[med-svn] [python-mne] 184/376: fixing manual

Yaroslav Halchenko debian at onerussian.com
Fri Nov 27 17:22:33 UTC 2015


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yoh pushed a commit to annotated tag v0.1
in repository python-mne.

commit 62e89f5d7f5dc8c51bda9378c7c62b68f839b173
Author: Emily Ruzich <emilyr at nmr.mgh.harvard.edu>
Date:   Tue Apr 5 14:45:41 2011 -0400

    fixing manual
---
 doc/source/manual/browse.rst   | 38 +++++++++++++++++++-------------------
 doc/source/manual/cookbook.rst | 13 +++++++------
 2 files changed, 26 insertions(+), 25 deletions(-)

diff --git a/doc/source/manual/browse.rst b/doc/source/manual/browse.rst
index 4c94d4e..7a1a4e2 100755
--- a/doc/source/manual/browse.rst
+++ b/doc/source/manual/browse.rst
@@ -2371,13 +2371,13 @@ Without loss of generality we can always decompose any INLINE_EQUATION-channel
 measurement INLINE_EQUATION into its signal and
 noise components as
 
-.. math::    1 + 1 = 2
+.. math::    b(t) = b_s(t) + b_n(t)
 
 Further, if we know that INLINE_EQUATION is
 well characterized by a few field patterns INLINE_EQUATION,
 we can express the disturbance as
 
-.. math::    1 + 1 = 2
+.. math::    b_n(t) = Uc_n(t) + e(t)\ ,
 
 where the columns of INLINE_EQUATION constitute
 an orthonormal basis for INLINE_EQUATION, INLINE_EQUATION is
@@ -2390,11 +2390,11 @@ a small basis set INLINE_EQUATION such that the
 conditions described above are satisfied. We can now construct the
 orthogonal complement operator
 
-.. math::    1 + 1 = 2
+.. math::    P_{\perp} = I - UU^T
 
 and apply it to INLINE_EQUATION yielding
 
-.. math::    1 + 1 = 2
+.. math::    b(t) = P_{\perp}b_s(t)\ ,
 
 since INLINE_EQUATION. The projection operator INLINE_EQUATION is
 called the signal-space projection operator and generally provides
@@ -2458,16 +2458,16 @@ software employs the average-electrode reference, which means that
 the average over all electrode signals INLINE_EQUATION is
 subtracted from each INLINE_EQUATION:
 
-.. math::    1 + 1 = 2
+.. math::    v_{j}' = v_j - \frac{1}{p} \sum_{k} v_k\ .
 
 It is easy to see that the above equation actually corresponds
 to the projection:
 
-.. math::    1 + 1 = 2
+.. math::    v' = (I - uu^T)v\ ,
 
 where
 
-.. math::    1 + 1 = 2
+.. math::    u = \frac{1}{\sqrt{p}}[1\ ...\ 1]^T\ .
 
 .. _CACHAAEG:
 
@@ -2486,11 +2486,11 @@ accepted INLINE_EQUATION samples from all channels to
 the vectors INLINE_EQUATION. The estimate of the covariance
 matrix is then computed as:
 
-.. math::    1 + 1 = 2
+.. math::    \hat{C} = \frac{1}{M - 1} \sum_{j = 1}^M {(s_j - \bar{s})(s_j - \bar{s})}^T
 
 where
 
-.. math::    1 + 1 = 2
+.. math::    \bar{s} = \frac{1}{M} \sum_{j = 1}^M s_j
 
 is the average of the signals over all times. Note that no
 attempt is made to correct for low frequency drifts in the data.
@@ -2501,7 +2501,7 @@ applied.
 For actual computations, it is convenient to rewrite the
 expression for the covariance matrix as
 
-.. math::    1 + 1 = 2
+.. math::    \hat{C} = \frac{1}{M - 1} \sum_{j = 1}^M {s_j s_j^T} - \frac{M}{M - 1} \bar{s} \bar{s}^T
 
 .. _BABHJDEJ:
 
@@ -2515,7 +2515,7 @@ epoch.
 
