About Us Synchrotron
CESR  |  CHESS  |  ERL  |  G-Line  |  MacCHESS  | 
Home
Facility Description
For Users
Job Openings
Journal Club
Map of Cornell (pdf)
Meetings
News / Research
Operations
Publications
Proposals
Safety
Staff Directory
Synchrotron Sources
Search Site
What is a Light Source?
X-Ray Status
Contact Info
  Shipping & Station Phone Numbers
Experiment Designing
  X-ray Sources
X-ray Optics
Character of Elements
Facility
 

CHESS East
D1
E-line
F1
F2
F3
F-Cave

CHESS West
A1
A2
A3
B1
B2
C1
G-line

Diffractometer
Station Equipment
Support Rooms

Hotels & Inns
Local Sites and Places
Maps & Directions
Staff Directory

CHESS West Map

Click on the station names for more information

A-line was again rebuilt in 2001, both on the accelerator side of the shielding wall and in the experimental hall. The A1 station receives half of the radiation from a 49 pole 0.8 T wiggler and is fixed in energy at ~13.1 keV with both vertical and horizontal focusing. A2 receives the other half of the wiggler beam via A3 which operates primarily as the optics room for A2. In certain instances A3 may be used as an end station for an undulator run and will also (at the expense of A2 operation) allow direct access to the 20 kW white beam (at 500 mA operation) 28 meters from the wiggler source.

B and C lines use radiation from the CESR high-field dipole bend magnets. B1 is dedicated to diamond anvil-cell high pressure experiments using the National High Pressure Facility.  The B1 hutch was expanded in 1995 and in the past year the optics have been modified to provide better access and safety control of the high power lasers in use at the station. 

B2 can deliver either white beam or monochromatic bend magnet radiation.  The peak spectral intensity occurs at about 11 KeV, and monochromatic beam has been used up to 35 KeV.  Over the last few years, B2 has been used for: angle-dispersive high pressure powder diffraction (ADXD), EXAFS, fluorescence spectroscopy (including micro-science utilizing focusing capillary optics), single crystal diffraction, and instrumentation development.  The monochromator has a simple, versatile design that permits relatively quick change between white beam and several choices of silicon and germanium crystals.  For ADXD most users prefer germanium (111) because it delivers the most flux at the standard energy, 25 KeV.  Over the last year (2004) ADXD experiments have gained in efficiency because of the MAR 345 detector.

The old C1 and C2 stations were replaced by a new single larger C1 x-ray hutch with a choice of x-ray optics.   One configuration is a side bounce monochromator to focus a wide energy range x-ray beam onto a small spot.  Alternately a double crystal monochromator feeds a 6-circle diffractometer for precise scattering studies.

 

Last Update: 2006-09-21

Cornell High Energy Synchrotron Source
200L Wilson Lab
Rt. 366 & Pine Tree Road
Ithaca, NY  14853

Direct questions, suggestions or problems to webmaster.
Copyright © 1998-2004  Cornell High Energy Synchrotron Source. All rights reserved.


NCRR

NCRR


NSF
NSF


NIGMS
NIGMS

Cornell University