APS / XOR XAFS beamline evaluation

The APS beamline evaluation was carried out by the Beamline Evaluation Group

BEAMLINE

DATA

LAB BOOK NOTES

RESULTS

PHOTOS

5-BM

5-BM data

5-BM notes

5-BM results

5-BM photos

9-BM

9-BM data

9-BM notes

9-BM results

9-BM photos

12-BM

12-BM data

12-BM notes

12-BM results

12-BM photos

20-BM

20-BM data

20-BM notes

20-BM results

20-BM photos

33-BM

33-BM data

33-BM notes

33-BM results

33-BM photos

Data Collection

Baseline Evaluation of XAFS Bending Magnet Beamlines (2006). All experiments were performed under “standard optimized operating conditions” for each beamline. Details are recorded in the Lab Book Notes.

Beamline Configuration

The following information was collected at each beamline:

Mono Calibration

Method: XANES scans of metal foil reference standards collected over a large energy range without recalibrating the monochromator between foils. (1 sec/point). Edge positions were measured using the first peak in the first derivative of XANES calculated at the beamline and using the BEAMLINE software. Measured energies were compared against nominal values as reported in Rev. Sci. Instrum., 67 (1996) 686.

Energy Resolution

Method: Measure the full width at half maximum of the V_2O_5 pre-edge feature.

Base Noise Levels

Method: record intensity at 10 keV for 3 minutes. Record with beam off for 3 minutes. Record data with knife edge 1/2 way through beam Vertical for 3 minutes. Set delay time to 0 seconds.

Detector Linearity

Method: scan a narrow slit across the beam horizontally to see how uniform the detector is from side to side. N.B., this test could not be performed on all beamlines.

Harmonic Content

Method: Scan the energy around 6.66 keV through a Mo foil to look for emergent Mo XANES from the third harmonic. Scan parameters are the same as for the Vanadate, but with larger steps in the XANES region.

Data Quality

Method: collect transmission EXAFS of solutions with 0.1 edge step in ca. 2 absorption lengths of water. Solutions and transmission cells were prepared by Matt Newville using dilution calculations by Bruce Ravel. Solutions of zinc nitrate and cadmium nitrate were used.

Beamline Operations

Method: collect objective and subjective data on the overall experience from an "outside user" point of view.

Data Processing

Mono Calibration

Summary Plot of Monochromator Calibration experiments attachment:MonoCalibrationSummaryPlot.pdf

Summary Data for Monochromator Calibration experiments attachment:MonoCalibrationSummaryData.txt

Zn Solution (noisy data)

The numerical results are shown below:

Scan

E0

Edge Step

epsilon_k

zn05_01.chi

9665.7189

0.0981006

0.0009736

zn05_02.chi

9665.7189

0.1004050

0.0009180

zn09_01.chi

9671.0000

0.1027941

0.0013858

zn13_01.chi

9668.5040

0.0934614

0.0005705

zn13_02.chi

9668.7460

0.0938051

0.0008412

zn20_01.chi

9666.4488

0.1271893

0.0003987

zn20_02.chi

9666.0854

0.1274453

0.0004710

zn33_01.chi

9668.6290

0.1185146

0.0010271

zn33_02.chi

9668.9400

0.1189671

0.0011380

The values for edge step are given as a guide -- the actual solutions used were from different batches, and so some variation is expected.

The values for "epsilon_k" ($\epsilon_k$) are the automatic estimates from IFEFFIT, and should also be taken with a grain of salt. The plot of $k^2\chi(k)$ below clearly shows the data from 20-BM to be the best, but the data from 5-BM, 13-BM, and 33-BM seem equally noisy to me:

APSXAFS/APS_XOR_Eval/ZnSolutions.png

APSXAFS/APS_XOR_Eval (last edited 2009-10-09 19:50:29 by localhost)