 Let the vectors
 
-.. math::    1 + 1 = 2
+.. math::    s_{rpj}\ ,\ p = 1\ ...\ P_r\ ,\ j = 1\ ...\ N_r\ ,\ r = 1\ ...\ R 
 
 be the samples from all channels in the baseline corrected epochs
 used to calculate the covariance matrix. In the above, INLINE_EQUATION is
@@ -2529,31 +2529,31 @@ correction is applied to the epochs but the means at individual
 samples are not subtracted. Thus the covariance matrix will be computed
 as:
 
-.. math::    1 + 1 = 2
+.. math::    \hat{C} = \frac{1}{N_C} \sum_{r,p,j} {s_{rpj} s_{rpj}^T}\ ,
 
 where
 
-.. math::    1 + 1 = 2
+.. math::    N_C = \sum_{r = 1}^R N_r P_r\ .
 
 If keepsamplemean is *not* specified,
 we estimate the covariance matrix as
 
-.. math::    1 + 1 = 2
+.. math::    \hat{C} = \frac{1}{N_C} \sum_{r = 1}^R \sum_{j = 1}^{N_r} \sum_{p = 1}^{P_r} {(s_{rpj} - \bar{s_{rj}}) ((s_{rpj} - \bar{s_{rj}})^T}\ ,
 
 where
 
-.. math::    1 + 1 = 2
+.. math::    \bar{s_{rj}} = \frac{1}{P_r} \sum_{p = 1}^{P_r} s_{rpj}
 
 and
 
-.. math::    1 + 1 = 2
+.. math::    N_C = \sum_{r = 1}^R {N_r (P_r - 1)}\ ,
 
 which reflects the fact that INLINE_EQUATION means
 are computed for category INLINE_EQUATION. It
 is easy to see that the expression for the covariance matrix estimate
 can be cast into a more convenient form
 
-.. math::    1 + 1 = 2
+.. math::    \hat{C} = \frac{1}{N_C} \sum_{r,p,j} {s_{rpj} s_{rpj}^T} - \frac{1}{N_C} \sum_r P_r \sum_j {\bar{s_{rj}} \bar{s_rj}^T}/ .
 
 Subtraction of the means at individual samples is useful
 if it can be expected that the evoked response from previous stimulus
@@ -2567,11 +2567,11 @@ estimates INLINE_EQUATION with corresponding degrees
 of freedom INLINE_EQUATION. We can combine these
 matrices together as
 
-.. math::    1 + 1 = 2
+.. math::    C = \sum_q {\alpha_q \hat{C}_q}\ ,
 
 where
 
-.. math::    1 + 1 = 2
+.. math::    \alpha_q = \frac{N_q}{\sum_q {N_q}}\ .
 
 SSP information included with covariance matrices
 =================================================
diff --git a/doc/source/manual/cookbook.rst b/doc/source/manual/cookbook.rst
index 14282a9..2fdad48 100755
--- a/doc/source/manual/cookbook.rst
+++ b/doc/source/manual/cookbook.rst
@@ -815,14 +815,15 @@ anatomy only, not on the MEG/EEG data to be analyzed.
 
 .. note:: The MEG head to MRI transformation matrix specified    with the ``--trans`` option should be a text file containing    a 4-by-4 matrix:
 
-.. math::    T = \[
+.. math::    \[
+		T=
 		\begin{matrix}
-		R_11 & R_12 & R_13 x_0 \\
-		R_13 & R_13 & R_13 y_0 \\
-		R_13 & R_13 & R_13 z_0 \\
-		0 & 0 & 0 & 1 \\
+		R_{11} & R_{12} & R_{13} x_{0} \\
+		R_{13} & R_{13} & R_{13} y_{0} \\
+		R_{13} & R_{13} & R_{13} z_{0} \\
+		0 & 0 & 0 & 1
 		\end{matrix}
-		\]
+	      \]
 
 defined so that if the augmented location vectors in MRI
 head and MRI coordinate systems are denoted by :math:`r_{head}[x_{head}\ y_{head}\ z_{head}\ 1]` and :math:`r_{MRI}[x_{MRI}\ y_{MRI}\ z_{MRI}\ 1]`,

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