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Inhouse Development of a vacuum goniometer with a sub-microradian resolution MEDSI 2018 PARIS, 25 th -29 th of June 2018, Frank-Uwe Dill, Petra III Beamline P01

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Page 1: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

Inhouse Development of a vacuum goniometer with a sub-microradian resolution

MEDSI 2018 PARIS, 25th-29th of June 2018, Frank-Uwe Dill, Petra III Beamline P01

Page 2: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 2

Motivation

Partnership with Max Planck Institute Stuttgart since 2015

Ruthenates will be potentially used for storage of information (quantum computing) and for superconductivity

Graphs by Hlynur Gretarsson

Physical phenomenas that are not understood.To support theoretical models, as many different variables

as possible should be determined by the experiments

-> high energy resolution at 2.84 keV is needed->everything has to be put in high vacuum (10-7mbar)

Page 3: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 3

New arrangement of beamline components

OH1 OH 1

EH 1 OH 2EH 2

Two new5m

undulators

DifferentialPumpingStation

Old positionin air RIXS

In vacuumRIXS

In vacuumIXS HRM

New positionin air IXS andNRS HRMs

Valveswith

diamondwindows

Beamline P01 for Inelastic X-Ray Scattering (IXS) and Nuclear Resonant Scattering (NRS) Experiments

Sample chamber and High Resolution Monochromator have to be put in High VacuumOptional no window towards the ring

KB DCM

Page 4: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 4

Previous high resolution monochromator (in air)

• Modifying of existing Kohzu KTG-15MA possible, but only for to 10-4mbar (≠ 10-7mbar). Same for new KTGs

Costs: modifying 4.300€brandnew 30.000€

• Some values of existing Kohzus:

- wobble 1 arcsec- resolution 120nrad (full step of stepper motor)- ±2° range fine- 360° with clutch and coarse motor

3 single setups (top view)

HRM_1HRM_3

HRM_2

beam

beam

Page 5: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 5

Requirements for the new goniometers

• wobble 1 arcsec (4,8µrad) within +-5° rotation

• Possible load of 6kg (for bigger crystal setups)

• Motorized Range of +-20°, manually +-90°

• Angular resolution of 0,5 microrad

• Vacuum compatible to 5x10-7mbar

Precise androbust bearing

Preciseactuatorwith long

travelrange

Page 6: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 6

High precicion bearing for 10-7mbar from Mahr

Shaftstainless steel, Ø16mm

Ball Cage, bronze

Housingstainless steel

Ø38mmLength 120mm

Balls stainless steel, Ø3mm

Axial Bearing, bronze

Original design byHans-Bernhard Peters

from ZM1-DESY

Page 7: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 7

High Precision Mahr Bearing, Measurement Record

Page 8: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 8

PiezoLEG and NANOS piezo driver and interpolation card

NANOS interpolation and driver card for 2 channelsInterpolation of 1VSS up to 100.000

-> 0,2nm with a 20µm scale(~1800€)

Page 9: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 9

Piezo driven goniometer

Spring

Encoder wheelØ 200mm

20µm scale(700€)

Kohzu tilt stage(5000€)

Piezo LEGS with rod

110mm length(1600€)

Encoder(700€)

Manual brake(for service)

WireØ 0,3mm

LimitSwitches

Inhouse Design S. Mayer

Crystal holderfor 2 channel cuts

Page 10: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 10

Complete IXS HRM

Tank 1,4m x 1,3m x 0,8m = 1,45m3

Body stainless steelTop / Bottom Aluminum

Vacuum3,6 x 10-7mbar with two 300l Getterpumps1,5 x 10-6mbar with one 300l Turbopump

turbopump

3 hrm units 2 pin diodeunits

Page 11: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 11

Complete IXS HRM

OH2OH1

Energy resolution150meV at 2.8keV

Page 12: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 12

New setup, 2 sets, each with 4 crystals

2 PIN diodes for diagnostics (2nd one at bottom side)

Hrm_1

Hrm_3

Hrm_2

beam

2 different crystalsetups can be moved

in and out

Double-tiltstages (piezos)

Page 13: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 13

New setup, 2 sets, each with 4 crystals

Energyresolution100meV at 2.8keV

Page 14: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14

Reproducibility and Jitter

0 nrad

20 nrad

10 nrad

Hrm_1, 28.02.2018

0 nrad

200 nrad

100 nrad

10 nrad

Hrm_1, 04.11.2017

-100 nrad±50nanorad

±10nanorad

Reproducible steps much better than 500nrad (required) but Jitter and resolution of goniometers changed

Hrm1 & 3 Jitter got worse after 4 months

Encoder values

Encoder values

Page 15: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 15

Reproducibility and Jitter

0 nrad

-50 nrad

50 nrad

0 nrad

200 nrad

100 nrad

50 nrad

150 nrad

Reproducible steps much better than 500nrad (required) but Jitter and resolution of goniometers changed

Hrm_2 Jitter got better after 4 months

±60nanorad±25nanorad

Hrm_2, 04.11.2017Hrm_2, 28.02.2018

Page 16: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 16

Possible reason for change of resolution and Jitter

The PiezoLEG does not likeany forces perpendicular to

the moving direction

-> add a linear guidance forthe wire

Page 17: Inhouse Development of a vacuum goniometer with …...MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 14 Reproducibility and Jitter 0 nrad 20 nrad 10

MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 17

Conclusion and Outlook

Very simple concept shows very good results over the last 12 months(installation and first use in June 2017)

-> scientists are happy

The goniometer is a cost-saving in house solution, ~ 8.000-10.000€ compaired to 30.000€ (my work not considered)

The three different setups do have different Jitters / resolutionsand both changes over time

– > PiezoLEG must be decoupled from the wire (urgent)

– > I should have built a fourth setup to do tests in general

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MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 18

Acknoledgements

Max Planck Institute Stuttgart Director Prof. B. Keimer, H. GretarssonB. Bruha

Desy P01 IXS groupH. Yavas (since Feb. 2018 LCLS Stanford)

S. Mayer

Desy Engineering DepartmentM. Lemke, S. Adler, C. Martens

Desy Workshop and work planning Dep.C. Conrad, B. Hager

Desy Electronic DepartmentD. Lotter, M. Paesler,F. Reedwisch, J. Voigt

- Initiator and partner of the project- Fabricating of almost all Aluminum parts

for the goniometers and stages

- Scientist - „Co-Engineer“

- Design/Simulation of the Tank (1,5m3)

- Fabrication of the Tank and big Aluminumparts

- Support for Cabling

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MEDSI 2018 PARIS | 25th-29th of June | Frank-Uwe Dill | Petra III Beamline P01 19

In Vacuum Goniometer

Thank you for your Attention