Add prefix for footnotes
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@ -415,14 +415,14 @@ The "controlled" DoF of each stage (for instance the $D_y$ direction for the tra
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The translation stage is used to position and scan the sample laterally with respect to the X-ray beam.
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A linear motor was first used to enable fast and accurate scans.
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It was later replaced with a stepper motor and lead-screw, as the feedback control used for the linear motor was unreliable[fn:12].
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It was later replaced with a stepper motor and lead-screw, as the feedback control used for the linear motor was unreliable[fn:ustation_12].
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An optical linear encoder is used to measure the stage motion and for controlling the position.
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Four cylindrical bearings[fn:4] are used to guide the motion (i.e. minimize the parasitic motions) and have high stiffness.
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Four cylindrical bearings[fn:ustation_4] are used to guide the motion (i.e. minimize the parasitic motions) and have high stiffness.
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**** Tilt Stage
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The tilt stage is guided by four linear motion guides[fn:1] which are placed such that the center of rotation coincide with the X-ray beam.
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The tilt stage is guided by four linear motion guides[fn:ustation_1] which are placed such that the center of rotation coincide with the X-ray beam.
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Each linear guide is very stiff in radial directions such that the only DoF with low stiffness is in $R_y$.
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This stage is mainly used in /reflectivity/ experiments where the sample $R_y$ angle is scanned.
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@ -449,13 +449,13 @@ To precisely control the $R_y$ angle, a stepper motor and two optical encoders a
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**** Spindle
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Then, a rotation stage is used for tomography experiments.
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It is composed of an air bearing spindle[fn:2], whose angular position is controlled with a 3 phase synchronous motor based on the reading of 4 optical encoders.
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It is composed of an air bearing spindle[fn:ustation_2], whose angular position is controlled with a 3 phase synchronous motor based on the reading of 4 optical encoders.
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Additional rotary unions and slip-rings are used to be able to pass electrical signals, fluids and gazes through the rotation stage.
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**** Micro-Hexapod
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Finally, a Stewart platform[fn:3] is used to position the sample.
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Finally, a Stewart platform[fn:ustation_3] is used to position the sample.
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It includes a DC motor and an optical linear encoders in each of the six struts.
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This stage is used to position the point of interest of the sample with respect to the spindle rotation axis.
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@ -481,7 +481,7 @@ It can also be used to precisely position the PoI vertically with respect to the
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<<ssec:ustation_motion_description>>
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**** Introduction :ignore:
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In this section, mathematical tools[fn:6] that are used to describe the motion of positioning stages are introduced.
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In this section, mathematical tools[fn:ustation_6] that are used to describe the motion of positioning stages are introduced.
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First, the tools to describe the pose of a solid body (i.e. it's position and orientation) are introduced.
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The motion induced by a positioning stage is described by transformation matrices.
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@ -558,7 +558,7 @@ For rotations along $x$, $y$ or $z$ axis, the formulas of the corresponding rota
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\end{subequations}
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Sometimes, it is useful to express a rotation as a combination of three rotations described by $\bm{R}_x$, $\bm{R}_y$ and $\bm{R}_z$.
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The order of rotation is very important[fn:5], therefore, in this study, rotations are expressed as three successive rotations about the coordinate axes of the moving frame eqref:eq:ustation_rotation_combination.
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The order of rotation is very important[fn:ustation_5], therefore, in this study, rotations are expressed as three successive rotations about the coordinate axes of the moving frame eqref:eq:ustation_rotation_combination.
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\begin{equation}\label{eq:ustation_rotation_combination}
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{}^A\bm{R}_B(\alpha, \beta, \gamma) = \bm{R}_u(\alpha) \bm{R}_v(\beta) \bm{R}_c(\gamma)
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@ -1398,7 +1398,7 @@ Therefore, from a control perspective, they are not important.
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**** Ground Motion
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The ground motion was measured by using a sensitive 3-axis geophone[fn:11] placed on the ground.
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The ground motion was measured by using a sensitive 3-axis geophone[fn:ustation_11] placed on the ground.
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The generated voltages were recorded with a high resolution DAC, and converted to displacement using the Geophone sensitivity transfer function.
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The obtained ground motion displacement is shown in Figure ref:fig:ustation_ground_disturbance.
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@ -1466,7 +1466,7 @@ exportFig('figs/ustation_ground_disturbance.pdf', 'width', 'half', 'height', 450
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**** Ty Stage
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To measure the positioning errors of the translation stage, the setup shown in Figure ref:fig:ustation_errors_ty_setup is used.
