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STATUS OF OTR IMAGER FOR THE LCLS UNDULATOR. Bingxin Yang, Jim Bailey, and Dean Walters Advanced Photon Source. OTR Imager Status. Specifications and designs LCLS PSD 1.4–004 (cancelled) LCLS ESD 1.4–109 LCLS Tech Note LCLS-TN-05-21 (most complete) - PowerPoint PPT Presentation
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A U.S. Department of EnergyOffice of Science LaboratoryOperated by The University of Chicago
Argonne National Laboratory
Office of ScienceU.S. Department of Energy
STATUS OF OTR IMAGER FOR THE LCLS UNDULATOR
Bingxin Yang, Jim Bailey, and Dean Walters
Advanced Photon Source
2
Pioneering Science andTechnology
Office of Science U.S. Department
of Energy
OTR Imager Status
Specifications and designs• LCLS PSD 1.4–004 (cancelled)
• LCLS ESD 1.4–109
• LCLS Tech Note LCLS-TN-05-21 (most complete)
• PAC 05, “Design of a high-resolution optical transition radiation imager for the linac coherent light source undulator,” by B.X. Yang, J. L. Bailey, D. R. Walters, and S. J. Stein.
Outline• Basic design features of the OTR imager
• Current status
• Future?
3
Pioneering Science andTechnology
Office of Science U.S. Department
of Energy
OTR imager specification
Basic requirements:• RMS resolution: 12 m
• Total field of view: 10 mm (H) 5 mm (V)
• Single shot imaging (1 nC @ 13.64 GeV) desirable
2D Graph 1
X (m)
-150 -100 -50 0 50 100 150
INT
EN
SIT
Y (
AR
B. U
NIT
S)
0.0
0.2
0.4
0.6
0.8
1.0
1.2
4
Pioneering Science andTechnology
Office of Science U.S. Department
of Energy
OTR imager optics geometry
Design features to obtain good resolution and large field of view simultaneously :(1) Use near normal incidence angle
(2) Tilt CCD camera* to coincide with the tilted image plane.
* CCD camera manufacturer specifies maximum tilt angle allowed.
5
Pioneering Science andTechnology
Office of Science U.S. Department
of Energy
OTR imager optics calculation: perfect optics
Specifications without aberrations:• Collection cone angle radius: 0.075 radian
• Diffraction contribution to resolution: 3.2 – 5.6 m (400 – 700 nm)
EFFICIENCY OF LIGHT COLLECTION
RADIUS OF COLLECTION CONE (RADIAN)
0.0 0.1 0.2 0.3 0.4 0.5 0.6
OP
TIC
AL
EF
FIC
IEN
CY
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
= 10
100
103
104
105
ISOTROPICLIGHT
LIGHT INTENSITY PROFILE NEAR FOCUS
x/0
-20 -15 -10 -5 0 5 10 15 20
INT
EN
SIT
Y P
RO
FIL
E (
AR
B U
NIT
S)
0.0
0.5
1.0
1.5
2.0
OTR LIGHT
ISOTROPIC
0=1000
Collection efficiency Radial distribution Integrated profile
LIGHT INTENSITY NEAR FOCUS
r/0
0 5 10
INT
EN
SIT
Y (
AR
B U
NIT
S)
0.0
0.5
1.0
7 2
01
3 10 ln lncollectedN photons Q nC
1/ 2
4.2res
6
Pioneering Science andTechnology
Office of Science U.S. Department
of Energy
OTR imager optics calculation: aberrations
Ray tracing studies for aberrations:• Commercial achromat lenses (M = 1)
• Spherical aberrations unimportant
• Chromatic aberrations dominant contribution
• Use laser mirrors as bandpass filters to improve efficiency
Table 3.12: RMS Size of the PSF from Geometrical Aberration at the Image (2 PAC089) RMS spot size (m) Aperture
size (mm) 550 nm 490–565 nm 515–585 nm 475–645 nm 500–700 nm 400–700 nm 10 0.05 0.8 1.7 1.7 2.9 3.8 15 0.17 1.6 2.5 2.3 4.4 5.8 20 0.36 2.0 3.3 3.2 5.7 7.8 25 0.64 2.9 3.9 3.9 7.0 9.8 30 1.00 4.4 4.4 4.9 8.3 12.0 35 1.37 3.6 5.0 6.0 9.4 14.4 40 1.66 4.5 5.4 7.2 10.5 17.0 45 1.78 5.6 5.8 8.6 11.4 20.0 48 1.71 6.3 6.0 9.5 11.9 22.0 50 1.62 6.9 6.4 10.2 12.2 23.4
7
Pioneering Science andTechnology
Office of Science U.S. Department
of Energy
OTR imager mechanical design: partially assembled
Design Parts
8
Pioneering Science andTechnology
Office of Science U.S. Department
of Energy
OTR imager intended location: long break sections
9
Pioneering Science andTechnology
Office of Science U.S. Department
of Energy
Summary and future
Summary• Parts are received and partially assembled
• To be tested- Verify resolution- Check resolution over the entire FOV
• Use this package at a different location in LCLS linac? to be studied…- Biggest issue: camera and controls