diff --git a/doc/html/user/MUSR/BmwLibs.html b/doc/html/user/MUSR/BmwLibs.html index 07f65b82..ef36899f 100644 --- a/doc/html/user/MUSR/BmwLibs.html +++ b/doc/html/user/MUSR/BmwLibs.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -151,7 +151,7 @@ pre {

- +

diff --git a/doc/html/user/MUSR/LibFitPofB.html b/doc/html/user/MUSR/LibFitPofB.html index 1b9d1aa7..53968165 100644 --- a/doc/html/user/MUSR/LibFitPofB.html +++ b/doc/html/user/MUSR/LibFitPofB.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -427,7 +427,7 @@ An example XML file looks as follows:

- +

diff --git a/doc/html/user/MUSR/LibZFRelaxation.html b/doc/html/user/MUSR/LibZFRelaxation.html index 89bd984a..aaef9b6d 100644 --- a/doc/html/user/MUSR/LibZFRelaxation.html +++ b/doc/html/user/MUSR/LibZFRelaxation.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -232,7 +232,7 @@ The parameters are:

    - +

    diff --git a/doc/html/user/MUSR/Msr2Data.html b/doc/html/user/MUSR/Msr2Data.html index 9ad2bccc..803fbd06 100644 --- a/doc/html/user/MUSR/Msr2Data.html +++ b/doc/html/user/MUSR/Msr2Data.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -392,7 +392,7 @@ For reporting bugs or requesting new features and improvements please use the

    - +

    diff --git a/doc/html/user/MUSR/MusrFit.html b/doc/html/user/MUSR/MusrFit.html index ea29b5cd..6614eab1 100644 --- a/doc/html/user/MUSR/MusrFit.html +++ b/doc/html/user/MUSR/MusrFit.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -583,7 +583,7 @@ The THEORY block is used to define the fit function. There is a set of predefine ab \sigma\,(\mu\text{s}^{-1}), \gamma\,(\mathrm{MHz}) \exp\left[-\frac{\sigma^2}{\gamma^2}\left(e^{-\gamma t}-1+\gamma t\right)\right] - dead! + dead! skewedGss @@ -592,6 +592,34 @@ The THEORY block is used to define the fit function. There is a set of predefine \frac{\sigma_{-}}{\sigma_{+}+\sigma_{-}}\exp\left[-\frac{\sigma_{-}^2t^2}{2}\right]\left\lbrace\cos\left(2\pi\nu t+\frac{\pi\varphi}{180}\right)+\sin\left(2\pi\nu t+\frac{\pi\varphi}{180}\right)\mathrm{Erfi}\left(\frac{\sigma_{-}t}{\sqrt{2}}\right)\right\rbrace+ \frac{\sigma_{+}}{\sigma_{+}+\sigma_{-}}\exp\left[-\frac{\sigma_{+}^2t^2}{2}\right]\left\lbrace\cos\left(2\pi\nu t+\frac{\pi\varphi}{180}\right)-\sin\left(2\pi\nu t+\frac{\pi\varphi}{180}\right)\mathrm{Erfi}\left(\frac{\sigma_{+}t}{\sqrt{2}}\right)\right\rbrace     memo pdf + + staticNKZF + snkzf + \Delta_0\,(\mu\text{s}^{-1}), R_b\,(\text{1}) + \frac{1}{3}+\frac{2}{3}\left(\frac{1+R_b^2}{1+R_b^2+R_b^2\Delta_0^2(1+R_b^2)t^2}\right)^{3/2} \left(1-\frac{\Delta_0^2 t^2}{1+R_b^2+R_b^2\Delta_0^2(1+R_b^2)t^2}\right)\,\exp\left[-\frac{\Delta_0^2 t^2}{2(1+R_b^2+R_b^2\Delta_0^2(1+R_b^2)t^2)}\right] + Phys. Rev. B 56 (1997) 2352; A. Yaouanc and P. Dalmas de Réotier "Muon Spin Rotation, Relaxation, and Resonance" Oxford Scientific Publication ">(10) + + + staticNKTF + snktf + \varphi\,(^{\circ}), \nu\,(\mathrm{MHz}), \Delta_0\,(\mu\text{s}^{-1}), R_b\,(\text{1}) + \sqrt{\frac{1+R_b^2}{1+R_b^2+R_b^2\Delta_0^2(1+R_b^2)t^2}}\,\exp\left[-\frac{\Delta_0^2 t^2}{2(1+R_b^2+R_b^2\Delta_0^2(1+R_b^2)t^2)}\right]\,\cos(\nu t+\varphi) + see note 10 + + + dynamicNKZF + dnkzf + \Delta_0\,(\mu\text{s}^{-1}), R_b\,(\text{1}), \nu_c\,(\text{MHz}) + \sqrt{\frac{1+R_b^2}{1+R_b^2+4 R_b^2\Delta_0^2(1+R_b^2) \Theta(t)}}\,\exp\left[-\frac{2 \Delta_0^2 (1+R_b^2) \Theta(t)}{1+R_b^2+4 R_b^2\Delta_0^2(1+R_b^2)\Theta(t)}\right]\quad,\, \Theta(t) = \frac{\exp(-\nu_c t) - 1 - \nu_c t}{\nu_c^2} + see note 10 + + + dynamicNKTF + dnktf + \varphi\,(^{\circ}), \nu\,(\mathrm{MHz}), \Delta_0\,(\mu\text{s}^{-1}), R_b\,(\text{1}), \nu_c\,(\text{MHz}) + \sqrt{\frac{1+R_b^2}{1+R_b^2+2 R_b^2\Delta_0^2(1+R_b^2) \Theta(t)}}\,\exp\left[-\frac{\Delta_0^2 (1+R_b^2) \Theta(t)}{1+R_b^2+2 R_b^2\Delta_0^2(1+R_b^2)\Theta(t)}\right]\, \cos(\nu t + \varphi) \quad,\, \Theta(t) = \frac{\exp(-\nu_c t) - 1 - \nu_c t}{\nu_c^2} + see note 10 + polynom p @@ -632,6 +660,8 @@ Notes

