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Detector Technology, Tips, Tricks Innovation with Integrity

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  • Detector Technology, Tips, Tricks

    Innovation with Integrity

  • X-Ray Powder Diffraction (XRPD) Bragg-Brentano Geometry

    14-15/12/2011 Advanced XRD Workshop 2

  • X-ray Detector From X-Ray Photon Energy h to CPS

    Sen

    sor

    Pre

    -am

    plif

    icat

    ion Photons

    h

    Am

    plif

    icat

    ion

    Sig

    nal

    pro

    cess

    ing

    Co

    un

    tin

    g

    14-15/12/2011 Advanced XRD Workshop 3

  • Point detectors (0-D)

    Scintillation counter

    Proportional counter

    Si(Li) solid state detector

    Ge solid state detectors

    Silicon pin diodes

    Silicon drift detectors

    Ionization chambers

    Commonly Used X-Ray Detectors

    Linear detectors (1-D)

    MikroGap detector

    Compound silicon strip

    detector

    Single wire

    proportional counter

    Image plate detector

    (IP)*

    Linear CCD*

    Photographic film*

    Area detectors (2-D)

    CCD camera*

    Multi wire

    proportional counter

    (MWPC)

    MikroGap detector

    Image plate detector

    (IP)*

    Photographic film*

    Pixel detectors

    CMOS detectors* Integrating (analog) detectors, of little use for XRD

    14-15/12/2011 Advanced XRD Workshop 4

  • Point detectors (0-D)

    Scintillation counter

    Proportional counter

    Si(Li) solid state detector

    Ge solid state detectors

    Silicon pin diodes

    Silicon drift detectors

    Ionization chambers

    Point Detectors

    Linear detectors (1-D)

    MikroGap detector

    Compound silicon strip

    detector

    Single wire

    proportional counter

    Image plate detector

    (IP)

    Linear CCD

    Photographic film

    Area detectors (2-D)

    CCD camera

    Multi wire

    proportional counter

    (MWPC)

    MikroGap detector

    Image plate detector

    (IP)

    Photographic film

    Pixel detectors

    CMOS detectors

    14-15/12/2011 Advanced XRD Workshop 5

  • Scintillation Counter

    Sodium-IodideCrystal

    Photocathode

    Optical Window

    -Pulse

    MeasuringDevice

    Light Photon Photomultiplier Tube

    Dynode Anode

    X-Rays

    14-15/12/2011 Advanced XRD Workshop 6

  • Scintillation Counter

    Active Area: 30 mm Sensitivity: from Cr- to Mo-radiation Energy resolution: 30% - 45% (2.5 keV at 8 keV e.g.)

    NaI(Tl) scintillation: Maximum count rate >2x106 cps Noise: < 0.3 cps

    Infinite life time Maintenance free Routine detector for all applications Potential angular resolution: no limit! (typical 0.037 for Bragg-Brentano geometry)

    14-15/12/2011 Advanced XRD Workshop 7

  • X-Ray Powder Diffraction with Scintillation Counter

    D8 ADVANCE diffractometer

    Cu-radiation 40 kV, 50 mA 0.3 divergence and anti-scatter slit

    2.5axial Soller slits 20m Ni Cu-K filter 0.05mm receiving slit Scintillation counter 0.006step size 10 seconds per step NIST 1976 Corundum sample

    FWHM at 100% reflection 0.04

    Angular position accuracy certified 0.01

    14-15/12/2011 Advanced XRD Workshop 8

  • Solid State DetectorSOL-XE Detector

    Active area: 4 x 15 mm2

    Si(Li) solid state energy dispersive detector Energy resolution < 350 eV(4.5%) at 50.000 cps

    Suppression of e.g. Fe-fluorescence and Cu-K radiation

    Linearity up to 75.000 cps integral events

    Wavelength range: 2 keV up to 30 keV (Cr-Mo-radiation)

    14-15/12/2011 Advanced XRD Workshop 9

  • Solid State DetectorFunctional Principle

    Lithium drifteddepletion region~ 0.5 3 mm

    AmplifierSignal processing

    counting

    Au Cathode~ - 500 V~ 200 nm

    Pre amplifierAu contact~ 20 nm

    X-Rays

    Be window

    P-typeRegion~ 0.1m

    n-typeRegion~ 0.1m

    Bias voltage

    h

    e-

    14-15/12/2011 Advanced XRD Workshop 10

  • X-Ray Powder Diffraction with Energy Dispersive SOL-XE

    D8 ADVANCE diffractometer

    Cu-radiation 40 kV, 50 mA 0.3 divergence and anti-scatter slit

    2.5axial Sollerslits

    No Ni Cu-K filter 0.05 receiving slit Sol-XE detector 0.006step size 2.8 seconds per step

