Running the application » History » Version 18
Anchi Cheng, 07/15/2010 09:40 PM
1 | 1 | Amber Herold | h1. Running the application |
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5 | h2. Import Notes about Image Intensity Recorded through |
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6 | Tomography Node |
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10 | 14 | Amber Herold | Tomography node saves the images in a different format from other Acquisition nodes. By |
11 | 1 | Amber Herold | default, the flat-field correct CCD counts are multiplied by 10 and converted to signed |
12 | 16-bit integer before the image is displayed and saved. This makes CCD counts of 3276.8 or |
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13 | larger overflow to negatives. Other Leginon Acquisition images are saved as float without |
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14 | manipulation. |
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17 | To avoid this problem, find out what exposure time corresponds to the fractionated dose |
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18 | from your tilt angle step and range and total dose and take an image at tomo preset with |
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19 | such an exposure in Navigation node. You will need to reduce the total dose if a good |
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20 | fraction of the counts are larger than 3200 even though it would not appear to be saturated |
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21 | in the float scale without the 10x factor. Alternatively, change the scale factor in |
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22 | Tomography node. |
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28 | h2. Multiscale Imaging |
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32 | * Preset image shift alignment/beam shift alignment are the same as in MSI |
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33 | application |
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36 | 5 | Amber Herold | * New dark/bright references should be reacquired for "tomo" preset that acquires the |
37 | 1 | Amber Herold | final data. It is best to do this at the same dose per tomography image calculated from |
38 | the total dose, the tilt parameters, and the dose measurement. |
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41 | * For best focusing result, perform autofocus at the same magnification as the |
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42 | tomography data collection, align microscope well at the eucentric focus and the |
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43 | rotation center and save them before data collection. |
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51 | h2. Using Tomography Preview |
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55 | * Preview targets (pink) can be selected when selecting targets in "Tomography |
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56 | Targeting" |
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59 | * When the targets are processed, targets that are of the type "preview" are |
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60 | processed before focus and acquisition targets. |
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62 | |||
63 | * Tomography Preview node acquires a image at the preview target using "preview" |
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64 | preset which should be set at minimal dose. |
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72 | h2. Dose Measurement |
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76 | If "Measure Dose before collection" is checked in Tomography node, the stage will be |
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77 | moved to the reference target and a dose image of the "tomo" preset will be acquired (center |
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78 | 512x512 of whateven binning of the preset) before each tilt series if the interval between |
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79 | the series is longer than the limit time set in the settings of Dose Measurement node. The |
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80 | measured value will then be used to recalculate the proper exposure time for tomography |
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81 | imaging. |
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84 | For this function to behave properly, the followings should be done during |
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85 | operation: |
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88 | * One, and only one, "reference" target should be selected in either "Square |
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89 | Targeting" or "Hole Targeting" or "Tomography Targeting" node. The reference target |
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90 | should be of either a broken square or a empty hole if no broken square can be |
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91 | found. |
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94 | * "Measure Dose" before collection should be selected in Tomography node. |
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97 | * "Exposure time max/min" in Tomography node should be in a range that can accommodate |
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98 | the electron beam fluctuation over time. |
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106 | h2. Align Zero Loss Peak |
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110 | This function applies only to Gatan energy filter EFTEM. If "Align ZLP before |
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111 | collection" is checked in Tomography node, the stage will be moved to the reference target |
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112 | and starts the procedure to align zero loss peak before each tilt series if the interval |
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113 | between the series is longer than the limit time set in the settings of Dose Measurement |
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114 | node. |
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116 | |||
117 | For this function to behave properly, the followings should be done during |
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118 | operation: |
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120 | |||
121 | * One, and only one, "reference" target should be selected in either "Square |
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122 | Targeting" or "Hole Targeting" or "Tomography Targeting" node. The reference target |
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123 | should be of either a broken square or a empty hole if no broken square can be found. |
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124 | This is the same reference target used for dose measurement. |
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127 | * "Align ZLP" before collection should be selected in Tomography node. |
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135 | h2. Low Magnification Model Fitting |
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139 | The fitting of optical axis offset does not always works if the offset is so large that |
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140 | the feature moves out of view with even a small tilt. In such a case, it is worth first |
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141 | collect a tomography series at a lower magnification to define roughly the model. |
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144 | At beginning of each session, or forced by the user, the model is initialized. By |
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145 | default, at the initialization, Tomography node uses past fitting results that show good |
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146 | agreement with the experimental data at the magnification of the preset used. If a good |