    9 : R. E. Turner and D. R. Harshman, Phys. Rev. B 34 (1986) 4467

    + 10 : D.R. Noakes and G.M. Kalvius, Phys. Rev. B 56 (1997) 2352; A. Yaouanc and P. Dalmas de Réotier "Muon Spin Rotation, Relaxation, and Resonance" Oxford Scientific Publication +

    @@ -949,7 +979,7 @@ The last accepted command in the COMMAND block is SCALE_N0_BKG TRUE | FA The Fourier transform is done and the results are plotted within musrview —as input data the actual data shown in musrview is used. In the FOURIER block of the msr file all necessary parameters for calculating and presenting the Fourier transform of the data specified in the PLOT block is given. If the FOURIER block is not present in the msr file, either the parameters set in the XML startup file or the system defaults are taken when the Fourier transform is performed. The block starts with the FOURIER keyword and may contain the following entries on the successive lines:
    units
    Here is specified in which domain the Fourier-transformed data is presented. One may choose between the field (Gauss), the frequency (MHz), and the angular-frequency domain (Mc/s).
    fourier_power
    It is possible (but not necessary) to set the number of data points used for the Fourier transform here. As argument the exponent n<21 of a power of 2 is accepted. The number of data points is then 2n. Attention: If the number of points given here is bigger than the actual number of available data points, the input data vector is filled with zeros until the number of requested points is reached (zero padding)! -
    apodization
    Here is decided if the data should be apodized before the Fourier transform is done and if yes, which apodization should be usedthe PhD thesis of T.M. Riseman <span class="foswikiIcon">pdf">(10). The argument to be put after the keyword is therefore one of the following: NONE, WEAK, MEDIUM or STRONG. If the data should be apodized, they are manipulated as follows: each data value is multiplied by the function \sum_{j=0}^4 c_j \left(\frac{i}{n}\right)^{2j}, where i is the data-point index and n is the total number of data points. The coefficients c_j for the different apodizations are given by:
    +
    apodization
    Here is decided if the data should be apodized before the Fourier transform is done and if yes, which apodization should be usedthe PhD thesis of T.M. Riseman <span class="foswikiIcon">pdf">(10). The argument to be put after the keyword is therefore one of the following: NONE, WEAK, MEDIUM or STRONG. If the data should be apodized, they are manipulated as follows: each data value is multiplied by the function \sum_{j=0}^4 c_j \left(\frac{i}{n}\right)^{2j}, where i is the data-point index and n is the total number of data points. The coefficients c_j for the different apodizations are given by:
    WEAK
    c_0 = 1,\, c_1 = -1.319391,\, c_2 = 0.703484,\, c_3=c_4=0
    MEDIUM
    c_0 = 1,\, c_1 = -1.831292,\, c_2 = 0.983734,\, c_3=c_4=0
    STRONG
    c_0 = 1,\, c_1 = -2.708894,\, c_2 = 2.953575,\, c_3=-1.599128,\, c_4=0.399782 @@ -982,7 +1012,7 @@ Altogether, a possible FOURIER block might look like that:

    Notes

    - 10 : For further details about apodization of μSR data refer to the PhD thesis of T.M. Riseman pdf + 10 : For further details about apodization of μSR data refer to the PhD thesis of T.M. Riseman pdf

    @@ -1449,7 +1479,7 @@ For reporting bugs or requesting new features and improvements please use the

    - +

    diff --git a/doc/html/user/MUSR/MusrFitAcknowledgements.html b/doc/html/user/MUSR/MusrFitAcknowledgements.html index 1d6de3bf..abb5d2c1 100644 --- a/doc/html/user/MUSR/MusrFitAcknowledgements.html +++ b/doc/html/user/MUSR/MusrFitAcknowledgements.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -149,7 +149,7 @@ pre {

    - +

    diff --git a/doc/html/user/MUSR/MusrFitSetup.html b/doc/html/user/MUSR/MusrFitSetup.html index 99716d81..1df36b92 100644 --- a/doc/html/user/MUSR/MusrFitSetup.html +++ b/doc/html/user/MUSR/MusrFitSetup.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -339,7 +339,7 @@ musrview test-histo-ROOT-NPP.msr

    Notes

    -     1 : In case only a single user is working at the machine it might be considerable to change the ownership of the ROOT folder so that the user has easy write access to this directory: + 1 : In case only a single user is working at the machine it might be considerable to change the ownership of the ROOT folder so that the user has easy write access to this directory:

    2 : When using GCC ≥ 4.2 please make sure that the environment variables USE_PARALLEL_MINUIT2 and USE_OPENMP are not set! Otherwise MINUIT2 will be compiled with parallelization support and cannot be used together with musrfit afterwards since the musrfit code is not fully thread-safe! When compiled with GCC ≥ 4.2 musrfit itself will parallelize the χ2 calculation.

    @@ -825,7 +825,7 @@ musrview test-histo-ROOT-NPP.msr

    - +

    diff --git a/doc/html/user/MUSR/MusrGui.html b/doc/html/user/MUSR/MusrGui.html index d3750609..10881c2a 100644 --- a/doc/html/user/MUSR/MusrGui.html +++ b/doc/html/user/MUSR/MusrGui.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -477,7 +477,7 @@ For reporting bugs or requesting new features and improvements please use the

    - +

    diff --git a/doc/html/user/MUSR/QuickStart.html b/doc/html/user/MUSR/QuickStart.html index 80689e6b..287ab661 100644 --- a/doc/html/user/MUSR/QuickStart.html +++ b/doc/html/user/MUSR/QuickStart.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -287,7 +287,7 @@ RUN 2008/lem08_his_8472 MUE4 PSI ROOT-NPP (name beamline institute dat

    - +

    diff --git a/doc/html/user/MUSR/TutorialSingleHisto.html b/doc/html/user/MUSR/TutorialSingleHisto.html index 855623cb..77269d6f 100644 --- a/doc/html/user/MUSR/TutorialSingleHisto.html +++ b/doc/html/user/MUSR/TutorialSingleHisto.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -374,7 +374,7 @@ This page only summarizes the very basic features and options of the programs co

    - +

    diff --git a/doc/html/user/MUSR/WebHome.html b/doc/html/user/MUSR/WebHome.html index 9ea36191..eb427c93 100644 --- a/doc/html/user/MUSR/WebHome.html +++ b/doc/html/user/MUSR/WebHome.html @@ -1,7 +1,7 @@ - + @@ -21,7 +21,7 @@ - + @@ -139,7 +139,7 @@ pre {
  1. Acknowledgements

    2. --- AS & BMW - last update May 25, 2012 +-- AS & BMW - last update May 31, 2012

    @@ -162,7 +162,7 @@ pre {

    - +

    diff --git a/doc/html/user/pub/System/PatternSkinTheme2009/style.css b/doc/html/user/pub/System/PatternSkinTheme2009/style.css index df75ca68..1f5799e2 100644 --- a/doc/html/user/pub/System/PatternSkinTheme2009/style.css +++ b/doc/html/user/pub/System/PatternSkinTheme2009/style.css @@ -23,8 +23,6 @@ html body { font-family:arial, verdana, sans-serif; font-size:104%; - voice-family:"\"}\""; - voice-family:inherit; font-size:small; } html>body { /* Mozilla */