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A special optical element (called a "straightness interferometer"[fn:9]) is fixed on top of the micro-station, while a laser source[fn:10] and a straightness reflector are fixed on the ground.
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A special optical element (called a "straightness interferometer"[fn:ustation_9]) is fixed on top of the micro-station, while a laser source[fn:ustation_10] and a straightness reflector are fixed on the ground.
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A similar setup was used to measure the horizontal deviation (i.e. in the $x$ direction), as well as the pitch and yaw errors of the translation stage.
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#+name: fig:ustation_errors_ty_setup
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@ -1564,9 +1564,9 @@ pxx_dy_dx = pxx_dy_dz;
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**** Spindle
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To measure the positioning errors induced by the Spindle, a "Spindle error analyzer"[fn:7] is used as shown in Figure ref:fig:ustation_rz_meas_lion_setup.
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To measure the positioning errors induced by the Spindle, a "Spindle error analyzer"[fn:ustation_7] is used as shown in Figure ref:fig:ustation_rz_meas_lion_setup.
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A specific target is fixed on top of the micro-station, which consists of two sphere with 1 inch diameter precisely aligned with the spindle rotation axis.
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Five capacitive sensors[fn:8] are pointing at the two spheres, as shown in Figure ref:fig:ustation_rz_meas_lion_zoom.
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Five capacitive sensors[fn:ustation_8] are pointing at the two spheres, as shown in Figure ref:fig:ustation_rz_meas_lion_zoom.
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From the 5 measured displacements $[d_1,\,d_2,\,d_3,\,d_4,\,d_5]$, the translations and rotations $[D_x,\,D_y,\,D_z,\,R_x,\,R_y]$ of the target can be estimated.
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#+name: fig:ustation_rz_meas_lion_setup
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@ -2274,7 +2274,7 @@ exportFig('figs/ustation_errors_model_dy_vertical.pdf', 'width', 'half', 'height
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:PROPERTIES:
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:UNNUMBERED: t
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:END:
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<<sec:uniaxial_conclusion>>
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<<sec:ustation_conclusion>>
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In this study, a multi-body model of the micro-station was developed.
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It was difficult to match the measured dynamics obtained from the modal analysis of the micro-station.
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@ -4664,15 +4664,15 @@ Otherwise, when the limbs' lengths derived yield complex numbers, then the posit
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* Footnotes
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[fn:12]It was probably caused by rust of the linear guides along its stroke.
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[fn:11]A 3-Axis L4C geophone manufactured Sercel was used.
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[fn:10]Laser source is manufactured by Agilent (5519b).
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[fn:9]The special optics (straightness interferometer and reflector) are manufactured by Agilent (10774A).
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[fn:8]C8 capacitive sensors and CPL290 capacitive driver electronics from Lion Precision.
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[fn:7]The Spindle Error Analyzer is made by Lion Precision.
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[fn:6]The tools presented here are largely taken from [[cite:&taghirad13_paral]].
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[fn:5]Rotations are non commutative in 3D.
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[fn:4]Ball cage (N501) and guide bush (N550) from Mahr are used.
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[fn:3]Modified Zonda Hexapod by Symetrie.
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[fn:2]Made by LAB Motion Systems.
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[fn:1]HCR 35 A C1, from THK.
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[fn:ustation_12]It was probably caused by rust of the linear guides along its stroke.
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[fn:ustation_11]A 3-Axis L4C geophone manufactured Sercel was used.
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[fn:ustation_10]Laser source is manufactured by Agilent (5519b).
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[fn:ustation_9]The special optics (straightness interferometer and reflector) are manufactured by Agilent (10774A).
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[fn:ustation_8]C8 capacitive sensors and CPL290 capacitive driver electronics from Lion Precision.
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[fn:ustation_7]The Spindle Error Analyzer is made by Lion Precision.
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[fn:ustation_6]The tools presented here are largely taken from [[cite:&taghirad13_paral]].
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[fn:ustation_5]Rotations are non commutative in 3D.
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[fn:ustation_4]Ball cage (N501) and guide bush (N550) from Mahr are used.
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[fn:ustation_3]Modified Zonda Hexapod by Symetrie.
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[fn:ustation_2]Made by LAB Motion Systems.
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[fn:ustation_1]HCR 35 A C1, from THK.
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