    NIST 1976 Corundum sample

    FWHM at 100% reflection 0.04

    SOL-XE: No Nickel filter, more than 2 times

    more intensity

    14-15/12/2011 Advanced XRD Workshop 11

  • MuscoviteHematiteHematite/Muscovite, 2 Soller, 0,5 slits, 0,2 mm DS, Ni-Filter - Step: 0.020 - Step time: 1. s

    Lin

    (Cou

    nts)

    0

    100

    200

    300

    400

    500

    600

    700

    800

    900

    1000

    1100

    1200

    1300

    1400

    1500

    2-Theta - Scale

    7 10 20 30 40 50

    Ni-Filter

    Measurement on Hematite/Muscovite composite with Cu-Radiation and scintillation counter

    Suppression of Fe-fluorescence

    14-15/12/2011 Advanced XRD Workshop 12

  • MuscoviteHematiteHematite/Muscovite, 2 Soller, 0,5 slits, 0,2 mm DS, Solid state Detektor - Step: 0.020 - Step time: 1. s

    Lin

    (Cou

    nts)

    0

    100

    200

    300

    400

    500

    600

    700

    800

    900

    1000

    2-Theta - Scale

    7 10 20 30 40 50

    Sol-X Detector

    Measurement on Hematite/Muscovite composite with Cu-Radiation, SOL-XE detector

    Suppression of Fe-fluorescence

    14-15/12/2011 Advanced XRD Workshop 13

  • X-Ray Powder Diffraction with SOL-XEMonochromatic K-radiation

    Energy dispersive SOL-XE detector can be used with any radiation source, not only Cu.

    Park the detector on K line of corundum, collect a peak and calibrate with 8.9 KeVfor K

    Very easy and fast way to switch between Kand K radiation or between different radiation sources

    Energy calibration window of SOL-XE detector

    14-15/12/2011 Advanced XRD Workshop 14

  • X-Ray Powder Diffraction with SOL-XEMonochromatic K-radiation

    NIST1976 corundum plate

    Bragg-Brentano geometry 0.5divergence 0.1 mm receiving slit

    Sol-XE detector

    K peaks of corundum

    K peaks of corundum

    00-046-1212 (*) - Corundum, syn - Al2O3 - WL: 1.3922200-046-1212 (*) - Corundum, syn - Al2O3 - WL: 1.5406File: NIST 1976_1sec kbeta.raw - Step: 0.010 - Step time: 1. s

    Lin

    (Cps

    )

    0

    100

    200

    300

    400

    500

    600

    700

    2-Theta - Scale

    46 50 60

    14-15/12/2011 Advanced XRD Workshop 15

  • Point detectors (0-D)

    Scintillation counter

    Proportional counter

    Si(Li) solid state detector

    Ge solid state detectors

    Silicon pin diodes

    Silicon drift detectors

    Ionization chambers

    Commonly Used X-Ray Detectors

    Linear detectors (1-D)

    MikroGap detector

    Compound silicon strip

    detector

    Single wire

    proportional counter

    Image plate detector

    (IP)

    Linear CCD

    Photographic film

    Area detectors (2-D)

    CCD camera

    Multi wire

    proportional counter

    (MWPC)

    MikroGap detector

    Image plate detector

    (IP)

    Photographic film

    Pixel detectors

    CMOS detectors

    14-15/12/2011 Advanced XRD Workshop 16

  • Compound Si Strip DetectorLYNXEYE Detector

    Active Area: 14.4 x 16 mm Capture angle 3.72theta for D8 ADVANCE

    Compound silicon strip detector technology Maximum global count rate: >100,000,000 cps

    Maximum local count rate: 700,000 cps

    Dynamic range >7x106

    Energy resolution: 25% (2 keV) Wavelength range: from Cr- to Cu-radiation

    Maintenance free

    14-15/12/2011 Advanced XRD Workshop 17

  • Compound Si Strip DetectorHow Does it Work

    h+

    e-

    Sketch taken from: from Kemmer et al., Phys. Bl., vol. 41, p117 (1985)