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147 | model is not found, that from lower magnifications will be used. It is possible to force the |
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148 | node to use a model fitted at a particular magnification by selecting it in |
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149 | Tomography/Settings/Model. |
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152 | Therefore, we recommend that, in case of fitting failure on good contrast images, the |
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153 | followings should be done: |
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156 | 3 | Amber Herold | # Tomography/Settings/Image Acquisition> change the preset to "hl". |
157 | # Tomography/Settings> adjust Tilt and Exposure parameters to match. |
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158 | # Acquire the tiltseries images. |
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159 | # If the tracking is good, change the preset back. |
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160 | # Tomography/Settings/Model> Initialize with the model of (the mag of "hl" |
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161 | 1 | Amber Herold | preset). |
162 | 3 | Amber Herold | # Acquire the tomo-series. |
163 | # If tracking is good, change back to Initialize with the model of "this preset and |
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164 | 1 | Amber Herold | lower" mag. |
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172 | h2. What is a Good Tilt-Axis Model? |
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176 | 5 | Amber Herold | The goniometer-tilt-axis-based tracking model developed by Zheng et. al. corrects the |
177 | specimen height (z-axis) by a change of defocus using measured shift of feature shifts in |
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178 | 1 | Amber Herold | the images (x and y-axes). The tracking in the x and y directions does not involve the use |
179 | 5 | Amber Herold | of such model, but is done by smooth curve fitting or preceding tilts. Therefore, to judge |
180 | 1 | Amber Herold | the adequacy of the model, one should check the resulting defocii of the images in the |
181 | series remain unchanged. |
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184 | On the other hand, the feature tracking in x and y is likely to fail only if the tilting |
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185 | does not induce a smooth shift of the imaging feature a sudden drop of specimen position at |
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186 | a particular tilt angle often throws off the smooth curve fitting. It is possible to reduce |
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187 | such effect by increasing the number of data points included in the smoothing as set in the |
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188 | model section of the tomography node settings window. Otherwise, the goniometer need to be |
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189 | serviced. |
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191 | 18 | Anchi Cheng | [[Tomography Trouble Shooting]] |
192 | 1 | Amber Herold | |
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196 | h2. Failure of xy feature tracking |
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200 | 9 | Amber Herold | Feature tracking in x and y axes is a 2nd order polynomial fit of preceeding data |
201 | 1 | Amber Herold | points. The default uses 5 data points. When a sudden jump occurs in the tracking error, it |
202 | tend to follow the trend of the last point. If the jump is a temporary clich in the |
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203 | goniometer, this tend to over correct the tracking error and eventually loose track as shown |
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204 | in Figure 5. A possible fix is to increase the number of data points in the fitting. This |
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205 | can be set in the tomography setting "Smooth n tilts for defocus prediction". 4 in defocus |
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206 | prediction is equivalent to 5 points (n+1) for xy tracking. |
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209 | 6 | Amber Herold | *Figure 5* |
210 | !http://emg.nysbc.org/software/leginon/images/images/tomoxbad.png! |
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211 | 1 | Amber Herold | |
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216 | h2. Large tracking error between the first and second tilt |
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217 | images |
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221 | The first image in each tilt group of the tilt series at the "start" angle (normally 0 |
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222 | deg) and the second image at tilt of "step" angle from the "start" angle do not use the |
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223 | fitted model. It is assumed that the eucentric height judged by stage alpha wobbling in the |
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224 | "Tomo Focus" node gives a stage height that the tracking of feature by such a small tilt |
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225 | would be good enough. In most cases this is a reasonable assumption. However, we have had |
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226 | experience of goniometer alignment problem where the assumption fails. The symptom is |
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227 | illustrated in Figure 6 below. Note that the Feature tracking error is displayed as |
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228 | percentage of the image length. |
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231 | 6 | Amber Herold | *Figure 6* |
232 | !http://emg.nysbc.org/software/leginon/images/images/tomoz0bad.png! |
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233 | 1 | Amber Herold | |
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235 | 11 | Amber Herold | This tilt series was taken with a starting angle of zero and at an image size of < 1 |
236 | um. As can be seen here, apart from the 2 and minus 2 degree tilts, the tracking error was less |
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237 | 8 | Amber Herold | than 2 % of the image. Only the tracking of the feature between 0 and +/- 2 degrees are |
238 | 11 | Amber Herold | large. At close to 20 % error, this made the overlap between plus and minus 2 degrees unacceptable and |
239 | 1 | Amber Herold | often cause popular alignment programs to misalign the two half of the series. |
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241 | |||
242 | The first solution is of course to report it to your microscope service engineer. When |
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243 | we had this problem, many users noticed that it was difficult to adjust stage to eucentric |
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244 | height manually with alpha wobbler. Features jumped while the goniometer changed rotation |
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245 | direction. In addition, different magnitude of tilt range suggests different eucentric |
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246 | heights. It is not easy to fix this, so it might take a while. |
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249 | Before the hardware is fixed physically, it is still possible collect tomograms. The |
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250 | model fitting of the overall curve in the above case gave z0 of +5 um through the whole tilt |
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251 | series (Figure not shown). Therefore, by moving the stage up by such an amount after the |
