Mechatronic design of a 3 DOF long stroke motion stage

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Last updated 10:08 AM on 8/4/26
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19 Terms

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  • particles on the reticle - repeat for each die on the wafer

  • particles on the wafer - can kill the action of dies

<ul><li><p>particles on the reticle - repeat for each die on the wafer</p></li><li><p>particles on the wafer - can kill the action of dies</p></li></ul><p></p>
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current state-of-the-art

+high resolution inspection and metrology capabilities

-slow, limited to small areas of interest

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challenges of SEM

  • high resolution → smaller field of view

  • high vacuum environment

  • very sensitive to variations in external magnetic field

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LoS - SS concept

  • inside the vacuum chamber

  • Lorentz actuator in SS

  • linear roller guides in LoS

  • active cooling with water

  • magnetic fields

→ costs

<ul><li><p>inside the vacuum chamber</p></li><li><p>Lorentz actuator in SS</p></li><li><p>linear roller guides in LoS</p></li><li><p>active cooling with water</p></li><li><p>magnetic fields</p></li></ul><p></p><p>→ costs</p><p></p>
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LoS outside chamber with piezoelectric short stroke

+magnetic fields reduced, motors in ambient, reduction of cooling hoses, motor cables in vacuum

-position dependent behvaior, only rotary vacuum moton feedthrough

→ ferrofluid seal - uses a magnetic fluid placed around a rotating shaft by a ring of permanent magnets = vacuum (has friction)

<p>+magnetic fields reduced, motors in ambient, reduction of cooling hoses, motor cables in vacuum</p><p>-position dependent behvaior, only rotary vacuum moton feedthrough</p><p></p><p>→ ferrofluid seal - uses a magnetic fluid placed around a rotating shaft by a ring of permanent magnets = vacuum (has friction)</p>
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requirements of the new system

  • reach wafer position

  • accurately position it under SEM

  • fit inside vacuum chamber

  • LoS actuation outside of the chamber

  • high voltage and magnetically compatible materias

  • bigger lifetime and sevice intervals

  • not higher costs

<ul><li><p>reach wafer position</p></li><li><p>accurately position it under SEM</p></li><li><p>fit inside vacuum chamber</p></li><li><p>LoS actuation outside of the chamber</p></li><li><p>high voltage and magnetically compatible materias</p></li><li><p>bigger lifetime and sevice intervals</p></li><li><p>not higher costs</p></li></ul><p></p>
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high-speed dynamically balanced robotic manipulator

  • favorable dynamics due to symmetry

  • only rotational bearings

  • vaccum compatible components

  • dynamic balance using passive counterweights

  • workspace matches purpose

→ dual purpose: actuatos in-plane DoF (x, y, Rz) and constraints out-of-plane DoF (z, Rx, Ry)

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kinematics of the high-speed dynamically balanced robotic manipulator

Uses a Jacobian matrix (position dependent) for actuators:

  • velocity

  • relative changes in position

  • torque (force)

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singularities

In a singularity, Jacobian matrix loses rank

0=singularity

1=equal in all directions

<p>In a singularity, Jacobian matrix loses rank</p><p>0=singularity</p><p>1=equal in all directions</p><p></p>
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three arms vs four arms

  • fourth arms add out-of-plane stiffness, creates symmetry, less out-of-plane rotations

  • eliminates singularities with LoS inside the chamber

  • good dynamics

  • less position dependent (no worst case)

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kinematic design (first order modelling)

what dimensions? where to place motors? can we reach all positions? does it fit inside the chamber?

parameters: vertical displacement due to gravity, torque index, accuracy index, relative angle between arms

  • vary link length and actuator placement

  • high eigenfrequency = good overall results

→ only configurations that fit inside chamber and cover workspace

→ minimal position dependent vertical deflections due to gravity

→ minimal position dependent eigenfrequency

→ minimal position dependent torque

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design considerations in vacuum and SEM environments

  • outgassing

  • virtual leaks

  • chamber deformation

  • ferromagnetic properties

  • bearings design

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carrier-arm connection

  • analogy to giving a hand

  • carrier compliant in torsion

  • mismatch in constraints due to angle between Ry, car and Ry, arm

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linkage 2

  • compliant in torsion to avoid overconstraint

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tolerances

  • on bearing and components lead to Ry rotations, resulting in z

  • sensitivity matrix - to calculate required vertical actuator displacement

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dynamic balancing

  • trade-off torque/mass/size

  • divide mass carrier over 4 arms

  • eigenfrequency decreases due to addition of required balance mass