    LYNXEYE: Compound Silicon Strip Detector

    14-15/12/2011 Advanced XRD Workshop 18

  • High Resolution XRPD in NIST 1976, LYNXEYE vs. Scintillation Counter

    D8 ADVANCE 35 kV, 50 mA 0.3divergence 2.5Soller 0.3anti-scatter 2.5Soller 0.5% Ni-filter 0.1 mm receiving slit 3opening 0.006step size 1 sec/step

    ~ 150,000 counts

    14-15/12/2011 Advanced XRD Workshop 19

  • High Resolution XRPD in NIST 1976, LYNXEYE vs. Scintillation Counter

    Inte

    nsity

    [cou

    nts

    ]

    0

    10000

    20000

    30000

    40000

    50000

    60000

    70000

    80000

    90000

    100000

    110000

    120000

    130000

    140000

    150000

    2-Theta [deg]

    25 30 40 50 60 70

    Inte

    nsity

    [co

    unts

    ]

    0

    10000

    20000

    30000

    40000

    50000

    60000

    70000

    80000

    90000

    100000

    110000

    120000

    130000

    140000

    150000

    2-Theta [deg]

    34.71 34.8 34.9 35.0 35.1 35.2 35.3 35.4 35.5 35.6 35.7

    Scinti:1100 counts

    LYNXEYE:138,000 counts

    14-15/12/2011 Advanced XRD Workshop 20

  • High Resolution XRPD in NIST 1976, LYNXEYE vs. Scintillation Counter

    SRM 660a

    115.50 116.00 116.50 117.00 117.50

    2 deg

    0.00

    20.00

    40.00

    60.00

    80.00

    100.00

    Irel

    ScintiLynxEye

    Normalised Intensity!

    14-15/12/2011 Advanced XRD Workshop 21

  • High-Resolution XRPD on NIST 660aResolution

    SRM 660a

    29.90 30.10 30.30 30.50 30.70 30.90

    2 deg

    0

    20000

    40000

    60000

    80000

    100000

    Counts

    LynxEye

    FWHM = 0.0365 2

    With standard slit settings,Using small slits and sollersresolution can be even improved!

    14-15/12/2011 Advanced XRD Workshop 22

  • High-Resolution XRPD on NIST 660a: LYNXEYE vs. Scintillation Counter

    SRM 660a

    0.00 40.00 80.00 120.00 160.00

    2 deg

    0.00

    0.02

    0.04

    0.06

    0.08

    0.10

    0.12

    0.14

    FWHM

    ScintiLynxEye

    14-15/12/2011 Advanced XRD Workshop 23

  • XRPD on NIST 660aResolution

    SRM 660a

    20.90 21.10 21.30 21.50 21.70 21.90

    2 deg

    0

    20

    40

    60

    80

    100

    Irel

    ScintiLynxEye

    14-15/12/2011 Advanced XRD Workshop 24

  • Bragg-Brentano Geometrie Flat Detector Error

    the 1-D Detector is tangential to goniometer circle, which causes shiftsand asymmetries of the reflections

    A narrower detector capture angle reduces the drawbacks for the price of smaller intensities

    14-15/12/2011 Advanced XRD Workshop 25

  • XRPD at Low Angles with LYNXEYEAg-Behenate

    D8 ADVANCE 35 kV, 50 mA 500 mm 0.1 divergence slit 2.5Soller slits Anti-scatter screen Ni 0.5 % filter 30 rpm LYNXEYE 1opening Step size: 0.006 Step time: 0.1 sec/step

    2Theta: 0.5

    14-15/12/2011 Advanced XRD Workshop 26

  • Compound Si Strip DetectorOptimized for Cu Radiation

    Sketch taken from: from Kemmer et al., Phys. Bl., vol. 41, p117 (1985)

    LYNXEYE: Compound Silicon Strip Detector

    14-15/12/2011 Advanced XRD Workshop 27

  • Compound Si Strip DetectorOptimized for Cu Radiation

    14-15/12/2011 28Advanced XRD Workshop

    Wavelength

    Linear absorptioncoefficient for Si

    (cm-1)

    Efficiency (300m sensor)

    Cr 439.3 > 99%

    Co 216.4 > 99%

    Cu 139.4 > 98%

    Mo 14.25 ~ 35%

  • Compound Si Strip DetectorFor Hard X-rays

    Sketch taken from: from Kemmer et al., Phys. Bl., vol. 41, p117 (1985)

    LYNXEYE: Compound Silicon Strip Detector

    14-15/12/2011 Advanced XRD Workshop 29

    500

    m

  • Compound Si Strip DetectorFor Hard X-rays

    14-15/12/2011 30Advanced XRD Workshop

    Wavelength

    Linear absorptioncoefficient for Si

    (cm-1)