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252 | stage-tilt-based autofocusing can bring us to the correct height for tomography. This can |
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253 | be acheived by saving the "tomo eucentric" focus current to the database, align rotation |
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254 | center for this stage height and focus. Then change the correction type of the |
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255 | "Beam_Tilt_Fine" focusing step to "Stage Z". |
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261 | h2. Failure of model-based correction |
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265 | The model used in the defocus correction in Leginon tomography node is a very simplified |
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266 | one. There are a few cases when the approach fails. Here are ones that we have |
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267 | encountered: |
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271 | h2. Y-axis looping |
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274 | |||
275 | The microscope goniometer does not move on only the tilt axis. With its complex |
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276 | structure, a common problem is that when the stage is highly tilt, the position slips in |
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277 | the y-direction. This is known as looping. Figure 7 shows an example of this problem. |
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280 | 6 | Amber Herold | *Figure 7* |
281 | !http://emg.nysbc.org/software/leginon/images/images/tomoxyloop.png! |
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282 | 1 | Amber Herold | |
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284 | While the x-axis position shifts monotonically as a stable model should be, the y-axis |
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285 | in the positive tilt direction changes little from 0-30 degrees before it increases |
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286 | rapidly after 30 degrees. Even though the tracking in xy plane is still good, the defocii |
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287 | correction at these higher tilts may no longer be correct if the tilt axis parameters are |
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288 | fitted dynamically. Figure 8 shows the model parameters of the same tilt series where the |
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289 | fitted phi and offset starts to change above 30 degrees even though the tilt axis has not |
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290 | moved according to the shrinking behavior of the images during the tilts. Note that in |
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291 | this particular case the looping problem is still mild so that the over-correction is not |
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292 | very strong. only a small slope change is resulted in z0 prediction. In worst cases, the |
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293 | defocus over-correction is so large that the adjacent images can not correlate properly |
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294 | and even the xy tracking would fail. The spikes around zero tilt is a display data sorting |
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295 | error of the identical starting tilt of the two tilt groups. |
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296 | |||
297 | |||
298 | 6 | Amber Herold | *Figure 8* |
299 | !http://emg.nysbc.org/software/leginon/images/images/tomomodelloop.png! |
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300 | 1 | Amber Herold | |
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302 | Other than asking microscope service engineer to fix the looping, one can find the |
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303 | best fixed model in the series to apply to future tilt data collection. To make the fixed |
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304 | model permantly saved to the database, follow these steps: |
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307 | 12 | Amber Herold | # tomography/settings/model>activate "keep the tilt axis parameters |
308 | 1 | Amber Herold | fixed". |
309 | 12 | Amber Herold | # tomography/settings/model>initialize the model with "custom values". Enter best |
310 | 1 | Amber Herold | estimate of the fixed model. For example, in the positive direction, enter phi as |
311 | -2.17 degrees and axis offset as -1.52 um. since these are the stable values up to the |
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312 | point the y-looping starts. |
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313 | 12 | Amber Herold | # tomography>collect a full tilt series. If the run is successful with good |
314 | 1 | Amber Herold | tracking in all three axis, the model will be saved in the database for this |
315 | magnification. |
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316 | 12 | Amber Herold | # tomography/settings/model>From now on, you can initialize the model with "only |
317 | 1 | Amber Herold | this preset" or "this preset and lower mags" |
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324 | |||
325 | h2. Grid slips between the first and second tilt directions |
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329 | When the holder does not hold the grid tightly, the grid slips to a different position |
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330 | when the first tilt direction ends and the goniometer quickly returns to zero tilt. |
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331 | Leginon is designed to adjust the target before the second tilt group starts. The default |
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332 | setting for this function is to use only the parent image (i.e. one ancestor) where the |
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333 | target comes from as reference. If the slip is larger than the size of the parent image, |
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334 | the adjustment may fail, and a random target would be acquired in the second tilt |
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335 | group. |
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338 | Starting from Leginon 1.6, the target adjustment can be done with all ancestor images |
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339 | of the target by choosing "all" in the acquisition part of the tomography node setting to |
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340 | 12 | Amber Herold | adjust target with all ancestors. The node "Target Adjustment" limits the lowest |
341 | 1 | Amber Herold | magnification that this target adjustment would go up in ancestry. The default is at 300x |
342 | 12 | Amber Herold | so that the presence of the objective aperture does not create difference in the reacquired |
343 | 1 | Amber Herold | ancestor image from its original. |
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349 | h2. Strong and continuous specimen drift |
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353 | The model used in Leginon considers any shift of feature in the image a result of tilt |
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354 | axis not aligning to the center of the detector. With the phi and offset fixed, all errors |
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355 | are accumulated in z0 and results in bad defocus correction. There is no solution to this |
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356 | at the moment. |
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357 | 13 | Amber Herold | |
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360 | |||
361 | ______ |
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362 | |||
363 | [[Set-up Before Running|< Set-up Before Running]] | [[Full Protocol on a F30 with an energy filter| Full Protocol on a F30 with an energy filter >]] |