP02</a>'</b>: The
Trott and Palmer 2002 2-site equation for all time scales with
<em>p<sub>A</sub> » p<sub>B</sub></em> and with parameters
<em>{R<sub>1ρ</sub>', ..., p<sub>A</sub>, Δω,
k<sub>ex</sub>}</em>.</li>
+ <li><b>'<a href="http://wiki.nmr-relax.com/TAP03";>TAP03</a>'</b>: The
Trott et al., 2003 off-resonance 2-site analytic equation for all time scales
with the weak condition <em>p<sub>A</sub> » p<sub>B</sub></em> and with
parameters <em>{R<sub>1ρ</sub>', ..., p<sub>A</sub>, Δω,
k<sub>ex</sub>}</em>.</li>
+ <li><b>'<a href="http://wiki.nmr-relax.com/MP05";>MP05</a>'</b>: The
Miloushev and Palmer 2005 off-resonance 2-site equation for all time scales
with parameters <em>{R<sub>1ρ</sub>', ..., p<sub>A</sub>, Δω,
k<sub>ex</sub>}</em>.</li>
+ </ul>
+
+ <h3>Numeric models for R1rho experiments</h3>
+ <p>The following numeric models are designed for
R<sub>1ρ</sub>-type experiments:</p>
+
+ <ul>
+ <li><b>'<a href="http://wiki.nmr-relax.com/NS_R1rho_2-site";>NS R1rho
2-site</a>'</b>: The model for 2-site exchange using 3D magnetisation
vectors. It has the parameters <em>{R<sub>1ρ</sub>', ...,
p<sub>A</sub>, Δω, k<sub>ex</sub>}</em>.</li>
+ </ul>
+
+ <h3>Analytic models for MMQ-type data</h3>
+ <p>The following analytic models are designed for combined
proton-heteronuclear SQ, ZQ, DQ and MQ (MMQ, or multi-multiple quantum)
CPMG-type experiments:</p>
+
+ <ul>
+ <li><b>'<a href="http://wiki.nmr-relax.com/MQ_CR72";>MQ CR72</a>'</b>:
The Carver and Richards (1972) 2-site model for most time scales expanded for
MQ CPMG data by Korzhnev et al., 2004. It has the parameters
<em>{R<sub>2</sub><sup>0</sup>, ..., p<sub>A</sub>, Δω,
Δω<sup>H</sup>, k<sub>ex</sub>}</em>.</li>
+ </ul>
+
+ <h3>Numeric models for MMQ-type data</h3>
+ <p>The following numeric models are designed for MMQ CPMG-type
experiments:</p>
+
+ <ul>
+ <li><b>'<a href="http://wiki.nmr-relax.com/MMQ_2-site";>MMQ
2-site</a>'</b>: The model for 2-site exchange whereby the simplification
<em>R<sub>2A</sub><sup>0</sup> = R<sub>2B</sub><sup>0</sup></em> is assumed.
It has the parameters <em>{R<sub>2</sub><sup>0</sup>, ..., p<sub>A</sub>,
Δω, Δω<sup>H</sup>, k<sub>ex</sub>}</em>.</li>
</ul>
</div>
r21698 - /website/analyses/relaxation_dispersion.html