    Efficiency (500m sensor)

    Cr 439.3 > 99%

    Co 216.4 > 99%

    Cu 139.4 > 99%

    Mo 14.25 ~ 50%

    Ag 7.09 ~ 30%

  • 14-15/12/2011 31Advanced XRD Workshop

    Optimized discriminator settings Improve peak-to-background ratio

    Compound Si Strip DetectorFluorescence DiscriminationN

    orm

    aliz

    edto

    max

    .Inte

    nsi

    ty

  • Functional Principle of Conventional Gas Filled Proportional Detector

    Pros High sensitivity, low noise due to high intrinsic amplification caused by avalanche multiplication of charges (1 to 2 orders higher than solid state detector)

    Big active area for affordable costs possible

    Cons Limited maximum count rate due to long ion drift times (6 sec) l (typically

  • Functional Principle of Conventional Gas Filled Proportional Detector

    Detection Gas

    ElectricalCurrent

    Measuring Device

    X-Rays

    Cathode -

    Anode +

    + -Voltage Source

    +

    -

    + + +

    - - -

    14-15/12/2011 Advanced XRD Workshop 33

  • MicroGap Detector Technology VNTEC-1TM Detector

    Large active area of 50x16 mm Capture angle >122 D8 ADVANCE

    100 msec Snapshots Super speed continuous scan mode

    MikroGap technology Global count rate >106 cps Detector background

  • MikroGapTM technology with resistive anode: shortens drift time of ions fast electrons induce charge on readout strips

    Adjusted surface resistance (105 - 107 / area): high enough to limit discharges

    low enough to support high count rates

    MicroGap Detector TechnologyHow Does it Work

    US Patent US 6,340,819 B1

    14-15/12/2011 Advanced XRD Workshop 35

  • VNTEC-1 Scanning DiffractionMeasurements

    Conventional proportional counter

    Angular resolution 0.05 -0.12

    Strong function of count rate

    MikroGapTM, VNTEC-1

    Angular resolution

  • VNTEC-1 in SNAPSHOT ModeKinetic Studies of Phase Transition

    D8 ADVANCE with Bragg-Brentano geometry

    Power: 40kV, 50 mA

    Optics: 0.5divergence slit

    4Soller slit Ni Cu-K-filter

    Step size: 0.023 Time per Snapshot: 1 sec

    High temperature chamber, permanent heating

    Phase Transition of NH4NO3, T = 3 K, 58 Snapshots

    Phase IV (orthorhombic)

    Phase II (tetragonal)

    Phase I (cubic)

    melted

    14-15/12/2011 Advanced XRD Workshop 37

  • VNTEC-1 in Scanning ModeHot Humidity Investigations by XRD

    Parallel beamGbel Mirror

    Line focusX-ray tube

    Hot HumiditySample chamber

    VNTEC-1detector

    Radial Sollerslit

    Heated supplyhose

    14-15/12/2011 Advanced XRD Workshop 38

  • VNTEC-1 in Scanning Mode Humidification Investigations on Creatine by Fast Continuous Scans

    00-029-1650 (D) - Creatine hydrate - C4H9N3O2H2O

    00-029-1649 (Q) - Creatine - C4H9N3O2

    Type: 2Th/Th locked - Start: 5.000 - End: 40.005 - Step: 0.007 - Step time: 0. s - Anode: Cu

    Lin

    (Cou

    nts)

    0

    500

    1000

    1500

    2000

    2500

    2Theta [deg]

    5 10 20 30 40

    Scan speed 30/minute 0.01 sec/step 0.0065 /step

    50 C

    0.5 % relative humidity

    14-15/12/2011 Advanced XRD Workshop 39

  • VNTEC-1 in Scanning Mode Humidification Investigations on Creatine by Fast Continuous Scans

    inte

    nsity

    [cps

    ]

    0

    10

    20

    30

    40

    50

    60

    70

    80

    90

    100

    110

    2-Theta [deg]

    5 10 20 30 40

    Measurement conditions: 5 402theta Step size 0.007

    Scan speed 30/min

    71 seconds/scan

    Creatine

    Creatinehydrate

    50 C

    80 % relative humidity

    14-15/12/2011 Advanced XRD Workshop 40

  • BAXS Detectors for XPRDD

    imen

    sio

    n

    Capabilities

    Gain factor 3

    GF >150 GF >500

    14-15/12/2011 Advanced XRD Workshop 41

  • Innovation with Integrity

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